IAEA-NDS ENDF Download System, v-2008-07-22 0 0 0 0
2.90000+ 4 6.29940+ 1 1 0 6 581295 1451 1
0.00000+ 0 0.00000+ 0 0 0 293 01295 1451 2
29-CU SAI EVAL-NOV73 M.K. DRAKE AND M.P. FRICKE 1295 1451 3
DIST-AUG74 REV-JUN75 1295 1451 4
*************** DNA 4529 MOD 1 ******************** 1295 1451 5
SAME AS DNA 4529 MOD 0 EXCEPT AS FOLLOWS 1295 1451 6
(1) EXCITATION FUNCTIONS FOR INELASTIC SCATTERING TO 0.962-MEV 1295 1451 7
LEVEL IN CU-63(MT=53,MF=3) AND TO 1.115-MEV LEVEL IN CU-65 1295 1451 8
(MT=54,MF=3) WERE INCREASED BETWEEN 3.5- AND 10-MEV INCIDENT 1295 1451 9
ENERGY TO BETTER AGREE WITH NEW ORNL DATA BETWEEN 5.5 AND 1295 1451 10
8.0 MEV (W.E. KINNEY, PRIVATE COMMUNICATION,1973). ADDITIONAL 1295 1451 11
INELASTIC SCATTERING CROSS SECTION WAS SUBTRACTED FROM ELASTIC 1295 1451 12
SCATTERING CROSS SECTION (MT=2,MF=3). 1295 1451 13
(2) LEGENDRE COEFFICIENTS FOR ELASTIC SCATTERING (MT=2,MF=4) 1295 1451 14
IN ABOVE REFERENCE ADDED AT INCIDENT ENERGIES 5.5 AND 8.5 MEV. 1295 1451 15
(3) PHOTON PRODUCTION MEASUREMENTS FROM 1.25- TO 20-MEV INCIDENT1295 1451 16
NEUTRON ENERGY WERE INCORPORATED FROM J.K. DICKENS ET AL., 1295 1451 17
ORNL-4846(1973). IN MF=13, ALL PHOTON PRODUCTION IS GIVEN UNDER 1295 1451 18
MT=3. IN MF=12 AND 15, PHOTON PRODUCTION FROM RADIATIVE CAPTURE 1295 1451 19
IS RETAINED SEPARATELY UNDER MT=102 AT NEUTRON ENERGIES BELOW 1295 1451 20
1.25 MEV. AT HIGHER NEUTRON ENERGIES, ALL PHOTON PRODUCTION IS 1295 1451 21
GIVEN IN MF=15 UNDER MT=3. 1295 1451 22
* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * 1295 1451 23
* * * THE FOLLOWING DESCRIPTION PERTAINS TO THE DATA OF MOD 0 * *1295 1451 24
1295 1451 25
* * * * * * *1295 1451 26
THIS MATERIAL CONTAINS NEUTRON AND GAMMA RAY PRODUCTION CROSS 1295 1451 27
SECTIONS FOR THE ELEMENT COPPER. ENERGY AND ANGULAR DISTRIBUTIONS1295 1451 28
ARE GIVEN FOR ALL SECONDARY NEUTRONS AND GAMMA RAYS PRODUCED BY 1295 1451 29
NEUTRON INTERECTIONS. THE CUTOFF DATE FOR NEW INFORMATION WAS 1295 1451 30
NOV. 1972. 1295 1451 31
* * * * * FILE 2 (RESONANCE PARAMETERS) * * * * * * * * * * * * 1295 1451 32
MULTI-LEVEL BRIET-WIGNER RESOLVED RESONANCE PARAMETERS HAVE 1295 1451 33
BEEN PROVIDED FOR THE ENERGY RANGE FROM 10 EV TO 30 KEV. SMALL 1295 1451 34
BACKGROUND C/S HAVE BEEN GIVEN IN FILE 3 FOR THE TOTAL, ELASTIC 1295 1451 35
SCATTERING, AND RADIATIVE CAPTURE C/S TO ACCOUNT FOR MISSING 1295 1451 36
LEVELS IN THE RESOLVED PARAMETERS. RESOLVED PARAMETERS WERE TAKEN1295 1451 37
FROM THE ENDF/B-III LIBRARY, MAT=1087. THIS EVALUATION USED THE 1295 1451 38
RECOMMENDED PARAMETERS GIVEN IN BNL-325 (2) AS THE PRINCIPAL 1295 1451 39
SOURCE OF INFORMATION (1). 1295 1451 40
NO UNRESOLVED RESONANCE PARAMETERS WERE GIVEN FOR THIS 1295 1451 41
MATERIAL. CONSIDERABLE STRUCTURE HAS BEEN OBSERVED IN THE TOTAL 1295 1451 42
