IAEA-NDS ENDF Download System, v-2008-07-22 0 0 0 0
1.30270+ 4 2.67500+ 1 0 0 6 46193 1451 1
0.00000+ 0 0.00000+ 0 0 0 138 06193 1451 2
13-AL-27 LASL EVAL-DEC73 P.G.YOUNG, D.G.FOSTER,JR. 6193 1451 3
DIST-FEB74 MOD3-NOV73 6193 1451 4
P.C. TO NORMALIZATION AND STANDARDS SUBCOMMITTEE MAY 1972 6193 1451 5
DATA SAME AS GENERAL FILE (MAT1193) 6193 1451 6
PERTINENT HOLLORITH AND ALL REFERENCES CARRIED OVER FROM GENERAL 6193 1451 7
FILE 6193 1451 8
6193 1451 9
******************* DNA 4135 MOD 3 11/73 ****************** 6193 1451 10
THE NEW EXPERIMENTAL DATA USED FOR THE MOD 3 REVISIONS ARE 6193 1451 11
INCLUDED IN THE DETAILED DESCRIPTIONS GIVEN BELOW. BRIEFLY, THE 6193 1451 12
FOLLOWING IMPROVEMENTS WERE MADE FOR MOD 3, 6193 1451 13
1. THE RADIATIVE CAPTURE GAMMA-RAY SPECTRUM FOR THERMAL 6193 1451 14
NEUTRONS WAS REVISED TO BETTER AGREE WITH RECENT DATA. 6193 1451 15
2. IMPROVED (N,P) AND (N,ALPHA) CROSS SECTIONS WERE INCOR- 6193 1451 16
PORATED. THESE DATA ARE THE SAME AS WERE PROVIDED 6193 1451 17
EARLIER TO THE STANDARDS SUBCOMMITTEE OF CSEWG. 6193 1451 18
3. FILE 13 AND FILE 15 (N,NGAMMA) AND (N,NPGAMMA) DATA WERE 6193 1451 19
REVISED TO INCLUDE THE MEASUREMENTS OF DI73. 6193 1451 20
4. THE (N,NPRIME) CROSS SECTIONS TO HIGH-LYING PSEUDO LEVELS 6193 1451 21
WERE REVISED FOR NEUTRON ENERGIES NEAR 14 MEV TO GIVE 6193 1451 22
BETTER AGREEMENT WITH MEASUREMENTS OF KA72. IN ADDITION, 6193 1451 23
(N,NPRIME) DATA TO LOWER LEVELS WERE REVISED TO BE 6193 1451 24
CONSISTENT WITH CHANGES MADE UNDER ITEM 3. 6193 1451 25
5. ANISOTROPIC (N,NPRIME) ANGULAR DISTRIBUTIONS BASED ON 6193 1451 26
EXPERIMENTAL DATA WERE INCORPORATED. 6193 1451 27
6. TOTAL NEUTRON CROSS SECTION WAS EXTENSIVELY REVISED, 6193 1451 28
ESPECIALLY BELOW EN=1 MEV, TO INCLUDE THE MEASUREMENT OF 6193 1451 29
PE72. 6193 1451 30
**************************************************************** 6193 1451 31
6193 1451 32
AL-27 FREE ATOM EVAL., NOV.1973, D.G.FOSTER,JR.,P.G.YOUNG (LASL) 6193 1451 33
REFERENCE -- LOS ALAMOS SCIENTIFIC LAB. REPORT LA-4726, (1972) 6193 1451 34
6193 1451 35
MF=2 --- RESONANCE PARAMETERS --- 6193 1451 36
MT=151 EFFECTIVE SCATTERING RADIUS = 0.32752E-12 CM 6193 1451 37
MF=3 6193 1451 38
MT=103 (N,P) CROSS SECTION (SEE YO72 FOR MORE DETAILS) 6193 1451 39
THRES. TO 4 MEV, BASED ON THE MEASUREMENTS OF HE54 AND GR67, 6193 1451 40
EXTRAPOLATED FROM 3 MEV TO THRESHOLD WITH AN L=0 PENETRA- 6193 1451 41
BILITY FUNCTION FOR THE OUTGOING P+MG27 CHANNEL. 6193 1451 42
4 TO 20 MEV, SMOOTH CURVE THROUGH THE MEASUREMENTS OF HE54, 6193 1451 43
GR67, CA62, BA66, MA60. 6193 1451 44
MT=107 (N,ALPHA) CROSS SECTION (SEE YO72 FOR MORE DETAILS). 6193 1451 45
THRES. TO 20 MEV, BASED ON A SMOOTH CURVE THROUGH EXPERI- 6193 1451 46
MENTAL DATA, MAINLY THOSE OF BU63, PA65, AND LI66, WITH 6193 1451 47
RESULTS FROM GR67, SC61, GR58, BA61, MA60, GA62, IM64, 6193 1451 48
KE59 AND SEVERAL 14-MEV POINTS ALSO BEING CONSIDERED. 6193 1451 49
THE CURVE WAS EXTRAPOLATED FROM 6 MEV TO THRESHOLD WITH AN 6193 1451 50
L=0 PENETRABILITY FUNCTION FOR THE OUTGOING ALPHA+NA24 6193 1451 51
CHANNEL. 6193 1451 52
--------------------------- REFERENCES --------------------------6193 1451 53
6193 1451 54
