IREF= 1 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 93-93 A-Range= 237-237 E-Range= 0- 30 MeV
Author(s)= P.G.Young and E.D.Arthur
Reference= Proc.Int.Conf.Nucl.Data Sci.and Tech.,Julich (1992) p894
Summary= modification of potential by Haouat,Lachkar,Lagrange et al, NSE 81,
(1982), especially for higher energy
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2 Neutron incident, CC vibrational model
Potential is non-relativistic and non-dispersive
Z-Range= 82-82 A-Range= 208-208 E-Range= 0-200 MeV
Author(s)= H.Vonach,A.Pavlik,M.B.Chadwick,R.C.Haight,R.O.Nelson,S.A.Wender,P.G.
Young
Reference= Phys. Rev. C 50, 1952 (1994)
Summary= Based on detailed fits to neutron data 8.5-10 MeV,simply
extrapolated to lower energies and extended to higher energies.
Reaction cross section deficient above 100 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 3 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 92-92 A-Range= 235-235 E-Range= 0- 30 MeV
Author(s)= P.G.Young and E.D.Arthur
Reference= Proc.Int.Conf.Nucl.Data Sci.and Tech.,Julich (1992) p894
Summary= modification of potential by Haouat,Lachkar,Lagrange et al, NSE 81,
(1982), especially for higher energy
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 92-92 A-Range= 237-237 E-Range= 0- 30 MeV
Author(s)= P.G.Young and E.D.Arthur
Reference= LANL Report LA-UR-91-1424,894(1992)
Summary= potential was inferred from the u-238 potential that covers the
same energy range
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 92-92 A-Range= 238-238 E-Range= 0- 30 MeV
Author(s)= P.G.Young and E.D.Arthur
Reference= LANL Report LA-UR-91-1424,894(1992)
Summary= modification of potential , NSE 81,49 (1982) , especially at higher
energies
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 6 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 94-94 A-Range= 242-242 E-Range= 0- 20 MeV
Author(s)= D.G.Madland and P.G.Young
Reference= Report LA-7533-MS (1978)
Summary= parameters were developed to provide Pu-242 total,elastic and
inelastic neutron data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 7 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 94-94 A-Range= 239-239 E-Range= 0- 30 MeV
Author(s)= P.G.Young and E.D.Arthur
Reference= LANL Report LA-UR-91-1424,894(1992)
Summary= Modification of potential by Haouat, Lachkar, Lagrange, et al., NSE
81 (1982) 49, especially above 20 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 8 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 95-95 A-Range= 241-243 E-Range= 0- 30 MeV
Author(s)= P.G.Young and E.D.Arthur
Reference= LANL Report LA-UR-95-3654, paper at RIPL CRP Mtg., Vienna, Oct.30-N
ov.3,1995.
Summary= based on pu-239 potential used for endf/b-vi with isospin
corrections and some adjustments to better match tot-xs
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 90-95 A-Range= 230-250 E-Range= 0- 10 MeV
Author(s)= D.G.Madland and P.G.Young
Reference= Int.Conf.,Harwell UK,Sept. 25-29,1978
Summary= derived by fitting inelastic, elastic and total cross sections of
several nuclides
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 10 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-26 A-Range= 54- 56 E-Range= 0- 52 MeV
Author(s)= E.D.Arthur and P.G.Young
Reference= LA-UR-95-3654 (1995),BNL-NCS-51245 (1980) p.731, LA-8626-MS (1980)
Summary= Potential for neutron reactions on Fe-54 and Fe-56 nuclides
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 11 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 27-27 A-Range= 59- 59 E-Range= 0- 27 MeV
Author(s)= E.D.Arthur, P.G.Young, and W.Matthes
Reference= BNL-51245,p.751 (1980); Nucl.Sci.Eng.124,271(1996)
Summary= potential developed for co-59 nuclide to analyze neutron reaction
data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 12 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 30-30 A-Range= 57- 81 E-Range= 0- 20 MeV
Author(s)= P.G.Young and D.Rutherford
Reference= Report IAEA-TECDOC-483,167 (1988)
Summary= potential developed for neutron interaction with zinc isotopes
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 13 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 39-39 A-Range= 89- 89 E-Range= 0- 21 MeV
Author(s)= E.D.Arthur
Reference= Nucl.Sci.Eng. 76,137 1980)
Summary= potential developed for neutron interaction with y-89 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 14 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 40-40 A-Range= 90- 90 E-Range= 0- 20 MeV
Author(s)= E.D.Arthur
Reference= Nucl.Sci.Eng. 76,137 (1980); LA-UR-94-3104 (1994)
Summary= potential developed for neutron interaction with zr-90 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 15 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 6- 6 A-Range= 12- 12 E-Range= 0- 65 MeV
Author(s)= M.B.Chadwick and P.G.Young
Reference= Nucl.Sci.Eng. 123, 17 (1996)
Summary= Calculation and evaluation of cross sections and kerma factors for
neutrons up to 100 MeV on carbon. Potential based on experimental
data and previous optical model analyses, especially Arthur and
Dimbylow. See LA-UR-95-3654.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 16 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 7- 7 A-Range= 14- 14 E-Range= 0- 60 MeV
Author(s)= M.B.Chadwick and P.G.Young
Reference= Nucl.Sci.Eng. 123, 17 (1996)
Summary= Calculation and evaluation of cross sections and kerma factors for
neutrons up to 100 MeV on carbon. Potential based on experimental
data and previous optical model analyses, especially Arthur and
Islam. See LA-UR-95-3654.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 17 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 8- 8 A-Range= 16- 16 E-Range= 0- 50 MeV
Author(s)= M.B.Chadwick and P.G.Young
Reference= Nucl.Sci.Eng. 123, 17 (1996)
Summary= Calculation and evaluation of cross sections and kerma factors for
neutrons up to 100 MeV on carbon. Potential based on experimental
data and previous optical model analyses, especially Arthur and
Islam. See LA-UR-95-3654.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 18 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 13-13 A-Range= 27- 27 E-Range= 0- 20 MeV
Author(s)= R.C.Harper and W.L.Alford
Reference= J.Phys.G:Nucl.Phys. 8, 153(1982)
Summary= Experimental and theoretical neutron cross sections at 14 MeV.
Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for
incident neutrons, protons, and alphas.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 19 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 58- 58 E-Range= 0- 20 MeV
Author(s)= R.C.Harper and W.L.Alford
Reference= J.Phys.G:Nucl.Phys. 8, 153(1982)
Summary= Experimental and theoretical neutron cross sections at 14 MeV.
Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for
incident neutrons, protons, and alphas.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 20 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 41-41 A-Range= 93- 93 E-Range= 0- 20 MeV
Author(s)= R.C.Harper and W.L.Alford
Reference= J.Phys.G:Nucl.Phys. 8, 153(1982)
Summary= Experimental and theoretical neutron cross sections at 14 MeV.
Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for
incident neutrons, protons, and alphas.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 21 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 79-79 A-Range= 197-197 E-Range= 0- 20 MeV
Author(s)= R.C.Harper and W.L.Alford
Reference= J.Phys.G:Nucl.Phys. 8, 153(1982)
Summary= Experimental and theoretical neutron cross sections at 14 MeV.
Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for
incident neutrons, protons, and alphas.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 100 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-92 A-Range= 40-238 E-Range= 10- 50 MeV
Author(s)= F.D.Becchetti, Jr. and G.W.Greenlees
Reference= Phys. Rev. 182,1190 (1969)
Summary= derived by fitting total and diff. elastic cross sections of
several nuclides
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 101 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 12-83 A-Range= 24-209 E-Range= 11- 11 MeV
Author(s)= J.C.Ferrer,J.D.Carlson and J.Rapaport
Reference= Nucl.Phys.A275,325(1977)
Summary= Derived by fitting pure diff. elastic cross sections of several
nuclides
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 102 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 82-82 A-Range= 206-208 E-Range= 5- 50 MeV
Author(s)= R.W.Finlay et al.
Reference= Phys. Rev. C 30, 796 (1984)
Summary= derived by fitting elastic cross sections of lead
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 103 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-26 A-Range= 56- 56 E-Range= 0-100 MeV
Author(s)= A.Prince
Reference= Int. Conf. on Nucl. Data, Antwerp ,1982
Summary= derived by applying sprt method and elastic and differential
elastic cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 104 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-26 A-Range= 54- 54 E-Range= 0-100 MeV
Author(s)= A.Prince
Reference= Int. Conf. on Nucl. Data, Antwerp ,1982
Summary= derived by applying sprt method and elastic and differential
elastic cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 105 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-26 A-Range= 57- 57 E-Range= 0-100 MeV
Author(s)= A.Prince
Reference= Int. Conf. on Nucl. Data, Antwerp ,1982
Summary= derived by applying sprt method and elastic and differential
elastic cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 106 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-26 A-Range= 58- 58 E-Range= 0-100 MeV
Author(s)= A.Prince
Reference= Int. Conf. on Nucl. Data, Antwerp ,1982
Summary= derived by applying sprt method and elastic and differential
elastic cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 107 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 58- 58 E-Range= 0-100 MeV
Author(s)= A.Prince
Reference= Int. Conf. on Nucl. Data, Antwerp ,1982
Summary= derived by applying sprt method and elastic and differential
elastic cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 108 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 60- 60 E-Range= 0-100 MeV
Author(s)= A.Prince
Reference= Int. Conf. on Nucl. Data, Antwerp ,1982
Summary= derived by applying sprt method and elastic and differential
elastic cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 109 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 61- 61 E-Range= 0-100 MeV
Author(s)= A.Prince
Reference= Int. Conf. on Nucl. Data, Antwerp ,1982
Summary= derived by applying sprt method and elastic and differential
elastic cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 110 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 62- 62 E-Range= 0-100 MeV
Author(s)= A.Prince
Reference= Int. Conf. on Nucl. Data, Antwerp ,1982
Summary= derived by applying sprt method and elastic and differential
elastic cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 111 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 64- 64 E-Range= 0-100 MeV
Author(s)= A.Prince
Reference= Int. Conf. on Nucl. Data, Antwerp ,1982
Summary= derived by applying sprt method and elastic and differential
elastic cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 112 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 24-24 A-Range= 50- 50 E-Range= 0-100 MeV
Author(s)= A.Prince
Reference= Int. Conf. on Nucl. Data, Antwerp ,1982
Summary= derived by applying sprt method and elastic and differential
elastic cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 113 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 24-24 A-Range= 53- 53 E-Range= 0-100 MeV
Author(s)= A.Prince
Reference= Int. Conf. on Nucl. Data, Antwerp ,1982
Summary= derived by applying sprt method and elastic and differential
elastic cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 114 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 24-24 A-Range= 52- 52 E-Range= 0-100 MeV
Author(s)= A.Prince
Reference= Int. Conf. on Nucl. Data, Antwerp ,1982
Summary= derived by applying sprt method and elastic and differential
elastic cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 115 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 24-24 A-Range= 54- 54 E-Range= 0-100 MeV
Author(s)= A.Prince
Reference= Int. Conf. on Nucl. Data, Antwerp ,1982
Summary= derived by applying sprt method and elastic and differential
elastic cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 116 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-83 A-Range= 40-209 E-Range= 0- 5 MeV
Author(s)= P.A.Moldauer
Reference= Nucl. Phys. 47,65(1963)
Summary= Based on analysis of low-energy neutron data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 117 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 13-13 A-Range= 27- 27 E-Range= 0- 60 MeV
Author(s)= J.Petler,M.S.Islam, and R.W.Finlay
Reference= Phys. Rev. C 32 ,673 (1985)
Summary= potential specifically developed for neutron interaction with al-27
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 118 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 39-51 A-Range= 85-125 E-Range= 0- 5 MeV
Author(s)= A.B.Smith,P.T.Guenther,J.F.Whalen
Reference= Nucl. Phys. A415,1 (1984)
Summary= Based on fits to measurements of total and differential elastic
scattering cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 119 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 67-67 A-Range= 165-165 E-Range= 0- 30 MeV
Author(s)= A.B.Smith
Reference= Report ANL/NDM-151 (December, 2000)
Summary= "Fast-Neutron Incident on Holmium". Based on analysis of
differential elastic scattering cross section data at incident
neutrons between 4.5-10.0 MeV measured at 40 angles or more. Pure
coupled-channel analysis incorporating 7/2- ground-state rotational
band.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 120 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and dispersive (Anal.Integr.)
Z-Range= 67-67 A-Range= 165-165 E-Range= 0- 30 MeV
Author(s)= A.B.Smith
Reference= Report ANL/NDM-151 (December, 2000)
Summary= "Fast-Neutron Incident on Holmium". Results from analyzing the same
differential elastic scattering cross section data between 4.5-10.0
MeV as RIPL ref.#119 but using a dispersive coupled-channel
potential incorporating 7/2- ground-state rotational band.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 121 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive (Anal.Integr.)
Z-Range= 82-82 A-Range= 208-208 E-Range= 0- 80 MeV
Author(s)= G.J.Weisel, W.Tornow et al
Reference= Phys. Rev. C 54,2410-2428 (1996)
Summary= A relativistic dispersive OMP for Pb-208. Fully constrained set
w/Wso from 4th column, Table II(p.2420)
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 122 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive (Anal.Integr.)
Z-Range= 83-83 A-Range= 209-209 E-Range= 0- 80 MeV
Author(s)= G.J.Weisel, W.Tornow et al
Reference= Phys. Rev. C 54,2410-2428 (1996)
Summary= A relativistic dispersive OMP for Bi-209. Fully constrained set
w/Wso from 4th column, Table II(p.2420)
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 123 Neutron incident, CC vibrational model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 148-150 E-Range= 0- 15 MeV
Author(s)= M.T.McEllistrem,R.E.Shamu,J.Lachkar,G.Haouat,Ch.Lagrange,Y.Patin et
al.
Reference= Phys.Rev.C 15,927(1977).
Summary= Deformation Effects in Neutron Scattering from the Sm Isotopes.
Vibrational model used for 148,150Sm [RIPL#123]. Rotational model
used for 150,152,154Sm [RIPL#124]. Saturation of Wd assumed at 10
MeV, as in earlier publication, Lagrange et al.,
Phys.Lett.58B,293(1975).
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 124 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 150-152 E-Range= 0- 15 MeV
Author(s)= M.T.McEllistrem,R.E.Shamu,J.Lachkar,G.Haouat,Ch.Lagrange,Y.Patin et
al.
Reference= Phys.Rev.C 15,927(1977).
Summary= Deformation Effects in Neutron Scattering from the Sm Isotopes.
Vibrational model used for 148,150Sm [RIPL#123]. Rotational model
used for 150,152,154Sm [RIPL#124]. Saturation of Wd assumed at 10
MeV, as in earlier publication, Lagrange et al.,
Phys.Lett.58B,293(1975).
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 125 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-26 A-Range= 54- 54 E-Range= 8- 14 MeV
Author(s)= S.M.El-Kadi,C.E.Nelson,F.O.Purser,R.L.Walter,A.Beyerle,C.R.Gould,L.W
.Seagondolla
Reference= Nucl.Phys. A390,509(1982).
Summary= (I).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and
63,65Cu. Spherical optical model potential from 54Fe experimental
data [Table 4]. See RIPL#129 and 130 for global spherical
potentials [Table 5]. Also, see RIPL#424-427 for vibrational model
potentials.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 126 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-26 A-Range= 56- 56 E-Range= 8- 14 MeV
Author(s)= S.M.El-Kadi,C.E.Nelson,F.O.Purser,R.L.Walter,A.Beyerle,C.R.Gould,L.W
.Seagondolla
Reference= Nucl.Phys. A390,509(1982).
Summary= (I).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and
63,65Cu. Spherical optical model potential from 56Fe experimental
data [Table 4]. See RIPL#129 and 130 for global spherical
potentials [Table 5]. Also, see RIPL#424-427 for vibrational model
potentials.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 127 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 29-29 A-Range= 63- 63 E-Range= 8- 14 MeV
Author(s)= S.M.El-Kadi,C.E.Nelson,F.O.Purser,R.L.Walter,A.Beyerle,C.R.Gould,L.W
.Seagondolla
Reference= Nucl.Phys. A390,509(1982).