ABOVE 30 KEV. THIS STRUCTURE WAS REPRESENTED IN FILE 3. 1295 1451 43
* * * * * FILE 3 (NEUTRON CROSS SECTIONS) * * * * * * * * * * * 1295 1451 44
LOW ENERGY CROSS SECTIONS * * * * * * * * * * * * ** * * * * 1295 1451 45
THE TOTAL, ELASTIC SCATTERING AND RADIATIVE CAPTURE C/S FROM 1295 1451 46
0.00001 TO 10 EV TAKEN FROM MAT=1087 (1). THERE WERE NO NEW 1295 1451 47
EXPERIMENTAL DATA FOR THIS ENERGY RANGE AND THE C/S IN MAT=1087 1295 1451 48
WERE CONSIDERED TO BE THE BEST AVAILABLE. 1295 1451 49
TOTAL CROSS SECTION (MT=1) * * * * * * * * * * * * * * * * * 1295 1451 50
BETWEEN 30 KEV AND 100 KEV, THE DATA MEASURED BY GARG, ET.AL. 1295 1451 51
(3) WERE USED. IN THIS ENERGY RANGE THERE WAS CONSIDERABLE 1295 1451 52
STRUCTURE IN THE EXPERIMENTAL DATA, BUT IT WAS NOT MEASURED 1295 1451 53
WELL ENOUGH TO OBTAIN RESOLVED RESONANCE PARAMETERS. IN THE EN. 1295 1451 54
REGION FROM 100 KEV TO 1.5 MEV, THE ANL RESULTS OBTAINED BY 1295 1451 55
MEADOWS AND WHALEN (4) WERE USED. IN THE UPPER PORTION OF THIS 1295 1451 56
ENERGY RANGE (1.2 TO 1.5 MEV) THE EXPERIMENTAL DATA WERE AVERAGED1295 1451 57
OVER 200 KEV ENERGY BANDS SINCE THE VARIATIONS IN THE EXPERIMENT-1295 1451 58
TAL DATA APPEARED TO BE MORE STATISTICAL THAN STRUCTURE IN C/S. 1295 1451 59
VERY POOR QUALITY DATA WERE AVAILABLE FOR THE REGION FROM 1.5 1295 1451 60
TO 2.3 MEV (5,6). A SMOOTH CURVE WAS DRAWN FOR THE TOTAL CROSS 1295 1451 61
SECTION. THE CURVE DID NOT GO THROUGH THE AVERAGE OF THE DATA, 1295 1451 62
RATHER THE CURVE WAS DRAWN TO FIT THE BETTER DATA BELOW 1.5 MEV 1295 1451 63
AND ABOVE 2.3 MEV. BETWEEN 2.3 AND 12 MEV, A SMOOTH CURVE WAS 1295 1451 64
DRAWN THROUGH THE FOSTER AND GLASGOW (7) DATA. AN AVERAGE OF THE 1295 1451 65
DATA MEASURED BY FOSTER AND GLASGOW (7), ALBERGOTTI AND FERGUSON 1295 1451 66
(8), AND ROBINSON, ET.AL.(9) WERE USED FOR NEUTRON ENERGIES 1295 1451 67
BETWEEN 12 AND 15 MEV. ABOVE 15 MEV A SMOOTH AND SLOWLY DECRES- 1295 1451 68
ING CURVE WAS DRAWN THROUGH THE AVAILABLE DATA (10,11,12,13). 1295 1451 69
* *ELASTIC SCATTERING CROSS SECTION (MT=2) * * * * * * * * * * * 1295 1451 70
IN THE REGION FROM 10 EV TO 30 KEV, THE ELASTIC SCATTERING C/S1295 1451 71
WAS REPRESENTED AS RESOLVED RESONANCE PARAMETERS. BETWEEN 1.0 AND1295 1451 72
30 KEV A SMALL BACKGROUND C/S HAS BEEN INCLUDED IN FILE 3 TO 1295 1451 73
ACCOUNT FOR MISSING LEVELS IN THE RESOLVED RESONANCES. AT ALL 1295 1451 74
OTHER ENERGIES, THE ELASTIC SCATTERING CROSS SECTION WAS OBTAINED1295 1451 75
BY SUBTRACTING THE NON-ELASTIC CROSS SECTION FROM THE EVALUATED 1295 1451 76
TOTAL CROSS SECTION. THE RESULTING CROSS SECTION WAS COMPARED TO 1295 1451 77
THE AVAILABLE EXPERIMENTAL DATA FOR ELASTIC SCATTERING. IN THE 1295 1451 78
ENERGY REGION FROM 0.3 TO 4.0 MEV, THE EVALUATED CROSS SECTION 1295 1451 79