Summary= (I).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and
63,65Cu. Spherical optical model potential from 63Cu experimental
data [Table 4]. See RIPL#129 and 130 for global spherical
potentials [Table 5]. Also, see RIPL#424-427 for vibrational model
potentials.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 128 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 29-29 A-Range= 65- 65 E-Range= 8- 14 MeV
Author(s)= S.M.El-Kadi,C.E.Nelson,F.O.Purser,R.L.Walter,A.Beyerle,C.R.Gould,L.W
.Seagondolla
Reference= Nucl.Phys. A390,509(1982).
Summary= (I).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and
63,65Cu. Spherical optical model potential from 65Cu experimental
data [Table 4]. See RIPL#129 and 130 for global spherical
potentials [Table 5]. Also, see RIPL#424-427 for vibrational model
potentials.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 129 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-29 A-Range= 54- 65 E-Range= 8- 30 MeV
Author(s)= S.M.El-Kadi,C.E.Nelson,F.O.Purser,R.L.Walter,A.Beyerle,C.R.Gould,L.W
.Seagondolla
Reference= Nucl.Phys. A390,509(1982).
Summary= (I).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and
63,65Cu. Global spherical potential [global set A in Table 5] See
RIPL#125-128 for spherical potentials directly from data. Also, see
RIPL#424-427 for vibrational model potentials.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 130 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-29 A-Range= 54- 65 E-Range= 8- 30 MeV
Author(s)= S.M.El-Kadi,C.E.Nelson,F.O.Purser,R.L.Walter,A.Beyerle,C.R.Gould,L.W
.Seagondolla
Reference= Nucl.Phys. A390,509(1982).
Summary= (I).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and
63,65Cu. Global spherical potential [global set B in Table 5] See
RIPL#125-128 for spherical potentials directly from data. Also, see
RIPL#424-427 for vibrational model potentials.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 131 Neutron incident, CC vibrational model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 58- 60 E-Range= 0- 80 MeV
Author(s)= P.P.Guss,R.C.Byrd,C.E.Floyd,C.R.Howell,K.Murphy,G.Tungate...,J.P.Del
aroche
Reference= Nucl.Phys. A438,187(1985).
Summary= Cross Sections and Analyzing Powers for Fast-Neutron Scattering to
the Ground and First Excited States of 58Ni and 60Ni. Vibrational
model analysis with ECIS coupled-channels code [see discussion
p.195 of Nucl.Phys. A438 on 2+ state reorientation matrix]. See
RIPL#132 for spherical potential.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 132 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 58- 60 E-Range= 0- 80 MeV
Author(s)= P.P.Guss,R.C.Byrd,C.E.Floyd,C.R.Howell,K.Murphy,G.Tungate...,J.P.Del
aroche
Reference= Nucl.Phys. A438,187(1985).
Summary= Cross Sections and Analyzing Powers for Fast-Neutron Scattering to
the Ground and First Excited States of 58Ni and 60Ni. Spherical
optical model analysis.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 133 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 22-22 A-Range= 44- 50 E-Range= 0- 20 MeV
Author(s)= D.W.Muir and E.D.Arthur
Reference= Journal of Nucl.Mat.122&123, 1058 (1984)
Summary= Improved Activation Cross Sections for Vanadium and Titanium
Spherical potentials used in calculations of fusion blankets.
Titanium potential.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 134 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 23-23 A-Range= 50- 51 E-Range= 0- 20 MeV
Author(s)= D.W.Muir and E.D.Arthur
Reference= Journal of Nucl.Mat.122&123, 1058 (1984)
Summary= Improved Activation Cross Sections for Vanadium and Titanium
Spherical potentials used in calculations of fusion blankets.
Vanadium potential.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 136 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 7- 7 A-Range= 14- 14 E-Range= 18- 60 MeV
Author(s)= M.S.Islam,R.W.Finlay,J.S.Petler,J.Rapaport,R.Alarcon
Reference= Phys.in Med.and Biol.33,315(1988).
Summary= Neutron Scattering Cross Sections and Partial Kerma Values for
Oxygen, Nitrogen and Calcium at 18<En<60 MeV. Spherical optical
model analysis of total,differential elastic and inelastic
scattering data. 14N potential.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 137 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 8- 8 A-Range= 16- 16 E-Range= 18- 60 MeV
Author(s)= M.S.Islam,R.W.Finlay,J.S.Petler,J.Rapaport,R.Alarcon
Reference= Phys.in Med.and Biol.33,315(1988).
Summary= Neutron Scattering Cross Sections and Partial Kerma Values for
Oxygen, Nitrogen and Calcium at 18<En<60 MeV. Spherical optical
model analysis of total,differential elastic and inelastic
scattering data. 14N potential.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 138 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-20 A-Range= 40- 40 E-Range= 18- 60 MeV
Author(s)= M.S.Islam,R.W.Finlay,J.S.Petler,J.Rapaport,R.Alarcon
Reference= Phys.in Med.and Biol.33,315(1988).
Summary= Neutron Scattering Cross Sections and Partial Kerma Values for
Oxygen, Nitrogen and Calcium at 18<En<60 MeV. Spherical optical
model analysis of total,differential elastic and inelastic
scattering data. 14N potential.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 139 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 90-90 A-Range= 232-232 E-Range= 0- 20 MeV
Author(s)= A.B.Smith and S.Chiba
Reference= Ann.Nucl.Energy 23(1996) 459-467
Summary= "Neutron scattering from elemental uranium and thorium". Based on
analysis of differential elastic scattering cross section data at
incident neutrons between 4.5-10.0 MeV measured at 40 angles or
more. Coupled-channel OMP for Th-232.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 140 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 92-92 A-Range= 238-238 E-Range= 0- 20 MeV
Author(s)= A.B.Smith and S.Chiba
Reference= Ann.Nucl.Energy 23(1996) 459-467
Summary= "Neutron scattering from elemental uranium and thorium". Based on
analysis of differential elastic scattering cross section data at
incident neutrons between 4.5-10.0 MeV measured at 40 angles or
more. Coupled-channel OMP for U-238.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 200 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 31-69 A-Range= 69-146 E-Range= 0- 20 MeV
Author(s)= S.Igarasi
Reference= Japan At.Ener.Res. Insti. 1228 , 41 (1973)
Summary= potential developed at Japan At.Ener.Res. Insti. to analyze neutron
reaction data up to the mass range 146
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 201 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 69-74 A-Range= 147-186 E-Range= 0- 20 MeV
Author(s)= S.Igarasi
Reference= Japan At.Ener.Res. Insti. 1228 , 41 (1973)
Summary= potential developed at Japan At.Ener.Res. Insti. to analyze neutron
reaction data in the mass range above 146
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 202 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 33-37 A-Range= 61-107 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= Potential developed at Japan At.Ener.Res. Insti. to provide data
for fission products in the charge range 33 to 37
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 203 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 38-42 A-Range= 69-116 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed for fp nuclides in the charge range 38 to 42
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 204 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 43-45 A-Range= 80-125 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp in the charge range 43
to 45
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 205 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 46-48 A-Range= 89-134 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 46 to 48
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 206 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 49-51 A-Range= 97-141 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 49 to 51
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 207 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 52-54 A-Range= 103-150 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 52 to 54
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 208 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 55-55 A-Range= 111-153 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 55 to 55
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 209 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 56-56 A-Range= 112-154 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 56 to 56
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 210 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 57-58 A-Range= 117-156 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 57 to 58
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 211 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 59-59 A-Range= 119-160 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 59 to 59
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 212 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 60-60 A-Range= 141-143 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 60 to 60
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 213 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 60-60 A-Range= 144-148 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 60 to 60
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 214 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 60-60 A-Range= 150-999 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 60 to 60
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 215 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 61-61 A-Range= 147-999 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 61 to 61
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 216 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 144-144 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 62 to 62
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 217 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 147-147 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 62 to 62
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 218 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 148-148 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 62 to 62
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 219 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 149-149 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 62 to 62
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 220 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 150-150 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 62 to 62
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 221 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 63-63 A-Range= 151-999 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 63 to 63
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 222 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 64-64 A-Range= 133-171 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 64 to 64
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 223 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 65-65 A-Range= 138-175 E-Range= 0- 20 MeV
Author(s)= Japan At.Ener.Res. Insti.
Reference= JNDC FP Nucl. Data WG
Summary= potential developed to provide data for fp nuclides in the charge
range 65 to 65
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 240 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 31-69 A-Range= 69-146 E-Range= 0- 20 MeV
Author(s)= S.Igarasi
Reference= JAERI-M 5752 (1974)
Summary= Potential developed at the Japan Atomic Energy Research Institute
to analyze neutron reaction data in the mass range below A=147
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 241 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 69-74 A-Range= 147-186 E-Range= 0- 20 MeV
Author(s)= S.Igarasi
Reference= JAERI-M 5752 (1974)
Summary= Potential developed at the Japan Atomic Energy Research Institute
to analyze neutron reaction data in the mass range above A=146
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 242 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 13-13 A-Range= 27- 27 E-Range= 0-250 MeV
Author(s)= Y.O.Lee et al.
Reference= J. Nucl. Sci. Tech. 36, 1125-1134 (1999)
Summary= Spherical potential for 27Al to 250 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 243 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 13-47 A-Range= 27-109 E-Range= 0- 80 MeV
Author(s)= N.Yamamuro
Reference= Int.Conf.on NDST,Mito,1988 p.489
Summary= Nuclear Cross Section Calculations with a Simplified-Input Version
of Eliese-Gnash Joint Program Combined Walter-Guss (RIPL#2101)
potential above 20 MeV with a new potential below 20 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 400 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 79-79 A-Range= 197-197 E-Range= 0- 57 MeV
Author(s)= J.P.Delaroche
Reference= Int.Conf.on Neut.Phys. for Reactors, Harwell(1978)
Summary= Based on analysis of n and p data, making use of sprt method and
the Lane model
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 401 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-92 A-Range= 40-238 E-Range= 0- 25 MeV
Author(s)= D.Wilmore and P.E.Hodgson
Reference= Nucl. Phys. 55,673 (1964)
Summary= derived by fitting total and diff. elastic cross sections of
several nuclides ranging from si to u
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 402 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 83-83 A-Range= 209-209 E-Range= 0- 30 MeV
Author(s)= O.Bersillon
Reference= CEA Report CEA-N-2284 (1982) p.130 and NEANDC-222U
Summary= derived by fitting elastic and total cross sections of bismuth
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 403 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 74-74 A-Range= 182-186 E-Range= 0- 30 MeV
Author(s)= J.P.Delaroche et al.
Reference= Int. Conf. on Nucl. Data, Knoxville,TN,1979
Summary= derived by fitting elastic and total cross sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 404 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 23-41 A-Range= 50- 95 E-Range= 0- 30 MeV
Author(s)= B.Strohmaier et al
Reference= IAEA Advisory Group Meeting, Rad.Damage 1981
Summary= Total and diff. elastic x-sections , av. reson. strength function
and (n,nx),(n,px) and (n,alpha x) data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 406 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 94-94 A-Range= 236-244 E-Range= 0- 20 MeV
Author(s)= Ch.Lagrange
Reference= CEA-N-1970, NEANDC(E) 179 "L", INDC(FR) 16/L (1977)
Summary= Calculs dans le cadre du modele optique en voies couplees de
sections efficaces neutroniques pour 236Pu, 238Pu, 240Pu, 244Pu
dans le domaine d-energie 1 keV - 20 MeV
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 408 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 90-90 A-Range= 230-232 E-Range= 0- 20 MeV
Author(s)= Ch.Lagrange
Reference= NEANDC(E)228 "L", INDC(FR) 56/L (1982)
Summary= Results of Coupled-Channels Calculations for the Neutron Cross
Sections of a Set of Actinide Nuclei. Included are parameters for
230,232Th, 234,238U, 242Pu, 246Cm, 252Cf.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 409 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 92-92 A-Range= 234-234 E-Range= 0- 20 MeV
Author(s)= Ch.Lagrange
Reference= NEANDC(E)228 "L", INDC(FR) 56/L (1982)
Summary= Results of Coupled-Channels Calculations for the Neutron Cross
Sections of a Set of Actinide Nuclei. Included are parameters for
230,232Th, 234,238U, 242Pu, 246Cm, 252Cf.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 410 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 92-92 A-Range= 238-238 E-Range= 0- 20 MeV
Author(s)= Ch.Lagrange
Reference= NEANDC(E)228 "L", INDC(FR) 56/L (1982)
Summary= Results of Coupled-Channels Calculations for the Neutron Cross
Sections of a Set of Actinide Nuclei. Included are parameters for
230,232Th, 234,238U, 242Pu, 246Cm, 252Cf.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 411 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 94-94 A-Range= 242-242 E-Range= 0- 20 MeV
Author(s)= Ch.Lagrange
Reference= NEANDC(E)228 "L", INDC(FR) 56/L (1982)
Summary= Results of Coupled-Channels Calculations for the Neutron Cross
Sections of a Set of Actinide Nuclei. Included are parameters for
230,232Th, 234,238U, 242Pu, 246Cm, 252Cf.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 412 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 96-96 A-Range= 246-246 E-Range= 0- 20 MeV
Author(s)= Ch.Lagrange
Reference= NEANDC(E)228 "L", INDC(FR) 56/L (1982)
Summary= Results of Coupled-Channels Calculations for the Neutron Cross
Sections of a Set of Actinide Nuclei. Included are parameters for
230,232Th, 234,238U, 242Pu, 246Cm, 252Cf.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 413 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 98-98 A-Range= 252-252 E-Range= 0- 20 MeV
Author(s)= Ch.Lagrange
Reference= NEANDC(E)228 "L", INDC(FR) 56/L (1982)
Summary= Results of Coupled-Channels Calculations for the Neutron Cross
Sections of a Set of Actinide Nuclei. Included are parameters for
230,232Th, 234,238U, 242Pu, 246Cm, 252Cf.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 414 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 90-90 A-Range= 232-232 E-Range= 0- 20 MeV
Author(s)= G.Haouat,J.Lachkar,Ch.Lagrange
Reference= Nucl.Sci.Engr.81,491(1982)
Summary= Neutron Scattering Cross Sections for 232Th, 233U, 235U, 238U,
239Pu, and 242Pu Between 0.6 and 3.4 MeV. Note that the actual
energy range of the experiments in this paper is 0.6 to 3.4 MeV but
the parameterization is assumed valid to approximately 20 MeV,
after saturation of Wd at 10 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 415 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 92-92 A-Range= 235-235 E-Range= 0- 20 MeV
Author(s)= G.Haouat,J.Lachkar,Ch.Lagrange
Reference= Nucl.Sci.Engr.81,491(1982)
Summary= Neutron Scattering Cross Sections for 232Th, 233U, 235U, 238U,
239Pu, and 242Pu Between 0.6 and 3.4 MeV. Note that the actual
energy range of the experiments in this paper is 0.6 to 3.4 MeV but
the parameterization is assumed valid to approximately 20 MeV,
after saturation of Wd at 10 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 416 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 92-94 A-Range= 238-239 E-Range= 0- 20 MeV
Author(s)= G.Haouat,J.Lachkar,Ch.Lagrange
Reference= Nucl.Sci.Engr.81,491(1982)
Summary= Neutron Scattering Cross Sections for 232Th, 233U, 235U, 238U,
239Pu, and 242Pu Between 0.6 and 3.4 MeV. Note that the actual
energy range of the experiments in this paper is 0.6 to 3.4 MeV but
the parameterization is assumed valid to approximately 20 MeV,
after saturation of Wd at 10 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 417 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 90-94 A-Range= 232-242 E-Range= 0- 20 MeV
Author(s)= G.Haouat,J.Lachkar,Ch.Lagrange
Reference= Nucl.Sci.Engr.81,491(1982)
Summary= Neutron Scattering Cross Sections for 232Th, 233U, 235U, 238U,
239Pu, and 242Pu Between 0.6 and 3.4 MeV. Note that the actual
energy range of the experiments in this paper is 0.6 to 3.4 MeV but
the parameterization is assumed valid to approximately 20 MeV,
after saturation of Wd at 10 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 418 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive (Anal.Integr.)
Z-Range= 13-13 A-Range= 27- 27 E-Range= 0-250 MeV
Author(s)= A.Molina, R.Capote, J.M.Quesada, M.Lozano.
Reference= Phys.Rev.C65,34616(2002)
Summary= A relativistic dispersive OMP for Al-27. Nonlocality in the volume
absorption was included. Requires OM code with relativistic
kinematics & total pot must be multiplied by 1 + E/(E+2*mc**2)
where E,m are for incident particle and E is th e total cm kinetic
energy (ECIS and SCAT2 do not need any modification )
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 419 Neutron incident, spherical nucleus model
Potential is non-relativistic and dispersive (Anal.Integr.)
Z-Range= 13-13 A-Range= 27- 27 E-Range= 0-150 MeV
Author(s)= A.Molina, R.Capote, J.M.Quesada, M.Lozano.
Reference= Phys.Rev.C65,34616(2002)
Summary= A non-relativistic dispersive OMP for Al-27
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 420 Neutron incident, CC vibrational model
Potential is non-relativistic and non-dispersive
Z-Range= 60-60 A-Range= 142-148 E-Range= 0- 15 MeV
Author(s)= G.Haouat,J.Lachkar,Ch.Lagrange,M.T.McEllistrem,Y.Patin,R.E.Shamu,J.S
igaud
Reference= Phys. Rev. C 20, 78 (1979).
Summary= Optical Potential and Nuclear Deformation for Even Nd Isotopes from
Fast Neutron Scattering. Vibrational model used for
142,144,146,148Nd [RIPL#420]. Rotational model used for 148,150Nd
[RIPL#421].
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 421 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 60-60 A-Range= 148-150 E-Range= 0- 15 MeV
Author(s)= G.Haouat,J.Lachkar,Ch.Lagrange,M.T.McEllistrem,Y.Patin,R.E.Shamu,J.S
igaud
Reference= Phys. Rev. C 20, 78 (1979).
Summary= Optical Potential and Nuclear Deformation for Even Nd Isotopes from
Fast Neutron Scattering. Vibrational model used for
142,144,146,148Nd [RIPL#420]. Rotational model used for 148,150Nd
[RIPL#421].
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 422 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 42-42 A-Range= 92-100 E-Range= 0- 20 MeV
Author(s)= Ch.Lagrange
Reference= Specialist Mtg on Neutron Data for Struct ...,Geel (1977)
Summary= Coherent Optical and Statistical Model Calculations of Neutron
Cross Sections for Mo Isotopes. Uses SPRT method to obtain
spherical potential.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 423 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 74-74 A-Range= 182-186 E-Range= 0- 9 MeV
Author(s)= J.P.Delaroche,G.Haouat,J.Lachkar,Y.Patin,J.Sigaud,J.Chardine
Reference= Phys. Rev. C 23, 136 (1981).
Summary= Deformations, Moments, and Radii of 182,183,184,186W from Fast
Neutron Scattering. Coupled-channels deformed optical model
analysis of direct experimental data only. See RIPL#2406 and 5406
for extended energy range and Lane model use.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 424 Neutron incident, CC vibrational model
Potential is non-relativistic and non-dispersive
Z-Range= 26-26 A-Range= 54- 54 E-Range= 0- 14 MeV
Author(s)= J.P.Delaroche,S.M.El-Kadi,P.P.Guss,C.E.Floyd,R.L.Walter
Reference= Nucl.Phys. A390,541(1982).
Summary= (II).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and
63,65Cu. Coupled-channels analysis with vibrational model - 54Fe.
See RIPL#125-130 for spherical potentials directly from same data.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 425 Neutron incident, CC vibrational model
Potential is non-relativistic and non-dispersive
Z-Range= 26-26 A-Range= 56- 56 E-Range= 0- 14 MeV
Author(s)= J.P.Delaroche,S.M.El-Kadi,P.P.Guss,C.E.Floyd,R.L.Walter
Reference= Nucl.Phys. A390,541(1982).
Summary= (II).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and
63,65Cu. Coupled-channels analysis with vibrational model - 56Fe.
See RIPL#125-130 for spherical potentials directly from same data.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 426 Neutron incident, CC vibrational model
Potential is non-relativistic and non-dispersive
Z-Range= 29-29 A-Range= 63- 63 E-Range= 0- 14 MeV
Author(s)= J.P.Delaroche,S.M.El-Kadi,P.P.Guss,C.E.Floyd,R.L.Walter
Reference= Nucl.Phys. A390,541(1982).
Summary= (II).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and
63,65Cu. Coupled-channels analysis with vibrational model - 63Cu.
See RIPL#125-130 for spherical potentials directly from same data.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 427 Neutron incident, CC vibrational model
Potential is non-relativistic and non-dispersive
Z-Range= 29-29 A-Range= 65- 65 E-Range= 0- 14 MeV
Author(s)= J.P.Delaroche,S.M.El-Kadi,P.P.Guss,C.E.Floyd,R.L.Walter
Reference= Nucl.Phys. A390,541(1982).
Summary= (II).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and
63,65Cu. Coupled-channels analysis with vibrational model - 65Cu.
See RIPL#125-130 for spherical potentials directly from same data.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 428 Neutron incident, CC vibrational model
Potential is non-relativistic and non-dispersive
Z-Range= 26-26 A-Range= 54- 56 E-Range= 0- 14 MeV
Author(s)= J.P.Delaroche,S.M.El-Kadi,P.P.Guss,C.E.Floyd,R.L.Walter
Reference= Nucl.Phys. A390,541(1982).
Summary= (II).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and
63,65Cu. Coupled-channels analysis with vibrational model - 54Fe
and 56Fe. See RIPL#125-130 for spherical potentials directly from
same data.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 429 Neutron incident, CC vibrational model
Potential is non-relativistic and non-dispersive
Z-Range= 29-29 A-Range= 63- 65 E-Range= 0- 14 MeV
Author(s)= J.P.Delaroche,S.M.El-Kadi,P.P.Guss,C.E.Floyd,R.L.Walter
Reference= Nucl.Phys. A390,541(1982).
Summary= (II).Elastic and Inelastic Scattering of Neutrons from 54,56Fe and
63,65Cu. Coupled-channels analysis with vibrational model - 63Cu
and 65Cu. See RIPL#125-130 for spherical potentials directly from
same data. 63Cu,65Cu calculation here is for 62Ni, 64Ni core 2+
states.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 430 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 13-82 A-Range= 27-208 E-Range= 0- 24 MeV
Author(s)= O.Bersillon and Cindro
Reference= Fifth Int. Sym. On Interactions of Fast Neutrons with Nuclei, Gaussi
g (1975)
Summary= Nonlocal neutron potential.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 500 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 31-31 A-Range= 69- 69 E-Range= 0- 20 MeV
Author(s)= Zhang Songbai (China Nuclear Data Center)
Reference= Communication of Nuclear Data Progress, No.21(1999)52
Summary= potential for neutron reactions on Ga-69 and Ga-71 nuclides
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 501 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 36-36 A-Range= 83- 83 E-Range= 0- 20 MeV
Author(s)= Cai Chonghai (Nankai University, Tianjin, P.R.China)
Reference= Communication of Nuclear Data Progress, No.21(1999)40
Summary= potential for neutron reactions on Kr-83,84,85 nuclides
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 502 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 36-36 A-Range= 86- 86 E-Range= 0- 20 MeV
Author(s)= Cai Chonghai (Nankai University, Tianjin, P.R.China)
Reference= Unpublished
Summary= potential for neutron reactions on Kr-86 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 503 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 37-37 A-Range= 85- 85 E-Range= 0- 20 MeV
Author(s)= Cai Chonghai (Nankai University, Tianjin, P.R.China)
Reference= Communication of Nuclear Data Progress, No.20(1998)70
Summary= potential for neutron reactions on Rb-85,87 nuclides
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 504 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 38-38 A-Range= 88- 88 E-Range= 0- 20 MeV
Author(s)= Cai Chonghai (Nankai University, Tianjin, P.R.China)
Reference= Communication of Nuclear Data Progress, No.20(1998)47
Summary= potential for neutron reactions on Sr-88,89,90 nuclides
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 505 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 39-39 A-Range= 89- 89 E-Range= 0- 20 MeV
Author(s)= Cai Chonghai (Nankai University, Tianjin, P.R.China)
Reference= Communication of Nuclear Data Progress, No.21(1999)39
Summary= potential for neutron reactions on Y-89 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 506 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 39-39 A-Range= 91- 91 E-Range= 0- 20 MeV
Author(s)= Cai Chonghai (Nankai University, Tianjin, P.R.China)
Reference= Unpublished
Summary= potential for neutron reactions on Y-91 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 507 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 41-41 A-Range= 93- 93 E-Range= 0- 20 MeV
Author(s)= Rong Jian, Zhang Zhengjun (China Nuclear Data Center)
Reference= Unpublished
Summary= Potential for neutron reactions on Nb-93 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 508 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 41-41 A-Range= 95- 95 E-Range= 0- 20 MeV
Author(s)= Rong Jian, Zhang Zhengjun (China Nuclear Data Center)
Reference= Unpublished
Summary= Potential for neutron reactions on Nb-95 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 509 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 42-42 A-Range= 95- 95 E-Range= 0- 20 MeV
Author(s)= Cai Chonghai
Reference= Unpublished
Summary= potential for neutron reactions on Mo-95 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 510 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 42-42 A-Range= 97- 97 E-Range= 0- 20 MeV
Author(s)= Cai Chonghai, Ge Zhigang (China Nuclear Data Center)
Reference= Unpublished
Summary= potential for neutron reactions on Mo-97 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 511 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 42-42 A-Range= 98- 98 E-Range= 0- 20 MeV
Author(s)= Cai Chonghai, Ge Zhigang (China Nuclear Data Center)
Reference= Unpublished
Summary= potential for neutron reactions on Mo-98 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 512 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 42-42 A-Range= 100-100 E-Range= 0- 20 MeV
Author(s)= Cai Chonghai (Nankai University, Tianjin, P.R.China)
Reference= Unpublished
Summary= potential for neutron reactions on Mo-100 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 513 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 43-43 A-Range= 99- 99 E-Range= 0- 20 MeV
Author(s)= Cai Chonghai (Nankai University, Tianjin, P.R.China)
Reference= Unpublished
Summary= potential for neutron reactions on Tc-99 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 514 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 44-44 A-Range= 99- 99 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Ru-99 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 515 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 44-44 A-Range= 100-100 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Ru-100 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 516 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 44-44 A-Range= 101-101 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun, Ge Zhigang (China Nuclear Data Center)
Reference= Unpublished
Summary= potential for neutron reactions on Ru-101 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 517 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 44-44 A-Range= 102-102 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Ru-102 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 518 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 44-44 A-Range= 103-103 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun, Ge Zhigang (China Nuclear Data Center)
Reference= Unpublished
Summary= potential for neutron reactions on Ru-103 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 519 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 44-44 A-Range= 104-104 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Ru-104 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 520 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 44-44 A-Range= 105-105 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Ru-105 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 521 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 45-45 A-Range= 103-103 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Rh-103 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 522 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 45-45 A-Range= 105-105 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Rh-105 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 523 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 46-46 A-Range= 105-105 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun et al.
Reference= Unpublished
Summary= potential for neutron reactions on Pd-105 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 524 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 46-46 A-Range= 108-108 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun et al.
Reference= Unpublished
Summary= potential for neutron reactions on Pd-108 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 525 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 48-48 A-Range= 113-113 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun et al.
Reference= Communication of Nuclear Data Progress, No. 20(1998)77.
Summary= potential for neutron reactions on Cd-113 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 526 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 49-49 A-Range= 115-115 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun et al.
Reference= Communication of Nuclear Data Progress, No. 20(1998)64.
Summary= potential for neutron reactions on In-115 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 527 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 51-51 A-Range= 121-121 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun et al.
Reference= Communication of Nuclear Data Progress, No. 20(1998)82.
Summary= potential for neutron reactions on Sb-121 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 528 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 51-51 A-Range= 123-123 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun et al.
Reference= Communication of Nuclear Data Progress, No. 20(1998)82.
Summary= potential for neutron reactions on Sb-123 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 529 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 52-52 A-Range= 130-130 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun et al.
Reference= Unpublished
Summary= potential for neutron reactions on Te-130 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 530 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 53-53 A-Range= 127-127 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun et al.
Reference= Unpublished
Summary= potential for neutron reactions on I-127 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 531 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 53-53 A-Range= 135-135 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun et al.
Reference= Unpublished
Summary= potential for neutron reactions on I-135 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 532 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 54-54 A-Range= 123-123 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Xe-123 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 533 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 54-54 A-Range= 124-124 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Xe-124 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 534 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 54-54 A-Range= 129-129 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao, Zhang Zhengjun (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Xe-129 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 535 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 54-54 A-Range= 131-131 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao, Zhang Zhengjun (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Xe-124 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 536 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 54-54 A-Range= 132-132 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao, Zhang Zhengjun (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Xe-132 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 537 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 54-54 A-Range= 134-134 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao, Zhang Zhengjun (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Xe-134 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 538 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 54-54 A-Range= 135-135 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao, Zhang Zhengjun (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Xe-135 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 539 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 54-54 A-Range= 136-136 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao, Zhang Zhengjun (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Xe-136 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 540 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 55-55 A-Range= 133-133 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Cs-133 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 541 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 55-55 A-Range= 134-134 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Cs-134 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 542 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 55-55 A-Range= 135-135 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Cs-135 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 543 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 55-55 A-Range= 137-137 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Ce-137 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 544 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 56-56 A-Range= 135-135 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Ba-135 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 545 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 56-56 A-Range= 136-136 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Ba-136 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 546 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 56-56 A-Range= 137-137 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Ba-137 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 547 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 56-56 A-Range= 138-138 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Ba-138 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 548 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 57-57 A-Range= 139-139 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for La-139 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 549 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 58-58 A-Range= 140-140 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Ce-140 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 550 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 58-58 A-Range= 141-141 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Ce-141 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 551 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 58-58 A-Range= 142-142 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Ce-142 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 552 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 58-58 A-Range= 144-144 E-Range= 0- 20 MeV
Author(s)= Zhang Zhengjun (Phys. Dept. of Northwest Univ., Xian)
Reference= Unpublished
Summary= potential developed for Ce-144 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 553 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 59-59 A-Range= 141-141 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Pr-141 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 554 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 60-60 A-Range= 142-142 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Nd-142 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 555 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 60-60 A-Range= 143-143 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Nd-143 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 556 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 60-60 A-Range= 144-144 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Nd-144 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 557 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 60-60 A-Range= 145-145 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Nd-145 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 558 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 60-60 A-Range= 146-146 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Nd-146 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 559 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 60-60 A-Range= 147-147 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Nd-147 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 560 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 60-60 A-Range= 148-148 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Nd-148 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 561 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 60-60 A-Range= 150-150 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Nd-150 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 562 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 61-61 A-Range= 147-147 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Pm-147 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 563 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 61-61 A-Range= 148-148 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Pm-148 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 564 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 61-61 A-Range= 149-149 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Pm-149 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 565 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 144-144 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Sm-144 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 566 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 147-147 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Sm-147 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 567 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 148-148 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Sm-148 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 568 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 149-149 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Sm-149 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 569 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 150-150 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Sm-150 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 570 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 151-151 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Sm-151 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 571 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 152-152 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Sm-152 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 572 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 154-154 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Sm-154 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 573 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 63-63 A-Range= 151-151 E-Range= 0- 20 MeV
Author(s)= Ge Zhigang (China Nuclear Data Center)
Reference= Communication of Nuclear Data Progress, No.21(1999)35
Summary= potential for neutron reactions on Ru-151 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 574 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 63-63 A-Range= 153-153 E-Range= 0- 20 MeV
Author(s)= Ge Zhigang (China Nuclear Data Center)
Reference= Communication of Nuclear Data Progress, No.21(1999)35
Summary= potential for neutron reactions on Ru-153 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 575 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 63-63 A-Range= 154-154 E-Range= 0- 20 MeV
Author(s)= Ge Zhigang (China Nuclear Data Center)
Reference= Communication of Nuclear Data Progress, No.21(1999)35
Summary= potential for neutron reactions on Ru-154 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 576 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 63-63 A-Range= 155-155 E-Range= 0- 20 MeV
Author(s)= Ge Zhigang (China Nuclear Data Center)
Reference= Communication of Nuclear Data Progress, No.21(1999)35
Summary= potential for neutron reactions on Ru-155 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 577 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 64-64 A-Range= 152-152 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Gd-152 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 578 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 64-64 A-Range= 154-154 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Gd-154 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 579 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 64-64 A-Range= 155-155 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Gd-155 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 580 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 64-64 A-Range= 156-156 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Gd-156 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 581 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 64-64 A-Range= 157-157 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Gd-157 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 582 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 64-64 A-Range= 158-158 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Gd-158 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 583 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 64-64 A-Range= 160-160 E-Range= 0- 20 MeV
Author(s)= Shen Qingbiao (China Nuclear Data Center)
Reference= Unpublished
Summary= potential developed for Gd-160 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 584 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 66-66 A-Range= 164-164 E-Range= 0- 20 MeV
Author(s)= Ge Zhigang (China Nuclear Data Center)
Reference= Unpublished
Summary= potential for neutron reactions on Dy-164 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 585 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 69-69 A-Range= 169-169 E-Range= 0- 20 MeV
Author(s)= Ge Zhigang (China Nuclear Data Center)
Reference= Unpublished
Summary= potential for neutron reactions on Tm-169 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 586 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 71-71 A-Range= 174-174 E-Range= 0- 20 MeV
Author(s)= Han Yinlu (China Nuclear Data Center)
Reference= Unpublished
Summary= potential for neutron reactions on Lu-174 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 587 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 71-71 A-Range= 175-175 E-Range= 0- 20 MeV
Author(s)= Han Yinlu (China Nuclear Data Center)
Reference= Unpublished
Summary= potential for neutron reactions on Lu-175 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 600 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 90-** A-Range= 227-260 E-Range= 0- 20 MeV
Author(s)= G.Vladuca , A.Tudora , and M.Sin
Reference= Rom. J. Phys. 41 (1996) 515-526
Summary= Regional phenomenological deformed optical potential for neutron
interactions with actinides. Coupled-channels calculations
performed with ECIS-95 code. Authors: Z-Range=90-103,
A-Range=227-260. Lower range in library corresponds to structure
data included in library.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 601 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 92-92 A-Range= 238-238 E-Range= 0-200 MeV
Author(s)= V.M.Maslov, Yu.V.Porodzinskij, N.A.Tetereva, M.Baba, A.Hasegawa
Reference= Nucl. Phys. A736, 77-92 (2004)
Summary= Rigid rotor OMP valid for incident energies from 1 kev to 200 MeV.