AGREED VERY WELL WITH THE AVAILABLE MEASUREMENTS (14,15,16,17). 1295 1451 80
BETWEEN 4 AND 8 MEV, THE EVALUATED CURVE WAS SLIGHLY HIGHER 1295 1451 81
THAN THE MEASURED DATA OF HOLMQVIST (17). 1295 1451 82
* *NON-ELASTIC CROSS SECTION (MT=3) * * * * * * * * * * * * * * 1295 1451 83
THE NON-ELASTIC CROSS SECTION FOR THE ELEMENT WAS OBTAINED 1295 1451 84
BY EVALUATING HHE NON-ELASTIC CROSS SECTIONS FOR THE ISOTOPES. 1295 1451 85
BELOW 600 KEV, THE NON-ELASTIC CROSS SECTION WAS THE SAME AS THE 1295 1451 86
RADIATIVE CAPTURE CROSS SECTION. BETWEEN 600 KEV AND 5 MEV, THE 1295 1451 87
NON-ELASTIC CROSS SECTIONS FOR THE ISOTOPES WERE OBTAINED BY 1295 1451 88
SUMMING THE COMPONENTS. ABOVE 5 MEV, THE NON-ELASTIC CROSS 1295 1451 89
SECTIONS FOR THE ISOTOPES WERE TAKEN TO BE THE SAME AS THE 1295 1451 90
ELEMENT WHICH WAS EVALUATED BY DRAWING A SMOOTH CURVE THROUGH 1295 1451 91
THE EXISTING EXPERIMENTAL DATA (18,19,20,21,22,23,24,25,26,27). 1295 1451 92
IN THE ENERGY RANGE FROM 6 TO 9 MEV, THERE WAS A DISCREPANCY 1295 1451 93
BETWEEN THE AVAILABLE EXPERIMENTAL DATA FOR ELASTIC SCATTERING 1295 1451 94
(17) AND NON-ELASTIC CROSS SECTION (18,20). THE EVALUATED CROSS 1295 1451 95
SECTION FOR BOTH THE ELASTIC AND NON-ELASTIC CROSS SECTIONS WERE 1295 1451 96
SLIGHLY HIGHER THAN THE EXPERIMENTAL DATA. THIS WAS DONE TO 1295 1451 97
PRESERVE THE TOTAL C/S WHICH WAS MEASURED MORE ACCURATELY. 1295 1451 98
* *(N,2N) CROSS SECTION (MT=16) * * * * * * * * * * * * * * * * 1295 1451 99
THE(N,2N) CROSS SECTION WAS OBTAINED FROM EVALUATIONS OF 1295 1451 100
OF THE (N,2N) CROSS SECTIONS FOR THE ISOTOPES. BOTH CU-63 (N,2N) 1295 1451 101
AND CU-65 (N,2N) CROSS SECTIONS HAVE USED AS CROSS SECTION 1295 1451 102
STANDARDS, CU-65 MORE THAN CU-63. 1295 1451 103
MANY SETS OF EXPERIMENTAL DATA WERE AVAILABLE FOR CU-63. SOME 1295 1451 104
WERE ABSOLUTE AND OTHERS WERE RELATIVE. THE RELATIVE MEASUREMENTS1295 1451 105
(28,29,30,31,32) WERE RE-NORMALIZED TO 0.568 BARNS AT 14.7 MEV, 1295 1451 106
CONSISTENT WITH THE CU-65 (N,2N) CROSS SECTION AT THIS ENERGY 1295 1451 107
THE ABSOLUTE VALUES (33,34,35,36) ALONG WITH THE RESULTS FROM 1295 1451 108
14 MEV MEASUREMENTS AND THE RE-NORMALIZED CROSS SECTION VALUES 1295 1451 109
WERE USED TO OBTAIN THE RECOMMENDED CROSS SECTION. 1295 1451 110
THE CU-65 (N,2N) CROSS SECTION WAS TAKEN FROM THE ENDF/B 1295 1451 111
DOSIMETRY LIBRARY. THIS EVALUATION WAS BASED ON MEASUREMENTS BY 1295 1451 112
SANTRY AND BUTLER (37), PRESTWOOD AND BAYHURST (38), PAULSEN AND 1295 1451 113
LISKIEN (39), RAYBURN (31), AND BORMANN AND LAMMERS (36). 1295 1451 114
* *(N,P) AND (N,N-P) CROSS SECTIONS (MT=28,103) * * * * * * * * 1295 1451 115
THESE CROSS SECTIONS WERE OBTAINED FOR THE ELEMENT BY EVAL- 1295 1451 116
UATING THE RESPECTIVE CROSS SECTIONS FOR THE ISOTOPES. THERE WAS 1295 1451 117