Best description of the total cross section data for U238 Wd:
10.915 = 9.315 + 0.08*20 ; Wv50: 3.75 = 5 - 0.025*50; Wv80: 4.15 =
5.75 - 0.02*80;
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 602 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 92-92 A-Range= 238-238 E-Range= 0-200 MeV
Author(s)= V.M.Maslov, Yu.V.Porodzinskij, N.A.Tetereva, M.Baba, A.Hasegawa
Reference= Nucl. Phys. A736, 77-92 (2004)
Summary= Rigid rotor OMP valid for incident energies from 1 kev to 200 MeV.
Best description of the fission cross section data for U238 Wd14:
10.123 = 8.443 + 0.12*14 ; Wd50: 12.443 = 8.443 + 0.08*50; Wv14:
-1.12=-14*0.08; Wv50: -2.12=2.88 - 0.1*50; Wv80: 4.28=5.88 -
0.02*80;
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 603 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 90-92 A-Range= 230-234 E-Range= 0-200 MeV
Author(s)= V.M.Maslov
Reference= Private communication to NDS (Updated on Dec.22, 2004)
Summary= Best description of the total cross section data for Th232, U233
U233 deformation taken from INDC(BLR)-018, Maslov evaluation for
U233
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 604 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 90-92 A-Range= 230-234 E-Range= 0-200 MeV
Author(s)= V.M.Maslov
Reference= Private communication to NDS (Updated on Dec.22, 2004)
Summary= Best description of the fission cross section data for Th232
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 605 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 90-92 A-Range= 228-234 E-Range= 0-200 MeV
Author(s)= E.Soukhovitski, R. Capote, J.M. Quesada, S. Chiba
Reference= Unpublished.
Summary= A new dispersive coupled channel neutron OMP for incident energies
between 1 keV and 200 MeV valid for Th-U Local Fermi energy used.
Recommended for Th230,232,U233
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 606 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 92-92 A-Range= 236-240 E-Range= 0-200 MeV
Author(s)= E.Soukhovitski, R. Capote, J.M. Quesada, S. Chiba
Reference= Unpublished.
Summary= A new dispersive coupled channel neutron OMP for incident energies
between 1 keV and 200 MeV valid for U238. Local Fermi energy used.
Recommended for U238.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 607 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 92-92 A-Range= 232-234 E-Range= 0-200 MeV
Author(s)= E.Soukhovitski, R. Capote, J.M. Quesada, S. Chiba
Reference= Unpublished.
Summary= A new dispersive coupled channel neutron OMP for incident energies
between 1 keV and 200 MeV valid for U-233. Local Fermi energy used.
Recommended for U233
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 608 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 90-91 A-Range= 228-234 E-Range= 0-200 MeV
Author(s)= E.Soukhovitski, R. Capote, J.M. Quesada, S. Chiba.
Reference= Phys.Rev.C72 (2005) 024604
Summary= A dispersive coupled channel neutron OMP for incident energies
between 1 keV and 200 MeV valid for Th, fitted to the new average
cross section derived by Geel group from 1 to 150 keV. Included Pa
data with fitted deformations. Local Fermi energy used. Recommended
for Th232 and Pa-231,233. Used in ENDF-B/VII.0 evals.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 609 Neutron incident, CC soft rotor model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 40-40 A-Range= 90- 92 E-Range= 0-200 MeV
Author(s)= E.Soukhovitskii and R.Capote
Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper)
Summary= Lane consistent dispersive CC neutron OMP for incident energies
between 1 keV and 200 MeV for Zr isotopes. Recommended for
Zr-90,92. Local Fermi energy used. See 4609 for proton OMP. Soft
rotor, OPTMAN should be used.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 610 Proton incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 72-74 A-Range= 174-186 E-Range= 0-200 MeV
Author(s)= E.Soukhovitskii and R.Capote
Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper)
Summary= Lane consistent dispersive CC neutron OMP for incident energies
between 1 keV and 200 MeV for Hf-W-Ta isotopes. Recommended for
Hf-178,180, Ta-181, all W. Local Fermi energy used. See 4610 for
proton OMP. Soft rotor. OPTMAN should be used.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 800 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-83 A-Range= 40-210 E-Range= 0-155 MeV
Author(s)= C.A.Engelbrecht and H.Fiedeldey
Reference= Ann. Phys. 42,262-295 (1967)
Summary= Derived from non-local formalism to fit total and nonelastic
x-sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1400 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 12-12 A-Range= 24- 24 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1401 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 12-12 A-Range= 26- 26 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1402 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 13-13 A-Range= 27- 27 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1403 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 14-14 A-Range= 28- 28 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1404 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 15-15 A-Range= 31- 31 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1405 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 16-16 A-Range= 32- 32 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1406 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 17-17 A-Range= 35- 35 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1407 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 19-19 A-Range= 39- 39 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1408 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 18-18 A-Range= 40- 40 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1409 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 20-20 A-Range= 40- 40 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1410 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 21-21 A-Range= 45- 45 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1411 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 22-22 A-Range= 48- 48 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1412 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 23-23 A-Range= 51- 51 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1413 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 24-24 A-Range= 52- 52 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1414 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 26-26 A-Range= 54- 54 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1415 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 25-25 A-Range= 55- 55 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1416 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 26-26 A-Range= 56- 56 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1417 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 28-28 A-Range= 58- 58 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1418 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 28-28 A-Range= 60- 60 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1419 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 27-27 A-Range= 59- 59 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1420 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 29-29 A-Range= 63- 63 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1421 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 29-29 A-Range= 65- 65 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1422 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 31-31 A-Range= 69- 69 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1423 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 32-32 A-Range= 74- 74 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1424 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 33-33 A-Range= 75- 75 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1425 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 33-33 A-Range= 79- 79 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1426 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 34-34 A-Range= 80- 80 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1427 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 37-37 A-Range= 85- 85 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1428 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 38-38 A-Range= 88- 88 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1429 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 39-39 A-Range= 89- 89 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1430 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 40-40 A-Range= 90- 90 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1431 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 40-40 A-Range= 91- 91 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1432 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 40-40 A-Range= 92- 92 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1433 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 42-42 A-Range= 92- 92 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1434 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 41-41 A-Range= 93- 93 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1435 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 40-40 A-Range= 94- 94 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1436 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 42-42 A-Range= 94- 94 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1437 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 42-42 A-Range= 96- 96 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1438 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 42-42 A-Range= 98- 98 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1439 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 43-43 A-Range= 99- 99 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1440 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 42-42 A-Range= 100-100 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1441 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 45-45 A-Range= 103-103 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1442 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 46-46 A-Range= 106-106 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1443 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 47-47 A-Range= 107-107 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1444 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 48-48 A-Range= 114-114 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1445 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 49-49 A-Range= 115-115 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1446 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 50-50 A-Range= 116-116 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1447 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 50-50 A-Range= 118-118 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1448 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 50-50 A-Range= 120-120 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1449 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 51-51 A-Range= 121-121 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1450 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 50-50 A-Range= 122-122 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1451 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 51-51 A-Range= 123-123 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1452 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 50-50 A-Range= 124-124 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1453 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 53-53 A-Range= 127-127 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1454 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 52-52 A-Range= 128-128 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1455 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 55-55 A-Range= 133-133 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1456 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 56-56 A-Range= 138-138 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1457 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 57-57 A-Range= 139-139 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1458 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 58-58 A-Range= 140-140 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1459 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 59-59 A-Range= 141-141 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1460 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 60-60 A-Range= 142-142 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1461 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 60-60 A-Range= 144-144 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1462 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 62-62 A-Range= 148-148 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1463 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 78-78 A-Range= 194-194 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1464 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 79-79 A-Range= 197-197 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1465 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 80-80 A-Range= 202-202 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1466 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 82-82 A-Range= 206-206 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1467 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 82-82 A-Range= 208-208 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1468 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 83-83 A-Range= 209-209 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 2405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1469 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 12-12 A-Range= 24- 24 E-Range= 0-200 MeV
Author(s)= B.Morillon and P.Romain
Reference= Phys. Rev. C70, 014601 (2004); Phys. Rev. C74, 014601 (2006)
Summary= The following modifications are required to the published OMP
parameters: As = -17 + 0.018*A ; Bs = 13 ; Cs = 0.025 ; nonlocality
gamma = 0.1165 - 1e-4*A A dispersive spherical optical model
potential for neutrons with incident energies between 1 keV and 200
MeV. [Radius 1.299 is derived using Mg data].
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1470 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 13-13 A-Range= 27- 27 E-Range= 0-200 MeV
Author(s)= B.Morillon and P.Romain
Reference= Phys. Rev. C70, 014601 (2004); Phys. Rev. C74, 014601 (2006)
Summary= The following modifications are required to the published OMP
parameters: As = -17 + 0.018*A ; Bs = 13 ; Cs = 0.025 ; nonlocality
gamma = 0.1165 - 1e-4*A A dispersive spherical optical model
potential for neutrons with incident energies between 1 keV and 200
MeV. Radius 1.267 is derived using Al data.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1471 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 14-14 A-Range= 28- 28 E-Range= 0-200 MeV
Author(s)= B.Morillon and P.Romain
Reference= Phys. Rev. C70, 014601 (2004); Phys. Rev. C74, 014601 (2006)
Summary= The following modifications are required to the published OMP
parameters: As = -17 + 0.018*A ; Bs = 13 ; Cs = 0.025 ; nonlocality
gamma = 0.1165 - 1e-4*A A dispersive spherical optical model
potential for neutrons with incident energies between 1 keV and 200
MeV. Radius 1.280 is derived using Si data.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1472 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 16-16 A-Range= 32- 32 E-Range= 0-200 MeV
Author(s)= B.Morillon and P.Romain
Reference= Phys. Rev. C70, 014601 (2004); Phys. Rev. C74, 014601 (2006)
Summary= The following modifications are required to the published OMP
parameters: As = -17 + 0.018*A ; Bs = 13 ; Cs = 0.025 ; nonlocality
gamma = 0.1165 - 1e-4*A A dispersive spherical optical model
potential for neutrons with incident energies between 1 keV and 200
MeV. Radius 1.298 is derived using S data.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1473 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 20-20 A-Range= 40- 40 E-Range= 0-200 MeV
Author(s)= B.Morillon and P.Romain
Reference= Phys. Rev. C70, 014601 (2004); Phys. Rev. C74, 014601 (2006)
Summary= The following modifications are required to the published OMP
parameters: As = -17 + 0.018*A ; Bs = 13 ; Cs = 0.025 ; nonlocality
gamma = 0.1165 - 1e-4*A A dispersive spherical optical model
potential for neutrons with incident energies between 1 keV and 200
MeV. Radius 1.301 is derived using Ca data.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1474 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 22-22 A-Range= 46- 46 E-Range= 0-200 MeV
Author(s)= B.Morillon and P.Romain
Reference= Phys. Rev. C70, 014601 (2004); Phys. Rev. C74, 014601 (2006)
Summary= The following modifications are required to the published OMP
parameters: As = -17 + 0.018*A ; Bs = 13 ; Cs = 0.025 ; nonlocality
gamma = 0.1165 - 1e-4*A A dispersive spherical optical model
potential for neutrons with incident energies between 1 keV and 200
MeV. Radius 1.292 is derived using Ti data.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1475 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 26-26 A-Range= 56- 56 E-Range= 0-200 MeV
Author(s)= B.Morillon and P.Romain
Reference= Phys. Rev. C70, 014601 (2004); Phys. Rev. C74, 014601 (2006)
Summary= The following modifications are required to the published OMP
parameters: As = -17 + 0.018*A ; Bs = 13 ; Cs = 0.025 ; nonlocality
gamma = 0.1165 - 1e-4*A A dispersive spherical optical model
potential for neutrons with incident energies between 1 keV and 200
MeV. Radius 1.268 is derived using Fe data.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1476 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive (Num.Integr.)
Z-Range= 13-13 A-Range= 27- 27 E-Range= 0- 80 MeV
Author(s)= M.M.Nagadi,C.R.Howell,W.Tornow et al
Reference= Phys.Rev.C68,044610(2003)
Summary= Dispersive optical model with special exponential decrease of the
surface term. The dispersive integral is solved numerically in the
interface code.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1477 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive (Num.Integr.)
Z-Range= 27-27 A-Range= 59- 59 E-Range= 0- 80 MeV
Author(s)= M.M.Nagadi,C.R.Howell,W.Tornow et al
Reference= Phys.Rev.C68,044610(2003)
Summary= Dispersive optical model with special exponential decrease of the
surface term. The dispersive integral is solved numerically in the
interface code.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1479 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 45-45 A-Range= 100-104 E-Range= 0-200 MeV
Author(s)= L.C.Mihailescu,I.Sirakov,R.Capote,E.Soukhovitski, et al.
Reference= Proc.Int.Conf. on NDST, ND2007, Nice, France, #617, DOI: 10.1051/nda
ta:07617
Summary= Geometry is different for Vhf and Wv. Dispersive coupled channel
neutron OMP for incident energies between 1 keV and 200 MeV.
Recommended for Rh-100 - 104. Local Fermi energy used.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1480 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 74-74 A-Range= 182-182 E-Range= 0-200 MeV
Author(s)= R.Capote, E.Soukhovitski, J.M.Quesada, S.Chiba
Reference= Unpublished.
Summary= A dispersive coupled channel neutron OMP for incident energies
between 1 keV and200 MeV valid for W-182,183. Local Fermi energy
used. Used in IAEA eval (2008).
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1481 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 74-74 A-Range= 183-184 E-Range= 0-200 MeV
Author(s)= R.Capote, E.Soukhovitski, J.M.Quesada, S.Chiba
Reference= Unpublished.
Summary= A dispersive coupled channel neutron OMP for incident energies
between 1 keV and200 MeV valid for W-183,184. Local Fermi energy
used. Used in IAEA eval (2008).
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1482 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 74-74 A-Range= 185-186 E-Range= 0-200 MeV
Author(s)= R.Capote, E.Soukhovitski, J.M.Quesada, S.Chiba
Reference= Unpublished.
Summary= A dispersive coupled channel neutron OMP for incident energies
between 1 keV and200 MeV valid for W-186. Local Fermi energy used.
Used in IAEA eval (2008).
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1483 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 79-79 A-Range= 195-200 E-Range= 0-200 MeV
Author(s)= E.Soukhovitskii and R. Capote
Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper)
Summary= Lane consistent dispersive CC neutron OMP for incident energies
between 1 keV and 200 MeV for gold. Local Fermi energy used.
Geometry is different for Vhf and Wv.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1484 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 25-25 A-Range= 50- 56 E-Range= 0-200 MeV
Author(s)= E.Soukhovitskii and R. Capote
Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper)
Summary= Lane consistent dispersive CC neutron OMP for incident energies
between 1 keV and 200 MeV for Mn-55. Local Fermi energy used.
Geometry is different for Vhf and Wv.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 1485 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 45-45 A-Range= 100-104 E-Range= 0-200 MeV
Author(s)= E.Soukhovitskii and R. Capote
Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper)
Summary= Geometry is different for Vhf and Wv. Dispersive coupled channel
neutron OMP for incident energies between 1 keV and 200 MeV.
Recommended for Rh-100 - 104. Local Fermi energy used.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2001 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 6-82 A-Range= 12-208 E-Range= 50-400 MeV
Author(s)= D.G.Madland
Reference= OECD/NEA Spec. Mtg. Nucleon-Nucleus Opt.Mod.to 200 MeV,Paris (1997)
p.129.
Summary= Update of Semmering potential [NEANDC-245 U (1988)] to include
generalized imag. diff. parameter. Global pot for incid. neuts and
prots. Requires OM code with relativistic kine. & total pot must be
multiplied by 1 + E/(E+2*mc**2) where E,m are for incident particle
and E = total cm kinetic energy. Checked by author.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2002 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 74-74 A-Range= 182-186 E-Range= 0-100 MeV
Author(s)= P.G.Young,E.D.Arthur,M.Bozian,T.R.England,G.M.Hale,R.J.LaBauve,R.C.L
ittle,et al.
Reference= LANL Reports LA-11753-MS (1990); see also LA-8630-PR,p2 (1980)
Summary= parameters are based on neutron elastic ,inelastic,total and
differential data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2003 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 67-69 A-Range= 165-169 E-Range= 0-100 MeV
Author(s)= E.D.Arthur and C.Philis
Reference= Report LA-8630-PR,p2 (1980)
Summary= parameters are based on fits to tm-169 low energy resonance data
and total x-section data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2004 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 63-63 A-Range= 151-153 E-Range= 0- 20 MeV
Author(s)= R.Macklin and P.G.Young
Reference= Nucl.Sci.Eng. 95,189(1987)
Summary= parameterization was developed to provide radiative capture
x-sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2005 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 75-75 A-Range= 185-187 E-Range= 0- 20 MeV
Author(s)= R.Macklin and P.G.Young
Reference= Nucl.Sci.Eng. 97,239(1987)
Summary= parameterization was developed to provide radiative capture cross
sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2006 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 92-92 A-Range= 238-238 E-Range= 0-200 MeV
Author(s)= P.G.Young
Reference= LANL Progress Report LA-11972-PR (1990) p.9
Summary= Modification of potential by Haouat, Lachkar, Lagrange, et al., NSE
81 (1982) 49. Extension above 20 MeV is based on total cross
section data from WNR. Reaction cross section is too high by almost
20% at 200 MeV - modification needed above 20 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2007 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 67-69 A-Range= 165-169 E-Range= 0- 30 MeV
Author(s)= P.G.Young
Reference= Report LA-UR (1997)
Summary= Modification of Arthur-Phylis potential: LA-8630-PR, p.2 (1980)
[RIPL pot# 2003]
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2008 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 92-92 A-Range= 232-240 E-Range= 0- 30 MeV
Author(s)= P.G.Young and E.D.Arthur
Reference= LANL Report LA-UR-91-1424,894(1992); IAEA-TECDOC-1034 (1998) p.131
Summary= modification of potential , NSE 81,49 (1982) , especially at higher
energies See also LA-UR-04-6456. This potential replaces RIPL # 5.
Used in ENDF-B/VII evaluation for n+U-236,U-238,U-240. To be
published in NDS 2007 (Table 1).
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2009 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 92-92 A-Range= 232-240 E-Range= 0-200 MeV
Author(s)= P.G.Young
Reference= LANL Progress Report LA-11972-PR (1990) p.9
Summary= Non-relativistic mod and replacement for RIPL # 2006. Using
Vr*Rr=36.75 and Wd=0.5 at 75 MeV as benchmarks. Mod Wr above 75 MeV
to decrease at 200 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2010 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 92-92 A-Range= 233-233 E-Range= 0-200 MeV
Author(s)= P.G.Young
Reference= LANL Mod of Progress Report LA-11972-PR (1990) p.9
Summary= Same as 2030 except 233U mass,structure. (Young internal number
1033) Same as 22 except couples 7 levels instead of 3. Incorporate
Koning-like Vso and Wso above 10 MeV. Use 5 linear segments to
grossly fit empirical Vr from total data.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2011 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 77-77 A-Range= 191-191 E-Range= 0- 20 MeV
Author(s)= M.B.Chadwick and A.C.Hayes (entered in current format by P.Talou)
Reference= [Ref. R.Macklin and P.G.Young, Nucl.Sci.Eng. 97,239(1987)]
Summary= Based on RIPL #2005, corrected for isospin, and fit to exp. total
x/s.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2012 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 77-77 A-Range= 193-193 E-Range= 0- 20 MeV
Author(s)= M.B.Chadwick and A.C.Hayes (entered in current format by P.Talou)
Reference= [Ref. R.Macklin and P.G.Young, Nucl.Sci.Eng. 97,239(1987)]
Summary= Based on RIPL #2005, corrected for isospin, and fit to exp. total
x/s.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2100 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-83 A-Range= 40-209 E-Range= 10- 26 MeV
Author(s)= R.L.Varner,W.J.Thompson,T.L.McAbee,E.J.Ludwig,T.B.Clegg
Reference= Phys. Rep. 201,57 (1991)
Summary= total x-section and polarization data together with (p,p) and
(n,n) data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2101 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-82 A-Range= 54-208 E-Range= 10- 80 MeV
Author(s)= R.L.Walter and P.P.Guss
Reference= Rad. Effects 95, 73 (1986) [1985 Santa Fe Conf. Proc.]
Summary= A Global Optical Model for Neutron Scattering for A>53, 10 MeV < E
< 80 MeV, based on fits to neutron and proton data. Note: Wd can be
negative at energies near 80 MeV. To avoid negative Wd, run
OMRETRIEVE with negative modtyp.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2300 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 92-92 A-Range= 238-238 E-Range= 0-200 MeV
Author(s)= A.V.Ignatyuk,V.P.Lunev,Yu.N.Shubin,E.V.Gai,N.N.Titarenko,A.Ventura,W
.Gudowski
Reference= Nucl.Sci.Engr. 136, 340 (2000).
Summary= Neutron Cross Section Evaluations for 238U Up to 150 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2301 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 90-90 A-Range= 227-260 E-Range= 0-200 MeV
Author(s)= A.V.Ignatyuk
Reference= Priv.communication to NDS, BROND 2003 evaluations up to 150 MeV for
232 Th
Summary=
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2302 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 90-90 A-Range= 227-260 E-Range= 0-150 MeV
Author(s)= A.V.Ignatyuk et al
Reference= Nucl.Sc.&.Eng.142 (2002) 177-194
Summary= Requires an updated RIPL2 interfase code (R= r0 + r1*E + R2*E*E)
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2303 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 90-92 A-Range= 230-234 E-Range= 0-200 MeV
Author(s)= A.V.Ignatyuk, E.V.Gai, V.P.Lunev, Yu.N.Shubin, N.N.Titarenko
Reference= Progress Report IAEA RC 12571 (Sept. 2004)
Summary=
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2404 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 40-40 A-Range= 90- 90 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.J.van Wijk, J.P.Delaroche
Reference= OECD/NEA Spec. Mtg. Nucleon-Nucleus Opt.Mod.to 200 MeV,Paris (1997)
p.111.
Summary= ECISVIEW: An interactive toolbox for optical model development. A
preliminary nucleon potential from 0-200 MeV is described for 90Zr
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2405 Neutron incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 13-83 A-Range= 27-209 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003) [Global potential].
Summary= A new global neutron optical model potential for incident energies
between 1 keV and 200 MeV and valid for Al through Bi. The
potential is based on detailed fits of neutron total and elastic
cross sections and elastic angular distributions with the ECISVIEW
interactive code.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2406 Neutron incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 74-74 A-Range= 182-186 E-Range= 0- 16 MeV
Author(s)= J.P.Delaroche,G.Haouat,J.Lachkar,Y.Patin,J.Sigaud,J.Chardine
Reference= Phys. Rev. C 23, 136 (1981).
Summary= Deformations, Moments, and Radii of 182,183,184,186W from Fast
Neutron Scattering. Coupled-channels deformed - neutron and proton
potentials via Lane model - valid to 16 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2407 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 27-83 A-Range= 59-209 E-Range= 0-200 MeV
Author(s)= B.Morillon and P.Romain
Reference= Phys. Rev. C70, 014601 (2004); Phys. Rev. C74, 014601 (2006)
Summary= The following modifications are required to the published OMP
parameters: As = -17 + 0.018*A ; Bs = 13 ; Cs = 0.025 ; nonlocality
gamma = 0.1165 - 1e-4*A A dispersive global spherical optical model
potential for neutrons with incident energies between 1 keV and 200
MeV and valid for Co(A=59) up to Bi(A=209).
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2408 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 90-97 A-Range= 228-249 E-Range= 0-200 MeV
Author(s)= R.Capote, E.Soukhovitski, S.Chiba, J.M.Quesada
Reference= J. Nucl. Sc.&Tech. (Japan) 45 (2008) 333-340. Nice ND2007 proceeding
s(pap#765).
Summary= Dispersive coupled channel neutron OMP for incident energies
between 1 keV and 200 MeV for actinides. Local Fermi energy used.
Tested for 31 actinides. Th232; Pa231,232,233; U233,235,238;
Pu239,240,242; Np237; Am241. Approximately Lane consistent (see
PRC76 (2007) 057602).
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2409 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 90-97 A-Range= 228-249 E-Range= 0-200 MeV
Author(s)= R.Capote, E.Soukhovitski, J.M.Quesada, S.Chiba
Reference= Unpublished.
Summary= Lane consistent dispersive CC neutron OMP for incident energies
between 1 keV and 200 MeV for actinides. Local Fermi energy used.
Tested for 31 actinides. (See 5409 for the proton OMP)
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2410 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 13-83 A-Range= 27-209 E-Range= 0-200 MeV
Author(s)= B.Morillon and P.Romain
Reference= Phys. Rev. C76, 044601 (2007)
Summary= A dispersive global spherical optical model potential for neutrons
(and protons) with incident energies between 1 keV and 200 MeV and
valid for Al(A=27) up to Bi(A=209). Taken from the Table 1 for
neutrons (M.R.07a)
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2411 Neutron incident, spherical nucleus model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 13-83 A-Range= 27-209 E-Range= 0-200 MeV
Author(s)= B.Morillon and P.Romain
Reference= Phys. Rev. C76, 044601 (2007)
Summary= A dispersive global spherical optical model potential for neutrons
(and protons) with incident energies between 1 keV and 200 MeV and
valid for Al(A=27) up to Bi(A=209). Taken from the Table 2 for
neutrons (M.R.07b)
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2600 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 90-94 A-Range= 232-242 E-Range= 0-200 MeV
Author(s)= E.Soukhovitski, S. Chiba, J. Lee, O. Iwamoto and T.Fukahori
Reference= J. Phys. G: Nucl. Part. Phys. 30, 905-920 (2004).
Summary= A new global coupled channel neutron OMP for incident energies
between 1 keV and 200 MeV and valid for actinides. Vr: -25.9826 =
-41.45 + 0.06667*232; Wd: 8.48744 = 17.38 - 0.03833*232; Updated
parameters: VR1=0.024; VR2=1.7E-4; Smooth Fermi energy dependence.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2601 Neutron incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 90-94 A-Range= 232-242 E-Range= 0-200 MeV
Author(s)= E.Soukhovitski, S. Chiba, J. Lee, O. Iwamoto and T.Fukahori
Reference= J. Phys. G: Nucl. Part. Phys. 30, 905-920 (2004).
Summary= A new global coupled channel neutron OMP for incident energies
between 1 keV and 200 MeV and valid for actinides. Vr: -25.9826 =
-41.45 + 0.06667*232; Wd: 8.48744 = 17.38 - 0.03833*232; Updated
parameters: VR1=0.024; VR2=1.7E-4; Local Fermi energy used.
Recommended for Th230,232; U233,235,238; Pu239,240,242
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2602 Neutron incident, CC soft rotor model
Potential is relativistic and non-dispersive
Z-Range= 12-50 A-Range= 24-124 E-Range= 0-200 MeV
Author(s)= E.Soukhovitski, S. Chiba and J. Lee
Reference= CP 769, Int.Conf.NDST, Santa Fe, USA, ed.by R.C.Haight et al, AIP 20
05, p. 1100.
Summary= A global coupled channel soft rotor neutron OMP for incident
energies between 1 keV and 200 MeV and valid for A=24-122 nuclei.
Local Fermi energy used. Updated parameters: VR1=0.017; VR2=1.5E-4.
Fitted to Mg24 26,Si28 30,S32,Ar40,Ca40,Ti48,Cr52,Fe54,56,Ni58
62,Zr90 92,Mo92-98 and Sn116 122 data. OPTMAN should be used.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 2700 Neutron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-83 A-Range= 40-210 E-Range= 0-155 MeV
Author(s)= C.A.Engelbrecht and H.Fiedeldey
Reference= Ann. Phys. 42,262-295 (1967)
Summary= Derived from non-local formalism to fit total and nonelastic
x-sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4000 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 25-26 A-Range= 54- 56 E-Range= 0- 28 MeV
Author(s)= E.D.Arthur and P.G.Young
Reference= LA-UR-95-3654 (1995),BNL-NCS-51245 (1980) p.731, LA-8626-MS (1980)
Summary= Parameters developed for proton reactions with nuclides around
Fe-54,Fe-56
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4001 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-27 A-Range= 59- 59 E-Range= 0- 23 MeV
Author(s)= E.D.Arthur,P.G.Young,W.Matthes
Reference= BNL-51245,p.751 (1980); Nucl.Sci.Eng.124,271(1996)
Summary= Parameters to include proton emission competition in neutron
induced cross-sections on Co-59
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4002 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 38-38 A-Range= 88- 89 E-Range= 0- 21 MeV
Author(s)= E.D.Arthur
Reference= Nucl.Sci.Eng. 76,137 (1980)
Summary= Potential developed to analyze proton-induced reaction x-sections
on Sr-88
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4003 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 39-39 A-Range= 89- 89 E-Range= 0- 21 MeV
Author(s)= E.D.Arthur
Reference= Nucl.Sci.Eng. 76,137 (1980)
Summary= potential developed for proton reactions on Y-89 nuclide
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4004 Proton incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 79-79 A-Range= 197-197 E-Range= 0- 57 MeV
Author(s)= P.G.Young and E.D.Arthur.
Reference= LA-UR-84-2767(1984); LA-UR-94-3104(1994).