VERY LITTLE EXPERIMENTAL DATA AVAILABLE FOR CU-63 (N,P) OR 1295 1451 118
CU-63 (N,N-P). THESE CROSS SECTIONS WERE OBTAINED FROM STATISTIC-1295 1451 119
AL MODEL CALCULATIONS. THE CALCULATED RESULTS WERE NORMALIZED AT 1295 1451 120
14.5 MEV TO THE SPARCE EXPERIMENTAL DATA (40,41,42,43) 1295 1451 121
THE (N,P) CROSS SECTION FOR CU-65 HAS BEEN MEASURED FROM 1295 1451 122
THRESHOLD (ABOUT 3 MEV) TO 20 MEV. THE DATA OF SANTRY AND BUTLER 1295 1451 123
(37) WERE USED FOR THE COMPLETE ENERGY RANGE. THE MAGNITUDE OF 1295 1451 124
THE CROSS SECTION NEAR 14 MEV WAS WELL ESTABLISHED BY SEVERAL 1295 1451 125
OTHER MEASUREMENTS. FEW AND WIDELY DISAGREEING VALUES HAVE BEEN 1295 1451 126
MEASURED FOR THE (N,N-P) C/S. THE SAME PROCEDURE FOR CU-63 1295 1451 127
(N,N-P) WAS USED FOR CU-65 (N,N-P) C/S. 1295 1451 128
* *(N,ALPHA) AND (N,N-ALPHA) CROSS SECTIONS (MT=22,107) * * * * 1295 1451 129
THE CROSS SECTIONS FOR THE ELEMENT WERE OBTAINED FROM 1295 1451 130
EVALUATED CROSS SECTIONS FOR THE ISOTOPES. THE (N,ALPHA) CROSS 1295 1451 131
SECTION FOR CU-63 WAS TAKEN FROM THE ENDF/B DOSIMETRY 1295 1451 132
FILE. THIS EVALUATION WAS BASED ON THE DATA OF PAULSEN AND 1295 1451 133
LISKIEN (44). THE (N,N-ALPHA) CROSS SECTION FOR CU-63 WAS BASED 1295 1451 134
ON A STATISTICAL MODEL CALCULATION WHICH WAS NORMALIZED TO AN 1295 1451 135
EXPERIMENTAL VALUE AT 14.8 MEASURED BY IRFAN AND JACK (45). 1295 1451 136
THE (N,ALPHA) CROSS SECTION FOR CU-65 WAS BASED ON A 1295 1451 137
STATISTICAL MODEL CALCULATION AND THE CALCULATED CURVE WAS 1295 1451 138
NORMALIZED TO THE AVAILABLE EXPERIMENTAL DATA(46,47,48) AT 1295 1451 139
14 MEV. THE (N,N-ALPHA) CROSS SECTION WAS BASED ON THE EXPERI- 1295 1451 140
MENTAL DATA OF SANTRY AND BUTLER (37), BRAMLITT AND FINK (46), 1295 1451 141
AND KANTELE AND GARDNER (49). 1295 1451 142
* *RADIATIVE CAPTURE CROSS SECTION (MT=102) * * * * * * * * * * 1295 1451 143
ABOVE 30 KEV, THE RADIATIVE CAPTURE CROSS SECTION WAS OBTAINED1295 1451 144
BY EVALUATING THIS CROSS SECTION FOR THE ISOTOPES. BETWEEN 30 KEV1295 1451 145
AND 3 MEV, THE CU-63 (N,G) CROSS SECTION WAS BASED ON THE EXPERI-1295 1451 146
MENTAL DATA OF DOVBENKO, ET.AL. (50) AND ZAIKIN, ET.AL.(51). 1295 1451 147
THE RECOMMENDED CURVE WAS DRAWN SLIGHLY HIGHER THAN THE DOVBENKO 1295 1451 148
DATA AND LOWER THAN THE ZAIKIN DATA. AT 14 MEV, THE CURVE WAS 1295 1451 149
DRAWN THROUGH PERKIN (52) AND A RECENT COLUMBIA VALUE (53). 1295 1451 150
THE CU-65 (N,G) CROSS SECTION HAD BEEN MEASURED SEVERAL TIMES 1295 1451 151
ABOVE 30 KEV. THE RESULTS FROM THESE MEASUREMENTS WERE NOT IN 1295 1451 152
GOOD AGREEMENT. THE RECOMMENDED CURVE WAS DRAWN THROUGH 46 MB 1295 1451 153
AT 25 KEV, WHICH WAS AN AVERAGE OF SEVERAL MONO-ENERGETIC MEASUR-1295 1451 154
EMENTS BETWEEN 20 AND 25 KEV. ABOVE 30 KEV, THE RECOMMENDED CURVE 1295 1451 155