Summary= Parameterization was developed for ENDF/B-VI to provide n,x gamma
x-section data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4015 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 6- 6 A-Range= 12- 12 E-Range= 0- 65 MeV
Author(s)= M.B.Chadwick and P.G.Young
Reference= Proc.Int. Particle Therapy Mtg. and PTCOG XXIV, 24-26 Apr. 1996,Detr
oit,Mich.
Summary= Proton Nuclear Interactions Up to 250 MeV for Radiation Transport
Sumulations of Particle Therapy. Potential based on experimental
data and previous optical model analyses, especially Arthur and
Dimbylow. See LA-UR-95-3654.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4016 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 7- 7 A-Range= 14- 14 E-Range= 0- 70 MeV
Author(s)= M.B.Chadwick and P.G.Young
Reference= Proc.Int. Particle Therapy Mtg. and PTCOG XXIV, 24-26 Apr. 1996,Detr
oit,Mich.
Summary= Proton Nuclear Interactions Up to 250 MeV for Radiation Transport
Sumulations of Particle Therapy. Potential based on experimental
data and previous optical model analyses, especially Arthur and
Islam. See LA-UR-95-3654.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4017 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 8- 8 A-Range= 16- 16 E-Range= 0- 50 MeV
Author(s)= M.B.Chadwick and P.G.Young
Reference= Proc.Int. Particle Therapy Mtg. and PTCOG XXIV, 24-26 Apr. 1996,Detr
oit,Mich.
Summary= Proton Nuclear Interactions Up to 250 MeV for Radiation Transport
Sumulations of Particle Therapy. Potential based on experimental
data and previous optical model analyses, especially Arthur and
Islam. See LA-UR-95-3654.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4018 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 13-13 A-Range= 27- 27 E-Range= 0- 20 MeV
Author(s)= R.C.Harper and W.L.Alford
Reference= J.Phys.G:Nucl.Phys. 8, 153(1982)
Summary= Experimental and theoretical neutron cross sections at 14 MeV.
Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for
incident neutrons, protons, and alphas.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4019 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 58- 58 E-Range= 0- 20 MeV
Author(s)= R.C.Harper and W.L.Alford
Reference= J.Phys.G:Nucl.Phys. 8, 153(1982)
Summary= Experimental and theoretical neutron cross sections at 14 MeV.
Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for
incident neutrons, protons, and alphas.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4020 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 41-41 A-Range= 93- 93 E-Range= 0- 20 MeV
Author(s)= R.C.Harper and W.L.Alford
Reference= J.Phys.G:Nucl.Phys. 8, 153(1982)
Summary= Experimental and theoretical neutron cross sections at 14 MeV.
Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for
incident neutrons, protons, and alphas.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4100 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 16-49 A-Range= 30-100 E-Range= 0- 22 MeV
Author(s)= F.G.Perey
Reference= Phys. Rev. 131,745 (1963)
Summary= parameters developed to proton reaction data for medium mass
nuclides
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4101 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-83 A-Range= 40-209 E-Range= 10- 50 MeV
Author(s)= F.D.Becchetti Jr. and G.W.Greenlees
Reference= Phys. Rev. 182,1190 (1969)
Summary= diff. elastic and polarization data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4102 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 6-82 A-Range= 12-208 E-Range= 30- 60 MeV
Author(s)= J.J.H.Menet,E.E.Gross,J.J.Malanify, and A.Zucker
Reference= Phys. Rev. C4,1114 (1971)
Summary= parameters developed to provide total , elastic and inelastic data.
Derived over 30-60 MeV energy range
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4108 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-82 A-Range= 48-208 E-Range= 25- 45 MeV
Author(s)= D.M.Patterson et al
Reference= Nucl. Phys. A263,261 (1976)
Summary= global potential -energy and a dependent 25 to 45 MeV,A=48-208
(p,n)reactions (Following paper E = Ep - 0.84 Z/A**1/3 for the real
potential !)
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4109 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 39-39 A-Range= 89- 89 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4110 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 41-41 A-Range= 93- 93 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4111 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 45-45 A-Range= 103-103 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4112 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 46-46 A-Range= 105-105 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4113 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 47-47 A-Range= 107-107 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4114 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 47-47 A-Range= 109-109 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4115 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 48-48 A-Range= 110-110 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4116 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 48-48 A-Range= 111-111 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4117 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 48-48 A-Range= 113-113 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4118 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 48-48 A-Range= 114-114 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4119 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 49-49 A-Range= 115-115 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4120 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 50-50 A-Range= 116-116 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4121 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 50-50 A-Range= 122-122 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4122 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 50-50 A-Range= 124-124 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4123 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 52-52 A-Range= 128-128 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4124 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 52-52 A-Range= 130-130 E-Range= 1- 7 MeV
Author(s)= C.H.Johnson et al
Reference= Phys. Rev. Lett.39,1604(1977); Phys. Rev. C20,2052(1979)
Summary= proton optical potential below 7 MeV,A=89-130 (p,n) reactions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4125 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 40-40 A-Range= 92- 92 E-Range= 2- 7 MeV
Author(s)= D.S.Flynn et al
Reference= Phys. Rev. C. 31, 87 (1985)
Summary= proton optical potential below 7 MeV,A=92- 100 (p,p) and (p,n)
excitation functions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4126 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 40-40 A-Range= 94- 94 E-Range= 2- 7 MeV
Author(s)= D.S.Flynn et al
Reference= Phys. Rev. C. 31, 87 (1985)
Summary= proton optical potential below 7 MeV,A=92- 100 (p,p) and (p,n)
excitation functions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4127 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 40-40 A-Range= 96- 96 E-Range= 2- 7 MeV
Author(s)= D.S.Flynn et al
Reference= Phys. Rev. C. 31, 87 (1985)
Summary= proton optical potential below 7 MeV,A=92- 100 (p,p) and (p,n)
excitation functions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4128 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 42-42 A-Range= 95- 95 E-Range= 2- 7 MeV
Author(s)= D.S.Flynn et al
Reference= Phys. Rev. C. 31, 87 (1985)
Summary= proton optical potential below 7 MeV,A=92- 100 (p,p) and (p,n)
excitation functions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4129 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 42-42 A-Range= 98- 98 E-Range= 2- 7 MeV
Author(s)= D.S.Flynn et al
Reference= Phys. Rev. C. 31, 87 (1985)
Summary= proton optical potential below 7 MeV,A=92- 100 (p,p) and (p,n)
excitation functions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4130 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 42-42 A-Range= 100-100 E-Range= 2- 7 MeV
Author(s)= D.S.Flynn et al
Reference= Phys. Rev. C. 31, 87 (1985)
Summary= proton optical potential below 7 MeV,A=92- 100 (p,p) and (p,n)
excitation functions
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4131 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 12-82 A-Range= 24-208 E-Range= 80-180 MeV
Author(s)= P.Schwandt, H.O.Meyer, W.W.Jacobs, A.D.Bacher, S.E.Vigdor, M.D.Kaitc
huck et al.
Reference= Phys. Rev. C. 26, 55 (1982)
Summary= Analyzing power of proton-nucleus elastic scattering between 80 and
180 MeV. Based on systematic analysis of elastic scattering of
polarized protons between 80-180 MeV for a number of target nuclei.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4300 Proton incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 92-92 A-Range= 238-238 E-Range= 0-200 MeV
Author(s)= A.V.Ignatyuk,V.P.Lunev,Yu.N.Shubin,E.V.Gai,N.N.Titarenko,A.Ventura,W
.Gudowski
Reference= Nucl.Sci.Eng. 136, 340 (2000).
Summary= Neutron Cross Section Evaluations for 238U Up to 150 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4301 Proton incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 90-90 A-Range= 227-260 E-Range= 0-200 MeV
Author(s)= A.V.Ignatyuk
Reference= Priv.communication to NDS, BROND 2003 evaluations up to 150 MeV for
232 Th
Summary=
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4302 Proton incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 90-90 A-Range= 227-260 E-Range= 0-150 MeV
Author(s)= A.V.Ignatyuk et al
Reference= Nucl.Sc.&.Eng.142 (2002) 177-194
Summary= Requires an updated RIPL2 interfase code (R= r0 + r1*E + R2*E*E)
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4303 Proton incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 90-92 A-Range= 228-234 E-Range= 0-200 MeV
Author(s)= A.V.Ignatyuk, E.V.Gai, V.P.Lunev, Yu.N.Shubin, N.N.Titarenko
Reference= Progress Report IAEA RC 12571 (Sept. 2004)
Summary=
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4416 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 13-13 A-Range= 27- 27 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 5405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4417 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 14-14 A-Range= 28- 28 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 5405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4418 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 20-20 A-Range= 40- 40 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 5405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4419 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 26-26 A-Range= 54- 54 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 5405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4420 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 26-26 A-Range= 56- 56 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 5405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4421 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 28-28 A-Range= 58- 58 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 5405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4422 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 28-28 A-Range= 60- 60 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 5405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4423 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 28-28 A-Range= 62- 62 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 5405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4424 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 29-29 A-Range= 63- 63 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 5405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4425 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 28-28 A-Range= 64- 64 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 5405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4426 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 40-40 A-Range= 90- 90 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 5405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4427 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 50-50 A-Range= 120-120 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 5405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4428 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 82-82 A-Range= 208-208 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 5405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4429 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 83-83 A-Range= 209-209 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003).
Summary= Local and Global Nucleon Optical Models from 1 keV to 200 MeV.
Based on detailed fits of neutron total and nucleon elastic cross
sections and angular distributions with the ECISVIEW interactive
code. See ref # 5405 for a global potential with same methodology.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4430 Proton incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 45-45 A-Range= 100-104 E-Range= 0-200 MeV
Author(s)= L.C.Mihailescu,I.Sirakov,R.Capote,E.Soukhovitski, et al.
Reference= Proc.Int.Conf. on NDST, ND2007, Nice, France, #617, DOI: 10.1051/nda
ta:07617
Summary= Geometry is different for Vhf and Wv. Dispersive coupled channel
proton OMP for incident energies between 1 keV and 200 MeV for
Rh-103 (based on 1479). pot(1,1,9) = Ccoul/1.73*rc = 0.63208;
rc=1.0935 Ccoul = 1.0 ac=0.36 Local Fermi energy used. Recommended
for Rh-100 - 104
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4431 Proton incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 74-74 A-Range= 178-183 E-Range= 0-200 MeV
Author(s)= R.Capote, E.Soukhovitski, J.M. Quesada, S. Chiba
Reference= Unpublished.
Summary= A dispersive coupled channel proton OMP for incident energies
between 1 keV and 200 MeV valid for W-182,183. (proton potential
for 1480) pot(1,1,9) = Ccoul/1.73*rc = 1.22763; rc=1.0619 Ccoul =
2.0 ac=0.64 Local Fermi energy used. Recommended for W-178,W-183
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4432 Proton incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 73-73 A-Range= 178-186 E-Range= 0-200 MeV
Author(s)= R.Capote, E.Soukhovitski, J.M. Quesada, S. Chiba
Reference= Unpublished.
Summary= A dispersive coupled channel proton OMP for incident energies
between 1 keV and 200 MeV valid for tantalum pot(1,1,9) =
Ccoul/1.73*rc = 1.22763; rc=1.0619 Ccoul = 2.0 ac=0.64 Local Fermi
energy used. Used in IAEA tungsten evaluation (proton emission).
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4433 Proton incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 79-79 A-Range= 195-200 E-Range= 0-200 MeV
Author(s)= E.Soukhovitskii and R.Capote
Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper)
Summary= Lane-consistent dispersive CC proton OMP for incident energies
between 1 keV and 200 MeV for gold. Local Fermi energy used. See
1483 for neutron OMP. Geometry is different for Vhf and Wv. Ep = Ep
- 0.92999 Z/A**1/3 See RIPL paper, Table 6.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4434 Proton incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 25-25 A-Range= 50- 56 E-Range= 0-200 MeV
Author(s)= E.Soukhovitskii and R.Capote
Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper)
Summary= Lane-consistent dispersive CC proton OMP for incident energies
between 1 keV and 200 MeV for Mn-55. Local Fermi energy used. See
1484 for neutron OMP. Geometry is different for Vhf and Wv. Ep = Ep
- 1.1 Z/A**1/3. See RIPL paper, Table 6.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4435 Proton incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 45-45 A-Range= 100-104 E-Range= 0-200 MeV
Author(s)= E.Soukhovitskii and R.Capote
Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper)
Summary= Lane-consistent dispersive coupled channel proton OMP for incident
energies between 1 keV and 200 MeV. Recommended for Rh-100 - 104.
Local Fermi energy used. See 1485 for neutron OMP. Ep = Ep -
1.10000 Z/A**1/3 See RIPL paper, Table 6.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4601 Proton incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 92-92 A-Range= 238-238 E-Range= 0-200 MeV
Author(s)= V.M.Maslov, Yu.V.Porodzinskij, N.A.Tetereva, M.Baba, A.Hasegawa
Reference= Nucl. Phys. A736, 77-92 (2004)
Summary= Rigid rotor OMP valid for incident energies from 1 kev to 200 MeV.
Best description of the total cross section data for U238 Wd:
10.915 = 9.315 + 0.08*20 ; Wv50: 3.75 = 5 - 0.025*50; Wv80: 4.15 =
5.75 - 0.02*80;
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4602 Proton incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 92-92 A-Range= 238-238 E-Range= 0-200 MeV
Author(s)= V.M.Maslov, Yu.V.Porodzinskij, N.A.Tetereva, M.Baba, A.Hasegawa
Reference= Nucl. Phys. A736, 77-92 (2004)
Summary= Rigid rotor OMP valid for incident energies from 1 kev to 200 MeV.
Best description of the fission cross section data for U238 Wd14:
10.123 = 8.443 + 0.12*14 ; Wd50: 12.443 = 8.443 + 0.08*50; Wv14:
-1.12=-14*0.08; Wv50: -2.12=2.88 - 0.1*50; Wv80: 4.28=5.88 -
0.02*80;
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4603 Proton incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 90-92 A-Range= 230-234 E-Range= 0-200 MeV
Author(s)= V.M.Maslov
Reference= Private communication to NDS (Updated on Dec.22,2004)
Summary= Best description of the total cross section data for Th232 rc taken
according to Koning recommendations
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4604 Proton incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 90-92 A-Range= 230-234 E-Range= 0-200 MeV
Author(s)= V.M.Maslov
Reference= Private communication to NDS (Updated on Dec.22, 2004)
Summary= Best description of the fission cross section data for Th232 rc
taken according to Koning recommendations
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4605 Proton incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 90-92 A-Range= 228-234 E-Range= 0-200 MeV
Author(s)= E.Soukhovitski, R. Capote, J.M.Quesada, S.Chiba
Reference= Unpublished.
Summary= A dispersive coupled channel proton OMP for incident energies
between 1 keV and 200 MeV valid for Th. pot(1,1,9) = Ccoul/1.73*rc
= 0.935699; rc=1.2452 Ccoul = 1.3 ac=0.542 Local Fermi energy used.
Recommended for Th232,U233
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4606 Proton incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 92-92 A-Range= 236-240 E-Range= 0-200 MeV
Author(s)= E.Soukhovitski, R. Capote, J.M. Quesada, S. Chiba
Reference= Unpublished.
Summary= A dispersive coupled channel proton OMP for incident energies
between 1 keV and 200 MeV valid for U238. pot(1,1,9) =
Ccoul/1.73*rc = 0.935699; rc=1.2452 Ccoul = 1.3 acoul=0.542 Local
Fermi energy used. Recommended for U238.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4607 Proton incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 92-92 A-Range= 232-234 E-Range= 0-200 MeV
Author(s)= E.Soukhovitski, R. Capote, J.M. Quesada, S. Chiba
Reference= Unpublished.
Summary= A dispersive coupled channel proton OMP for incident energies
between 1 keV and 200 MeV valid for U-233. pot(1,1,9) =
Ccoul/1.73*rc = 0.935699; rc=1.2452 Ccoul = 1.3 acoul=0.542 Local
Fermi energy used. Recommended for U233
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4608 Proton incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 90-91 A-Range= 228-234 E-Range= 0-200 MeV
Author(s)= E.Soukhovitski, R. Capote, J.M. Quesada, S. Chiba
Reference= Phys.Rev.C72 (2005) 024604
Summary= A dispersive coupled channel proton OMP for incident energies
between 1 keV and 200 MeV valid for Th, fitted to the new average
cross section derived by Geel g roup from 1-150 keV. Local Fermi
energy used. Recommended for Th232,Pa231,233. pot(1,1,9) =
Ccoul/1.73*rc = 0.935699; rc=1.2452 Ccoul = 1.3 acoul = 0.545
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4609 Proton incident, CC soft rotor model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 40-40 A-Range= 90- 92 E-Range= 0-200 MeV
Author(s)= E.Soukhovitskii and R. Capote
Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper)
Summary= Lane-consistent dispersive CC proton OMP for incident energies
between 1 keV and 200 MeV for Zr isotopes. Recommended for
Zr-90,92,94,96. Local Fermi energy used. See 4609 for proton OMP.
Soft rotor. See RIPL paper, Table 6. Following paper E = Ep - 1.1 *
Z/A**1/3. See 609 for neutron potential.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4610 Proton incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 72-74 A-Range= 174-186 E-Range= 0-200 MeV
Author(s)= E.Soukhovitskii and R. Capote
Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper)
Summary= Lane consistent dispersive CC proton OMP for incident energies
between 1 keV and 200 MeV for Hf-W-Ta isotope. Recommended for
Hf-178,180, Ta-181, all W. Local Fermi energy used. See 610 for
neutron OMP. Soft rotor. OPTMAN should be used. Ep = Ep - 1.33
Z/A**1/3, rc=1.0626, ac=0.64.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4650 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 21-21 A-Range= 45- 45 E-Range= 3- 5 MeV
Author(s)= S.Kailas et al
Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986)
Summary= proton optical potential below 5 MeV for medium-weight nuclei
A=45-80
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4651 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-20 A-Range= 48- 48 E-Range= 3- 5 MeV
Author(s)= S.Kailas et al
Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986)
Summary= proton optical potential below 5 MeV for medium-weight nuclei
A=45-80
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4652 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 23-23 A-Range= 51- 51 E-Range= 3- 5 MeV
Author(s)= S.Kailas et al
Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986)
Summary= proton optical potential below 5 MeV for medium-weight nuclei
A=45-80
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4653 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 24-24 A-Range= 54- 54 E-Range= 3- 5 MeV
Author(s)= S.Kailas et al
Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986)
Summary= proton optical potential below 5 MeV for medium-weight nuclei
A=45-80
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4654 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 27-27 A-Range= 59- 59 E-Range= 3- 5 MeV
Author(s)= S.Kailas et al
Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986)
Summary= proton optical potential below 5 MeV for medium-weight nuclei
A=45-80
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4655 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 61- 61 E-Range= 3- 5 MeV
Author(s)= S.Kailas et al
Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986)
Summary= proton optical potential below 5 MeV for medium-weight nuclei
A=45-80
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4656 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 29-29 A-Range= 65- 65 E-Range= 3- 5 MeV
Author(s)= S.Kailas et al
Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986)
Summary= proton optical potential below 5 MeV for medium-weight nuclei
A=45-80
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4657 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 31-31 A-Range= 71- 71 E-Range= 3- 5 MeV
Author(s)= S.Kailas et al
Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986)
Summary= proton optical potential below 5 MeV for medium-weight nuclei
A=45-80
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4658 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 33-33 A-Range= 75- 75 E-Range= 3- 5 MeV
Author(s)= S.Kailas et al
Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986)
Summary= proton optical potential below 5 MeV for medium-weight nuclei
A=45-80
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4659 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 34-34 A-Range= 80- 80 E-Range= 3- 5 MeV
Author(s)= S.Kailas et al
Reference= Phys. Rev. C 20, 1272(1979); Pramana.J.Phys.27, 139(1986)
Summary= proton optical potential below 5 MeV for medium-weight nuclei
A=45-80
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4660 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 19-19 A-Range= 41- 41 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4661 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 21-21 A-Range= 45- 45 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4662 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-20 A-Range= 48- 48 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4663 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 22-22 A-Range= 49- 49 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4664 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 23-23 A-Range= 51- 51 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4665 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 25-25 A-Range= 55- 55 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4666 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 27-27 A-Range= 59- 59 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4667 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 61- 61 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4668 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 29-29 A-Range= 65- 65 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4669 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 30-30 A-Range= 68- 68 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4670 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 31-31 A-Range= 71- 71 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4671 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 33-33 A-Range= 75- 75 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4672 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 34-34 A-Range= 80- 80 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4673 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 39-39 A-Range= 89- 89 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4674 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 41-41 A-Range= 93- 93 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4675 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 42-42 A-Range= 96- 96 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4676 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 42-42 A-Range= 98- 98 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4677 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 45-45 A-Range= 103-103 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4678 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 46-46 A-Range= 105-105 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4679 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 47-47 A-Range= 107-107 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4680 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 47-47 A-Range= 109-109 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4681 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 48-48 A-Range= 110-110 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4682 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 49-49 A-Range= 115-115 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4683 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 50-50 A-Range= 120-120 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4684 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 50-50 A-Range= 124-124 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4685 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 52-52 A-Range= 128-128 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 4686 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 52-52 A-Range= 130-130 E-Range= 1- 7 MeV
Author(s)= Y.P.Viyogi
Reference= Ph.D Thesis (Calcutta University 1983)
Summary= proton optical potential below 7 MeV for nuclei A=40-130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5001 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 6-82 A-Range= 12-208 E-Range= 50-400 MeV
Author(s)= D.G.Madland
Reference= OECD/NEA Spec. Mtg. Nucleon-Nucleus Opt.Mod.to 200 MeV,Paris (1997)
p.129.
Summary= Update of Semmering potential [NEANDC-245 U (1988)] to include
generalized imag. diff. parameter. Global pot for incid. neuts and
prots. Requires OM code with relativistic kine. & total pot must be
multiplied by 1 + E/(E+2*mc**2) where E,m are for incident particle
and E = total cm kinetic energy. Checked by author.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5002 Proton incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 74-74 A-Range= 182-186 E-Range= 0-100 MeV
Author(s)= P.G.Young,E.D.Arthur,M.Bozian,T.R.England,G.M.Hale,R.J.LaBauve,R.C.L
ittle,et al.
Reference= LANL Report LA-11753-MS (1990); see also LA-8630-PR,p2 (1980)
Summary= parameters are based on neutron elastic ,inelastic,total and
differential data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5003 Proton incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 67-69 A-Range= 165-169 E-Range= 0-100 MeV
Author(s)= E.D.Arthur and C.Philis
Reference= Report LA-8630-PR,p2 (1980)
Summary= Parameters are based on fits to 169Tm low-energy resonance data and
total cross sections, plus fits to 11-MeV neutron scattering on
165Ho. Lane model used to relate n and p potentials.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5004 Proton incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 63-63 A-Range= 151-153 E-Range= 0- 20 MeV
Author(s)= R.Macklin and P.G.Young
Reference= Nucl.Sci.Eng. 95,189(1987)
Summary= parameterization was developed to provide radiative capture
x-sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5005 Proton incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 75-75 A-Range= 185-187 E-Range= 0- 20 MeV
Author(s)= R.Macklin and P.G.Young
Reference= Nucl.Sci.Eng. 97,239(1987)
Summary= parameterization was developed to provide radiative capture cross
sections
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5006 Proton incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 92-92 A-Range= 238-238 E-Range= 0-200 MeV
Author(s)= P.G.Young
Reference= LANL Progress Report LA-11972-PR (1990) p.9
Summary= Modification of potential by Haouat, Lachkar, Lagrange, et al., NSE
81 (1982) 49. Extension above 20 MeV is based on total cross
section data from WNR. Reaction cross section is too high by almost
20% at 200 MeV - modification needed above 20 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5100 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-83 A-Range= 40-209 E-Range= 16- 65 MeV
Author(s)= R.L.Varner,W.J.Thompson,T.L.McAbee,E.J.Ludwig,T.B.Clegg
Reference= Phys. Rep. 201,57 (1991)
Summary= Total x-section and polarization data, together with (p,p) and
(n,n) data, were fit
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5101 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-82 A-Range= 54-208 E-Range= 10- 80 MeV
Author(s)= R.L.Walter and P.P.Guss
Reference= Rad. Effects 95, 73 (1986) [1985 Santa Fe Conf. Proc.]
Summary= A Global Optical Model for Neutron Scattering for A>53, 10 MeV < E
< 80 MeV, based on fits to neutron and proton data.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5404 Proton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 40-40 A-Range= 90- 90 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.J.van Wijk, J.P.Delaroche
Reference= OECD/NEA Spec. Mtg. Nucleon-Nucleus Opt.Mod.to 200 MeV,Paris (1997)
p.111.
Summary= ECISVIEW: An interactive toolbox for optical model development. A
preliminary nucleon potential from 0-200 MeV is described for 90Zr
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5405 Proton incident, spherical nucleus model
Potential is relativistic and non-dispersive
Z-Range= 13-83 A-Range= 27-209 E-Range= 0-200 MeV
Author(s)= A.J.Koning, J.P.Delaroche
Reference= Nucl. Phys. A713, 231 (2003) [Global potential].
Summary= A new global proton optical model potential for incident energies
between 1 keV and 200 MeV and valid for Al through Bi. The
potential is based on detailed fits of proton elastic cross
sections and elastic angular distributions with the ECISVIEW
interactive code.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5406 Proton incident, CC rigid rotor deformed model
Potential is non-relativistic and non-dispersive
Z-Range= 74-74 A-Range= 182-186 E-Range= 0- 16 MeV
Author(s)= J.P.Delaroche,G.Haouat,J.Lachkar,Y.Patin,J.Sigaud,J.Chardine
Reference= Phys. Rev. C 23, 136 (1981).
Summary= Deformations, Moments, and Radii of 182,183,184,186W from Fast
Neutron Scattering. Coupled-channels deformed - neutron and proton
potentials via Lane model - valid to 16 MeV.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5408 Proton incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 90-97 A-Range= 228-249 E-Range= 0-200 MeV
Author(s)= R.Capote, E.Soukhovitski, S. Chiba, J.M.Quesada
Reference= J. Nucl. Sc.&Tech. (Japan) 45 (2008) 333-340. Nice ND2007 proceeding
s(pap#765).
Summary= Dispersive coupled channel proton OMP for incident energies between
1 keV and 200 MeV for actinides. Local Fermi energy used. Tested
for 31 actinides. Th232; Pa231,232,233; U233,235,238;
Pu239,240,242; Np237; Am241. pot(1,1,9) = Ccoul/1.73*rc = 1.13999;
rc=1.2174 Ccoul = 1.62 acoul = 0.551
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5409 Proton incident, CC rigid rotor deformed model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 90-97 A-Range= 228-249 E-Range= 0-200 MeV
Author(s)= R.Capote, E.Soukhovitski, J.M.Quesada, S.Chiba
Reference= Unpublished.
Summary= Lane consistent dispersive CC proton OMP for incident energies
between 1 keV and 200 MeV for actinides. Local Fermi energy used.
Tested for 31 actinides. Ccoul = 1.10, acoul = 0.40. Following
paper E = Ep - Ccoul * Z/A**1/3. See 2409 for neutron potential.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5410 Proton incident, spherical nucleus model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 13-83 A-Range= 27-209 E-Range= 0-200 MeV
Author(s)= B.Morillon and P.Romain
Reference= Phys. Rev. C76, 044601 (2007)
Summary= A dispersive global spherical optical model potential for neutrons
(and protons) with incident energies between 1 keV and 200 MeV and
valid for Al(A=27) up to Bi(A=209). Taken from the Table 1 for
protons (M.R.07a). Coulomb correction is constant and equal to
1.15Z/RC with RC=rc*A^(1/3). pot(1,1,9)=1.15/1.73=0.66474
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5411 Proton incident, spherical nucleus model
Potential is relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 13-83 A-Range= 27-209 E-Range= 0-200 MeV
Author(s)= B.Morillon and P.Romain
Reference= Phys. Rev. C76, 044601 (2007)
Summary= A dispersive global spherical optical model potential for neutrons
(and protons) with incident energies between 1 keV and 200 MeV and
valid for Al(A=27) up to Bi(A=209). Taken from the Table 2 for
protons (M.R.07b) + Table 1. Coulomb correction is constant and
equal to 1.15Z/RC with RC=rc*A^(1/3).
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5501 Proton incident, spherical nucleus model
Potential is non-relativistic and dispersive+SO(Anal.Integr.)
Z-Range= 12-94 A-Range= 24-240 E-Range= 0-200 MeV
Author(s)= Xiaohua Li, Chonghai Cai
Reference= Nucl. Phys. A801, 43-67 (2008).
Summary= A global dispersive spherical proton OMP for incident energies
between 1 keV and 200 MeV. Local Fermi energy dependence.
Non-relativistic OMP. Published potential reffited due to errata in
OMP definition. Parameter set corresponding to the LAB energies
(priv. comm. by authors)
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5600 Proton incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 90-94 A-Range= 232-242 E-Range= 0-200 MeV
Author(s)= E.Soukhovitski, S. Chiba, J. Lee, O. Iwamoto and T.Fukahori
Reference= J. Phys. G: Nucl. Part. Phys. 30, 905-920 (2004).
Summary= A new global coupled channel proton OMP for incident energies
between 1 keV and 200 MeV and valid for actinides. Vr: -25.9826 =
-41.45 + 0.06667*232; Ccoul=1; pot(1,1,9)=Ccoul/1.73*rc=0.730809;
Wd: 8.48744=17.38-0.03833*232; ac=0.343 Updated parameters:
VR1=0.024; VR2=1.7E-4; Smooth Fermi energy dependence.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5601 Proton incident, CC rigid rotor deformed model
Potential is relativistic and non-dispersive
Z-Range= 90-94 A-Range= 232-242 E-Range= 0-200 MeV
Author(s)= E.Soukhovitski, S. Chiba, J. Lee, O. Iwamoto and T.Fukahori
Reference= J. Phys. G: Nucl. Part. Phys. 30, 905-920 (2004).
Summary= A new global coupled channel proton OMP for incident energies
between 1 keV and 200 MeV and valid for actinides. Vr: -25.9826 =
-41.45 + 0.06667*232; Ccoul=1; pot(1,1,9)=Ccoul/1.73*rc=0.730809;
Wd: 8.48744=17.38-0.03833*232; ac=0.343 Updated parameters:
VR1=0.024; VR2=1.7E-4; Local Fermi energy dependence.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 5602 Proton incident, CC soft rotor model
Potential is relativistic and non-dispersive
Z-Range= 12-50 A-Range= 24-124 E-Range= 0-200 MeV
Author(s)= E.Soukhovitski, S. Chiba and J. Lee
Reference= CP 769, Int.Conf.NDST, Santa Fe, USA, ed.by R.C.Haight et al, AIP 20
05, p. 1100.
Summary= A global coupled channel soft rotor proton OMP for incident
energies between 1 keV and 200 MeV and valid for A=24-122 nuclei.
Local Ef used. Updated parameters: VR1=0.017; VR2=1.5E-4. Fitted to
Mg24 26,Si28 30,S32,Ar40,Ca40,Ti48,Cr52,Fe54,56,Ni58 62,Zr90
92,Mo92-98 and Sn116 122 data.pot(1,1,9)=Ccoul*0.832*rc=0.944431
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 6100 Deuteron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-83 A-Range= 40-209 E-Range= 8- 13 MeV
Author(s)= J.M.Lohr and W.Haeberli
Reference= Nucl. Phys. A232,381(1974)
Summary= Parameters developed to provide data for differential ela and
inelastic data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 6101 Deuteron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-82 A-Range= 40-208 E-Range= 11- 27 MeV
Author(s)= C.M.Perey and F.G.Perey
Reference= Phys. Rev. 132,755 (1963)
Summary= diff. elastic x-section data and other measured data analysis
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 6112 Deuteron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-20 A-Range= 40- 40 E-Range= 11- 90 MeV
Author(s)= W.W.Daehnick, J.D.Childs, and Z.Vrcelj.