WAS DRAWN ON THE LOW SIDE OF VALUES MEASURED BY TOLSTIKOV (54) 1295 1451 156
AND STAVISSKII AND TOLSTIKOV (55). BETWEEN 600 KEV AND 3 MEV, 1295 1451 157
THE DATA MEASURED BY ZAIKIN, ET.AL, WERE USED. 1295 1451 158
* *INELASTIC SCATTERING CROSS SECTIONS (MT=4,51,52,..,91) * * * 1295 1451 159
THE INELASTIC SCATTERING CROSS SECTION WAS MADE UP OF 11 1295 1451 160
DISCRETE LEVELS AND A CONTINUUM. SEVERAL SETS OF INELASTIC 1295 1451 161
SCATTERING AND GAMMA RAY PRODUCTION CROSS SECTION MEASUREMENTS 1295 1451 162
WERE USED TO OBTAINED THE LEVEL EXCITATION CROSS SECTIONS FOR 1295 1451 163
NEUTRON ENERGIES UP TO 1.5 MEV (14,56,57,58,59) FOR THE 0.67 1295 1451 164
AND 0.912 MEV LEVELS IN CU-63 AND THE 0.77 AND 1.115 MEV LEVELS 1295 1451 165
IN CU-65. THE HELENE CODE WAS USED TO OBTAIN LEVEL EXCITATION 1295 1451 166
FUNCTIONS FOR THE HIGHER ENERGY LEVELS. THE DWUCK CODE WAS USED 1295 1451 167
TO ESTIMATE DIRECT INTERACTION CONTRIBUTIONS. ABOVE 1.5 MEV THE 1295 1451 168
MODEL CODES WERE USED TO ESTIMATE ALL LEVEL EXCITATION CROSS 1295 1451 169
SECTIONS AND THE CONTINUUM PART. 1295 1451 170
* * * * * FILE 4 (ANGULAR DISTRIBUTIONS FOR SECONDARY NEUTRONS) 1295 1451 171
* *ELASTIC SCATTERING (MT=2) * * * * * * * * * * * * * * * * * 1295 1451 172
BELOW 100 KEV THE ANGULAR DISTRIBUTIONS FOR ELASTICALLY 1295 1451 173
SCATTERED NEUTRONS WERE TAKEN TO BE ISOTROPIC. ABOVE 100 KEV THE 1295 1451 174
ANGULAR DISTRIBUTIONS WERE OBTAINED BY FITTING EXPERIMENTAL DATA 1295 1451 175
WITH LEGENDRE COEFFICIENTS. BETWEEN 100 KEV AND 600 KEV THE 1295 1451 176
DATA OF LANE, ET.AL (60) WERE USED. BETWEEN 600 KEV AND 1.2 MEV,1295 1451 177
THE DATA MEASURED BY COX (61) WERE USED AND BETWEEN 1.5 AND 8 MEV1295 1451 178
THE MEASUREMENT MADE BY HOLMQVIST (17) WAS USED. NEAR 14 MEV THE 1295 1451 179
RESULTS FROM SEVERAL MEASUREMNTS WERE USED (62,63,64). FROM 8 1295 1451 180
TO 14 MEV AND ABOVE 15 MEV, THE ANGULAR DISTRIBUTIONS WERE 1295 1451 181
CALCULATED USING THE HELENE AND DWUCK CODES. 1295 1451 182
* *NON-ELASTIC REACTION (MT=51,52,..,91,22,28,16) * * * * * * * 1295 1451 183
ANGULAR DISTRIBUTIONS FOR NEUTRONS FROM INELASTIC LEVEL 1295 1451 184
REACTIONS WERE OBTAINED FROM THE HELENE CODE (COMPOUND NUCLEUS 1295 1451 185
PART) AND THE DWUCK CODE (DIRECT INTERACTION PART). CALCULATIONS 1295 1451 186
WERE MADE FOR THE FIRST 3 LEVELS IN EACH ISOTPE. THERE WAS 1295 1451 187
REASONABLY GOOD AGREEMENT BETWEEN THE CALCULATED DISTRIBUTIONS 1295 1451 188
FOR THE 0.77 AND 1.115 MEV LEVELS AT 2.33 MEV AND A MEASUREMENT 1295 1451 189
BY ROGERS ET.AL.(65). ALL OTHER LEVELS , THE CONTINUUM, AND ALL 1295 1451 190
OTHER NEUTRON PRODUCING REACTIONS WERE ASSUMED TO HAVE ISOTROPIC 1295 1451 191
DISTRIBUTIONS IN THE C.M. SYSTEM. 1295 1451 192
* * * * * FILE 5 (ENERGY DISTRIBUTIONS FOR SECONDARY NEUTRONS) 1295 1451 193