Reference= Phys.Rev.C21,2253(1980).
Summary= Global optical model potential for elastic deuteron scattering from
12 to 90 MeV. Fit 4000 data points - 50 reaction x/s, 13 vect pol
a/d, 103 elas scat a/d. This potential is a fit by Kailas to Wv,
Wd, and a imaginary terms in order to get into RIPL2 format.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 6113 Deuteron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 58- 58 E-Range= 11- 90 MeV
Author(s)= W.W.Daehnick, J.D.Childs, and Z.Vrcelj.
Reference= Phys.Rev.C21,2253(1980).
Summary= Global optical model potential for elastic deuteron scattering from
12 to 90 MeV. Fit 4000 data points - 50 reaction x/s, 13 vect pol
a/d, 103 elas scat a/d. This potential is a fit by Kailas to Wv,
Wd, and a imaginary terms in order to get into RIPL2 format.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 6114 Deuteron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 40-40 A-Range= 90- 90 E-Range= 11- 90 MeV
Author(s)= W.W.Daehnick, J.D.Childs, and Z.Vrcelj.
Reference= Phys.Rev.C21,2253(1980).
Summary= Global optical model potential for elastic deuteron scattering from
12 to 90 MeV. Fit 4000 data points - 50 reaction x/s, 13 vect pol
a/d, 103 elas scat a/d. This potential is a fit by Kailas to Wv,
Wd, and a imaginary terms in order to get into RIPL2 format.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 6115 Deuteron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 50-50 A-Range= 120-120 E-Range= 11- 90 MeV
Author(s)= W.W.Daehnick, J.D.Childs, and Z.Vrcelj.
Reference= Phys.Rev.C21,2253(1980).
Summary= Global optical model potential for elastic deuteron scattering from
12 to 90 MeV. Fit 4000 data points - 50 reaction x/s, 13 vect pol
a/d, 103 elas scat a/d. This potential is a fit by Kailas to Wv,
Wd, and a imaginary terms in order to get into RIPL2 format.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 6116 Deuteron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 82-82 A-Range= 208-208 E-Range= 11- 90 MeV
Author(s)= W.W.Daehnick, J.D.Childs, and Z.Vrcelj.
Reference= Phys.Rev.C21,2253(1980).
Summary= Global optical model potential for elastic deuteron scattering from
12 to 90 MeV. Fit 4000 data points - 50 reaction x/s, 13 vect pol
a/d, 103 elas scat a/d. This potential is a fit by Kailas to Wv,
Wd, and a imaginary terms in order to get into RIPL2 format.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 6200 Deuteron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 6-92 A-Range= 12-238 E-Range= 1-200 MeV
Author(s)= Haixia An and Chonghai Cai.
Reference= Phys. Rev. C73, 054605 (2006)
Summary= Elastic deuteron scattering and deuteron reaction cross sections
for energies up to 183 MeV. Vc=0.642/0.4=1.605
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 6201 Deuteron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 6-83 A-Range= 12-209 E-Range= 1-200 MeV
Author(s)= Yinlu Han, Yuyang Shi, Qingbiao Shen.
Reference= Phys.Rev.C74, 044615 (2006)
Summary= Elastic deuteron scattering and deuteron reaction cross sections
for energies up to 200 MeV. Vc=1.0584/0.4=2.646
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 6202 Deuteron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 3- 3 A-Range= 6- 7 E-Range= 1-200 MeV
Author(s)= Yinlu Han, Yuyang Shi, Qingbiao Shen.
Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper)
Summary= Elastic deuteron scattering and deuteron reaction cross sections
for energies up to 200 MeV on Lithium. Local potential.
Vc=0.7593/0.4=1.89825. See theory in Phys. Rev. C74 044615 (2006)
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 6203 Deuteron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 4- 4 A-Range= 8- 10 E-Range= 1-200 MeV
Author(s)= Yinlu Han, Yuyang Shi, Qingbiao Shen.
Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper)
Summary= Elastic deuteron scattering and deuteron reaction cross sections
for energies up to 200 MeV on Be-9. Local potential.
Vc=1.7719/0.4=4.42975. See theory in Phys. Rev. C74 044615 (2006)
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 6204 Deuteron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 6- 6 A-Range= 11- 13 E-Range= 1-200 MeV
Author(s)= Yinlu Han, Yuyang Shi, Qingbiao Shen.
Reference= Nucl. Data Sheets 110 (2009) 3107-3214 (RIPL paper)
Summary= Elastic deuteron scattering and deuteron reaction cross sections
for energies up to 200 MeV on C-12. Local potential.
Vc=1.4140/0.4=3.535. See theory in Phys. Rev. C74 044615 (2006)
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 6400 Deuteron incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 6-82 A-Range= 12-208 E-Range= 20-100 MeV
Author(s)= J.Bojowald et al
Reference= Phys. Rev. C 38,1153(1988)
Summary= Elastic deuteron scattering for energies up to 100 MeV
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 7100 Triton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-82 A-Range= 40-208 E-Range= 1- 40 MeV
Author(s)= F.D.Becchetti Jr. and G.W.Greenlees
Reference= Ann. Rept. J.H.Williams Lab., Univ. Minnesota (1969)
Summary= Parameterization developed to analyze measured data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 7200 Triton incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 13-90 A-Range= 27-232 E-Range= 1- 40 MeV
Author(s)= Xiaohua Li, Chuntian Liang, Chonghai Cai.
Reference= Nucl.Phys.A789, 103-113(2007)
Summary= Elastic triton scattering for Al-27, F-19 and Ca-Th nuclei up to 40
MeV. Vc=1.0474/0.4=2.6185
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 8100 He-3 incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-82 A-Range= 40-208 E-Range= 1- 40 MeV
Author(s)= F.D.Becchetti Jr. and G.W.Greenlees
Reference= Ann. Rept. J.H.Williams Lab., Univ. Minnesota (1969)
Summary= Parameters developed to analyze measured data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 8101 He-3 incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-20 A-Range= 40- 40 E-Range= 21- 84 MeV
Author(s)= H.H.Chang et al
Reference= Nucl. Phys. A297,105 (1978)
Summary= Helium-3 on 40Ca and 58Ni energies 27.7,51.4,73.2,83.5 MeV
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 8102 He-3 incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 58- 58 E-Range= 22- 84 MeV
Author(s)= H.H.Chang et al
Reference= Nucl. Phys. A297,105 (1978)
Summary= Helium-3 on 40Ca and 58Ni energies 27.7,51.4,73.2,83.5 MeV
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9000 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 13-26 A-Range= 27- 56 E-Range= 1-100 MeV
Author(s)= E.D.Arthur and P.G.Young
Reference= Report LA-8636-MS(ENDF-304) (1980)
Summary= potential developed to analyze alpha reaction data for medium
nuclides
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9001 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 27-27 A-Range= 59- 59 E-Range= 1-100 MeV
Author(s)= E.D.Arthur,P.G.Young,W.Matthes
Reference= Report BNL-51245,751(1980)
Summary= potential developed for alpha reaction data for co-59 and other
nuclides in the vicinity
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9018 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 13-13 A-Range= 27- 27 E-Range= 0- 20 MeV
Author(s)= R.C.Harper and W.L.Alford
Reference= J.Phys.G:Nucl.Phys. 8, 153(1982)
Summary= Experimental and theoretical neutron cross sections at 14 MeV.
Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for
incident neutrons, protons, and alphas.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9019 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 58- 58 E-Range= 0- 20 MeV
Author(s)= R.C.Harper and W.L.Alford
Reference= J.Phys.G:Nucl.Phys. 8, 153(1982)
Summary= Experimental and theoretical neutron cross sections at 14 MeV.
Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for
incident neutrons, protons, and alphas.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9020 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 41-41 A-Range= 93- 93 E-Range= 0- 20 MeV
Author(s)= R.C.Harper and W.L.Alford
Reference= J.Phys.G:Nucl.Phys. 8, 153(1982)
Summary= Experimental and theoretical neutron cross sections at 14 MeV.
Optical potentials given for 27Al, 58Ni, 93Nb, and 197Au for
incident neutrons, protons, and alphas.
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9100 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 8-82 A-Range= 16-208 E-Range= 1- 25 MeV
Author(s)= L.McFadden and G.R.Satchler
Reference= Nucl. Phys. 84, 177 (1966)
Summary= parameters developed to analyze elastic scattering data for several
nuclides
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9101 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 10-92 A-Range= 20-235 E-Range= 1- 46 MeV
Author(s)= J.R.Huizenga and G.Igo
Reference= Nucl. Phys. 29,462 (1962)
Summary= total x-section and transmission coefficient calculations for
several nuclides used to determine potential
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9400 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 20-45 A-Range= 40-100 E-Range= 1- 30 MeV
Author(s)= B.Strohmaier et al
Reference= IAEA Advisory Group Meeting, Rad.Damage 1981
Summary= For structural materials based on (n,nx),(n,px) and (n,alpha x) data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9401 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 22-30 A-Range= 37- 86 E-Range= 20- 30 MeV
Author(s)= O.F.Lemos
Reference= Orsay, Series A ,No.136 (1972)
Summary= Diffusion Elastique de Particules Alpha de 21 a 29.6 MeV de la
Region Ti-Zn, Orsay, France
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9600 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 8-96 A-Range= 16-250 E-Range= 1- 73 MeV
Author(s)= V.Avrigeanu,P.E.Hodgson, and M.Avrigeanu
Reference= Report OUNP-94-02 (1994) , Phys. Rev. C49,2136 (1994)
Summary= global potential - extension of potential by Nolte et al ref. Phys.
Rev. c36,1312 (1987)
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9601 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 39-50 A-Range= 89-124 E-Range= 1- 32 MeV
Author(s)= M.Avrigeanu,W.von Oertzen,F.L.Roman, and V.Avrigeanu
Reference= Progress Report IAEA RC 12422/R1 (2004), see also Nucl. Phys. A723,1
04(2003)
Summary= Regional potential parameters based on alpha-particle elastic
differential data
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9603 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 21-21 A-Range= 44- 46 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 21 A = 45
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9604 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 22-22 A-Range= 43- 45 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 22 A = 44
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9605 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 22-22 A-Range= 45- 47 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 22 A = 46
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9606 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 22-22 A-Range= 47- 49 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 22 A = 48
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9607 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 22-22 A-Range= 49- 51 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 22 A = 50
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9608 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 23-23 A-Range= 50- 52 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 23 A = 51
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9609 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 24-24 A-Range= 49- 51 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 24 A = 50
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9610 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 24-24 A-Range= 51- 52 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 24 A = 52
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9611 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 24-24 A-Range= 52- 54 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 24 A = 53
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9612 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 25-25 A-Range= 54- 56 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 25 A = 55
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9613 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-26 A-Range= 53- 55 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 26 A = 54
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9614 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-26 A-Range= 55- 57 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 26 A = 56
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9615 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 26-26 A-Range= 57- 59 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 26 A = 58
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9616 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 27-27 A-Range= 58- 60 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 27 A = 59
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9617 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 57- 59 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 28 A = 58
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9618 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 59- 61 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 28 A = 60
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9619 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 61- 63 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 28 A = 62
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9620 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 28-28 A-Range= 63- 65 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 28 A = 64
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9621 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 29-29 A-Range= 62- 64 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 29 A = 63
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9622 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 29-29 A-Range= 64- 66 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 29 A = 65
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9623 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 32-32 A-Range= 69- 71 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 32 A = 70
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9624 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 32-32 A-Range= 71- 73 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 32 A = 72
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9625 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 32-32 A-Range= 73- 75 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 32 A = 74
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9626 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 32-32 A-Range= 75- 77 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 32 A = 76
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9627 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 34-34 A-Range= 75- 77 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 34 A = 76
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9628 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 34-34 A-Range= 77- 79 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 34 A = 78
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9629 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 34-34 A-Range= 79- 81 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 34 A = 80
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9630 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 39-39 A-Range= 88- 90 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 39 A = 89
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9631 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 40-40 A-Range= 89- 90 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 40 A = 90
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9632 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 40-40 A-Range= 90- 92 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 40 A = 91
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9633 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 40-40 A-Range= 91- 93 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 40 A = 92
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9634 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 42-42 A-Range= 91- 93 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 42 A = 92
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9635 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 42-42 A-Range= 93- 95 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 42 A = 94
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9636 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 44-44 A-Range= 95- 97 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 44 A = 96
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9637 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 44-44 A-Range= 97- 99 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 44 A = 98
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9638 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 47-47 A-Range= 106-108 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 47 A = 107
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9639 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 48-48 A-Range= 105-107 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 48 A = 106
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9640 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 49-49 A-Range= 112-114 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 49 A = 113
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9641 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 49-49 A-Range= 114-116 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 49 A = 115
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9642 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 50-50 A-Range= 111-113 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 50 A = 112
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9643 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 50-50 A-Range= 115-116 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 50 A = 116
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9644 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 50-50 A-Range= 116-117 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 50 A = 117
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9645 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 50-50 A-Range= 117-120 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 50 A = 118
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9646 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 50-50 A-Range= 121-123 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 50 A = 122
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9647 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 50-50 A-Range= 123-125 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 50 A = 124
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9648 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 51-51 A-Range= 120-122 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 51 A = 121
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9649 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 51-51 A-Range= 122-124 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 51 A = 123
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9650 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 52-52 A-Range= 119-121 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 52 A = 120
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9651 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 52-52 A-Range= 123-125 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 52 A = 124
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9652 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 52-52 A-Range= 125-127 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 52 A = 126
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9653 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 52-52 A-Range= 127-129 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 52 A = 128
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9654 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 52-52 A-Range= 129-131 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 52 A = 130
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9655 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 53-53 A-Range= 126-128 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 53 A = 127
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9656 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 54-54 A-Range= 135-137 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 54 A = 136
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9657 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 56-56 A-Range= 131-133 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 56 A = 132
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9658 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 56-56 A-Range= 133-135 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 56 A = 134
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9659 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 56-56 A-Range= 135-137 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 56 A = 136
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9660 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 56-56 A-Range= 137-139 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 56 A = 138
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9661 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 57-57 A-Range= 138-140 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 57 A = 139
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9662 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 58-58 A-Range= 139-141 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 58 A = 140
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9663 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 59-59 A-Range= 140-142 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 59 A = 141
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9664 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 60-60 A-Range= 152-154 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 60 A = 153
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9665 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 143-145 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 62 A = 144
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9666 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 62-62 A-Range= 153-155 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 62 A = 154
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9667 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 65-65 A-Range= 158-160 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 65 A = 159
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9668 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 67-67 A-Range= 164-166 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 67 A = 165
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9669 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 69-69 A-Range= 168-170 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 69 A = 169
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9670 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 73-73 A-Range= 180-182 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 73 A = 181
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9671 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 74-74 A-Range= 181-183 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 74 A = 182
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9672 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 74-74 A-Range= 183-185 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 74 A = 184
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9673 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 74-74 A-Range= 185-187 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 74 A = 186
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9674 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 76-76 A-Range= 191-193 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 76 A = 192
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9675 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 77-77 A-Range= 190-192 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 77 A = 191
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9676 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 79-79 A-Range= 196-198 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 79 A = 197
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9677 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 82-82 A-Range= 207-209 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 82 A = 208
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
IREF= 9678 Alpha incident, spherical nucleus model
Potential is non-relativistic and non-dispersive
Z-Range= 83-83 A-Range= 208-210 E-Range= 1- 50 MeV
Author(s)= M.Avrigeanu, A.C. Obreja, F.L. Roman, V. Avrigeanu, and W. von Oert
zen
Reference= At. Data Nucl. Data Tables 95(2009)501; EFFDOC-1081, OECD/NEA, Paris
, Nov. 2009.
Summary= Regional parameter set for alpha-particles, from analysis of
elastic-scattering data for nuclei within 50<A<209 mass and ~13-50
MeV energy ranges, and (alpha,x)reaction cross-sections for target
nuclei from 45Sc to 197Au, below ~12-20 MeV. Target: Z = 83 A = 209
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++