THE ENERGY DISTRIBUTIONS FOR INELASTIC SCATTERING CONTINUUM 1295 1451 194
(MT=91) AND (N,2N) (MT=16) WERE BASED ON THE STATISTICAL MODEL. 1295 1451 195
AN EFFECTIVE NUCLEAR TEMPERAURE OF 1.02 MEV AT 14.1 MEV WAS 1295 1451 196
USED. THE EFFECTIVE NUCLEAR TEMPERATURE OF THE SECOND NEUTRON FOR1295 1451 197
THE (N,2N) REACTION WAS 0.4 MEV AT 14 MEV. 1295 1451 198
* * * * * FILE 12 (MULTIPLICITIES FOR RADIATIVE CAPTURE) * * * * 1295 1451 199
THE MULTIPLICITIES FOR RADIATIVE CAPTURE GAMMA RAYS WAS TAKEN 1295 1451 200
FROM A THERMAL NEUTRON MEASUREMENT MADE BY ORPHAN, ET.AL (66). 1295 1451 201
THE MULTIPLICITIES WERE INCREASED AS A FUNCTION OF THE NEUTRON 1295 1451 202
ENERGY TO PRESERVE TOTAL ENERGY RELEASED. 1295 1451 203
* * * * FILE 13 (N,N-G) AND (N,2N-G) GAMMA RAY PRODUCTION 1295 1451 204
CROSS SECTIONS * * * * * * * * * * * * * * * * * * * * 1295 1451 205
THE TOTAL PRODUCTION CROSS SECTION DUE TO THE (N,N-G) REACTION1295 1451 206
WAS MADE UP OF 5 DISCRETE LINES AND A CONTINUUM PART. THE GAMMA 1295 1451 207
RAY PRODUCTION CROSS SECTIONS AND THE ENERGY DISTRIBUTIONS OF THE1295 1451 208
SECONDARY GAMMA RAYS WERE OBTAINED BY USING A MODIFIED VERSION 1295 1451 209
OF THE SPECT10 CODE. CALCULATIONS WERE MADE FOR EACH ISOTOPE 1295 1451 210
USING THE EVALUATED DISCRETE LEVEL EXCITATION CROSS SECTIONS, 1295 1451 211
THE CONTINUUM CROSS SECTION, BRANCHING RATIOS, AND NUCLEAR LEVEL 1295 1451 212
DENSITY DATA. THE CALCULATED PRODUCTION CROSS SECTIONS FOR THE 1295 1451 213
DISCRETE LINES WERE INCREASED SLIGHLY (ABOUT 20 PERCENT) NEAR 1295 1451 214
15 MEV TO OBTAIN AGREEMENT WITH JONSSON ET. AL. (67). 1295 1451 215
SIMILAR CALCULATIONS WERE MADE FOR THE (N,2N-G) REACTION. ALL 1295 1451 216
GAMMA RAYS WERE TREATED AS A CONTINUUM. 1295 1451 217
* * * * * FILE 15 (ENERGY DISTRIBUTIONS FOR SECONDARY GAMMA RAYS)1295 1451 218
THE SPECT10 CODE WAS USED TO ESTIMATE THE ENERGY DISTRIBUTIONS1295 1451 219
FOR ALL SECONDARY GAMMA RAYS FROM INELASTIC SCATTERING AND 1295 1451 220
(N,2N) REACTIONS. THE ENERGY DISTRIBUTIONS FOR GAMMA RAYS FROM 1295 1451 221
RADIATIVE CAPTURE WERE TAKEN FROM A MEASUREMNT MADE BY ORPHAN, 1295 1451 222
ET. AL. (66). 1295 1451 223
(1) J.M.OTTER,ET.AL., REPORT AI-AEC-1271 (1968) 1295 1451 224
(2) M.D.GOLDBERG, ET.AL., BNL-325, 2ND ED., SUPPL. 2, VOL IIA 1295 1451 225
(1966) 1295 1451 226
(3) J.B.GARG, J.RAINWATER, AND W.W.HAVENS,JR., REPORT 1295 1451 227
EANDC(US)- 54 L (1964) 1295 1451 228
(4) J.W.MEADOWS AND J.F. WHALEN (ANL) PRI.COMM. (1972) 1295 1451 229
(5) M.N.NIKOLAYEV. ET.AL., PHYS OF FAST AND INTERMEDIATE 1295 1451 230
REACTORS, VOL.I, (1961) 1295 1451 231
(6) D.W.MILLER, ET.AL., PHYS.REV. 88, 1042 (1952) 1295 1451 232
(7) D.G.FOSTER,JR. AND D.W. GLASGOW, PHYS.REV. 3,C576 (1971) 1295 1451 233
(8) J.C.ALBERGOTTI AND J.M.FERGUSON, NUCL.PHYS. 82,652 (1966) 1295 1451 234
(9) W.K.ROBINSON, ET.AL., AMERICAN J.PHYS. 37,482 (1969) 1295 1451 235
(10) P.H.BOWEN, ET.AL., NUCL.PHYS. 22,640 (1960) 1295 1451 236
(11) J.M.PETERSON, ET.AL., PHYS.REV. 120,521 (1960) 1295 1451 237
(12) R.B.DAY AND R.L.HENKEL, PHYS.REV. 92,358 (1958) 1295 1451 238
(13) M.MAZARI, ET.AL., PHYS. REV. 100,972 (1955) 1295 1451 239
(14) A.B.SMITH, ET.AL., PHYS. REV. 135,76 (1964) 1295 1451 240
(15) I.A.KORZH, ET.AL., AT. EN. 16,260 (1964) 1295 1451 241
(16) L.YA.KASAKOVA, ET.AL., CONF. ON NUCLEAR STRUCTURE STUDY 1295 1451 242
WITH NEUTRONS, P 200, ANTWERP (1965) 1295 1451 243
(17) B.HOLMQVIST, ARKIV FYSIK 38,403 (1968) 1295 1451 244
(18) J.R.BEYSTER, ET.AL., PHYS.REV. 104,1319 (1956) 1295 1451 245
(19) H.L.TAYLOR, ET.AL., PHYS.REV. 100,174 (1955) 1295 1451 246
(20) W.P.BALL, ET.AL., PHYS.REV. 110,1392 (1958) 1295 1451 247
(21) T.W.BONNER AND J.C. SLATTERY, PHYS.REV. 113,1088 (1959) 1295 1451 248
(22) G.M.HAAS AND P.L.OKHUYSEN, PHYS.REV. 132,1211 (1963) 1295 1451 249
(23) D.D.PHILLIPS, ET.AL., PHYS.REV. 88,600 (1952) 1295 1451 250
(24) M.H.MAC GREGOR, ET.AL., PHYS.REV. 108,726 (1957) 1295 1451 251
(25) D.DIDIER, ET.AL., REPORT EANDC(E) - 49 L (1963) 1295 1451 252
(26) A.CHATTERJEE AND A.M.GHOSE, PHYS.REV. 161,1181 (1967) 1295 1451 253
(27) YU.G.DEGTYAREV AND V.G.NADTOCHII, AT.EN. 11, 397 (1961) 1295 1451 254
(28) D.R.KOHLER AND W.L.ALFORD, REPORT AOMC-RR-62-1 (1969) 1295 1451 255
(29) A.V.COHEN AND P.H.WHITE, NUCL.PHYS. 1, 73 (1956) 1295 1451 256
(30) J.C.CSIKAI AND G.PETO, ACTAPHYS.ACAD.SCI.HUNGARICAE 1295 1451 257
23, 87 (1967) 1295 1451 258
(31) L.A.RAYBURN, PHYS.REV. 130, 731 (1963) 1295 1451 259
(32) R.N.GLOVER AND E.WEIGOLD, NUCL.PHYS. 29, 309 (1962) 1295 1451 260
(33) W.E.THOMSON AND J.M.FERGUSON, PHYS.REV. 118, 228 (1960) 1295 1451 261
(34) M.BORMANN, ET.AL., Z.PHYSIK 166, 477 (1962) 1295 1451 262
(35) H.LISKIEN AND A.PAULSEN, J.NUCL.ENERGY A/B 19, 73 (1965) 1295 1451 263
(36) M.BORMANN AND B.LAMMERS, NUCL.PHYS. A130, 195 (1969) 1295 1451 264
(37) D.C.SANTRY AND J.P.BUTLER, CAN.J.PHYS. 44, 1183 (1966) 1295 1451 265
(38) R.J.PRESTWOOD AND B.P.BAYHURST, PHYS.REV. 121, 1438 (1961) 1295 1451 266
(39) A.PAULSEN AND H.LISKIEN, NUKLEONIK 7, 117 (1965) 1295 1451 267
(40) D.L.ALLAN, NUCL.PHYS. 24,274 (1961) 1295 1451 268
(41) R.S.STOREY, ET.AL., PROC.PHYS.SOC. 75,526 (1960) 1295 1451 269
(42) L.COLLI, ET.AL., NUOVO CIMENTO 13, 730 (1959) 1295 1451 270
(43) D.L.ALLAN, PROC.PHYS.SOC. 70, 195 (1957) 1295 1451 271
(44) A.PAULSEN, NUKLEONIK 10, 91 (1967) 1295 1451 272
(45) M.IRFAN AND W.JACK, PROC.PHYS.SOC. 81, 808 (1963) 1295 1451 273
(46) E.T.BRAMLITT AND R.W.FINK, PHYS.REV. 131, 2649 (1963) 1295 1451 274
(47) I.L.PRIESS AND R.W.FINK, NUCL.PHYS. 15, 626 (1960) 1295 1451 275
(48) D.L.CLAYTOR, DISSERTATION ABSTR. 30B, 2850 (1969) 1295 1451 276
(49) J.KANTELE AND D.G.GARDNER, NUCL.PHYS. 35, 353 (1962) 1295 1451 277
(50) A.G.DOVBENKO, ET.AL., REPORT INDC-260 E, P 11 (1969) 1295 1451 278
(51) G.G.ZAIKIN, ET.AL., AT.EN. 25,526 (1968) 1295 1451 279
(52) J.L.PERKIN, PROC.PHYS.SOC. 72, 505 (1958) 1295 1451 280
(53) M.STAMATELATOS, PRI.COMM. (1972) 1295 1451 281
(54) V.A.TOLSTIKOV, ET.AL., AT.EN. 17, 505 (1964) 1295 1451 282
(55) YU.YA.STAVISSKII AND V.A.TOLSTIKOV, AT.EN. 10, 508 (1961) 1295 1451 283
(56) N.P.GLAZKOV, AT.EN. 15,416 (1963) 1295 1451 284
(57) A.B.TUCKER, ET.AL., PHYS.REV. 137, 1181 (1965) 1295 1451 285
(58) B.HOLMQVIST AND T.WIEDLING, ARKIV FYSIK 35, 71 (1967) 1295 1451 286
(59) K.NISHIMURA, ET.AL., NUCL.PHYS. 70, 421 (1965) 1295 1451 287
(60) R.O.LANE, ET.AL., ANN.PHYS. 12, 135 (1961) 1295 1451 288
(61) S.A.COX, BULL.AM.PHYS.SOC 8, 478 (1963) 1295 1451 289
(62) J.H.COON, ET.AL., PHYS.REV. 111, 250 (1958) 1295 1451 290
(63) S.BERKO, ET.AL., NUCL.PHYS. 6, 210 (1958) 1295 1451 291
(64) B.YA.GUZHOVSKI, AT.EN. 11, 395 (1961) 1295 1451 292
(65) W.L.ROGERS, ET.AL., REPORT COO-1573-33 (1967) 1295 1451 293
(66) V.J.ORPHAN, ET.AL., REPORT GA-10248 (1970) 1295 1451 294
(67) B.JONSSON, ET.AL., ARKIV FYSIK 39, 295 (1969) 1295 1451 295
1 451 353 1295 1451 296
2 151 57 1295 1451 297
3 1 180 1295 1451 298
3 2 170 1295 1451 299
3 3 177 1295 1451 300
3 4 68 1295 1451 301
3 16 10 1295 1451 302
3 17 4 1295 1451 303
3 22 10 1295 1451 304
3 28 11 1295 1451 305
3 51 54 1295 1451 306
3 52 47 1295 1451 307
3 53 40 1295 1451 308
3 54 34 1295 1451 309
3 55 29 1295 1451 310
3 56 27 1295 1451 311
3 57 27 1295 1451 312
3 58 25 1295 1451 313
3 59 25 1295 1451 314
3 60 22 1295 1451 315
3 61 22 1295 1451 316
3 91 22 1295 1451 317
3 102 139 1295 1451 318
3 103 72 1295 1451 319
3 104 11 1295 1451 320
3 106 9 1295 1451 321
3 107 17 1295 1451 322
3 251 18 1295 1451 323
3 252 18 1295 1451 324
3 253 18 1295 1451 325
4 2 188 1295 1451 326
4 16 10 1295 1451 327
4 17 10 1295 1451 328
4 22 10 1295 1451 329
4 28 10 1295 1451 330
4 51 91 1295 1451 331
4 52 91 1295 1451 332
4 53 91 1295 1451 333
4 54 91 1295 1451 334
4 55 85 1295 1451 335
4 56 10 1295 1451 336
4 57 85 1295 1451 337
4 58 10 1295 1451 338
4 59 10 1295 1451 339
4 60 10 1295 1451 340
4 61 10 1295 1451 341
4 91 10 1295 1451 342
5 16 91 1295 1451 343
5 17 7 1295 1451 344
5 22 7 1295 1451 345
5 28 7 1295 1451 346
5 91 199 1295 1451 347
12 102 6 1295 1451 348
13 3 180 1295 1451 349
14 3 1 1295 1451 350
14 102 1 1295 1451 351
15 3 203 1295 1451 352
15 102 22 1295 1451 353
1295 1 0 354
1295 0 0 355
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1.00000+ 1 3.00000+ 4 1 2 0 01295 2151 358
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6.23890+ 1 0.00000+ 0 0 0 168 281295 2151 360
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