BA58 W.P.BALL ET AL.(LRL), PHYS.REV.110,1392 (1958). 6193 1451 55
BA61 B.P.BAYHURST+R.J.PRESTWOOD (LAS),PHYS.REV.121,1438 (1961). 6193 1451 56
BA66 R.BASS, EANDC(E)-66U,P64, AND PRIVATE COMMUNICATION (1966).6193 1451 57
BA67 G.A.BARTHOLOMEW ET AL., NUCL. DATA A3, 367 (1967) 6193 1451 58
BE55 J.R.BEYSTER ET AL.(LAS), PHYS.REV.98,1216 (1955). 6193 1451 59
BE56 J.R.BEYSTER ET AL.(LAS), PHYS.REV.104,1319 (1956). 6193 1451 60
BE58 S.BERKO ET AL., NUCL. PHYS. 6, 210 (1958) 6193 1451 61
BE66 V.M.BEZOTOSNYI ET AL.(RUS),SOV.J.NUCL.PHYS.3,632 (1966). 6193 1451 62
BL68 R.C.BLOCK, PRIVATE COMMUNICATION TO R.J.HOWERTON (1968) 6193 1451 63
BO59 N.A.BOSTROM ET AL.(TNC), WADC-TN-59-107 (1959). 6193 1451 64
BO65 V.N.BOCHKAREV+V.V.NEFEDOV (LEB),SOV.J.NUCL.PHYS.1,574(1965)6193 1451 65
BO65A G.C.BONAZZOLA ET AL.(TUR), PHYS.REV.140,835 (1965). 6193 1451 66
BU63 J.P.BUTLER AND D.C.SANTRY, CAN.J.PHYS.41, 372 (1963.) 6193 1451 67
CA60 R.L.CALDWELL ET AL.(SOC),NUCL.SCI.ENG.8,173 (1960). 6193 1451 68
CA62 G.CALVI ET AL., NUCL. PHYS. 39, 621 (1962) 6193 1451 69
CA67 A.D.CARLSON AND H.H.BARSCHALL, PHYS. REV. 158, 1142 (1967) 6193 1451 70
CH66 J.P.CHIEN AND A.B.SMITH, NUCL. SCI. ENG. 26, 500 (1966) 6193 1451 71
CH67 A.CHATTERJEE+A.M.GHOSE(BOS), PHYS.REV.161,1181 (1967). 6193 1451 72
CH68 K.C.CHUNG ET AL.(KTY),NUCL.PHYS.68,476 (1968). 6193 1451 73
CI68 S.CIERJACKS ET AL., KFK-1000 (1968) 6193 1451 74
CL69 G.CLAYEUX+G.GRENIER (FR),CEA-R-3807,(1969). 6193 1451 75
CO58 J.H.COON ET AL.(LAS), PHYS.REV. 111,250 (1958). 6193 1451 76
CO59 J.H.COON (LAS),PRIVATE COMMUNICATION TO R.J.HOWERTON (1959)6193 1451 77
DE61 YU.G.DEGTYAREV+V.G.NADTOCHII (RUS), SOV.J.AT.ENERGY 11,10436193 1451 78
(1961). 6193 1451 79
DE65 YU.G.DEGTYAREV (RUS), J.NUCL.ENERGY 20,818 (1965). 6193 1451 80
DI71 J.K.DICKENS (ORL), ORNL-TM-3284, 1971. 6193 1451 81
DI73 J.K.DICKENS ET AL., ORNL-TM-4232 (1973). 6193 1451 82
DR70 D.M.DRAKE ET AL. (LAS), NUCL.SCI.ENG.40,294 (1970). 6193 1451 83
EN67 F.C.ENGESSER+W.E.THOMPSON (NRD),J.NUCL.ENERGY 21,487 (1967)6193 1451 84
FE67 J.M.FERGUSON+J.C.ALBERGOTTI (NRD),NUCL.PHYS.98,65 (1967). 6193 1451 85
FL56 N.N.FLEROV+V.M.TALYZIN (RUS),ATOMNAYA ENERGIYA 1,155 (1956)6193 1451 86
FO71 D.G.FOSTER JR. AND D.W.GLASGOW, PHYS. REV. C 3, 576 (1971) 6193 1451 87
GA62 F.GABBARD+B.D.KERN(KTY), PHYS.REV.128,1276 (1962). 6193 1451 88
GA65 J.B.GARG ET AL., PRIV. COMM. TO R.J.HOWERTON (1965) 6193 1451 89
GL61 R.N.GLOVER+E.WIEGOLD (CBR),NUCL.PHYS.24,630 (1961). 6193 1451 90
GL72 D.W.GLASGOW, PRIVATE COMMUNICATION (1972). 6193 1451 91
GO71 D.T.GOLDMAN, UNPUBLISHED EVALUATION (1971) 6193 1451 92
GR53 E.R.GRAVES+L.ROSEN(LAS),PHYS.REV.89,343 (1953). 6193 1451 93
GR55 E.R.GRAVES+R.W.DAVIS(LAS), PHYS.REV.97, 1205(1955). 6193 1451 94
GR58 J.A.GRUNDL ET AL.(LAS),PHYS.REV.109,425 (1958). 6193 1451 95
GR67 J.A.GRUNDL (LAS), NUCL.SCI.ENG.30,69 (1967). 6193 1451 96
HA69 R.HARDELL ET AL., NUCL.PHYS.A126,392 (1969). 6193 1451 97
HE50 R.L.HENKEL AND H.H.BARSCHALL, PHYS. REV. 80, 145 (1950) 6193 1451 98
HE53 R.L.HENKEL, PRIV. COMM. TO SIGMA CENTER (1953) 6193 1451 99
HI59 C.T.HIBDON, PHYS. REV. 114, 179 (1959) 6193 1451 100
HO69 B.HOLMQVIST+T.WIEDLING (AE), AE-366 (1969). 6193 1451 101
IM64 W.L.IMHOF (LOK),PRIVATE COMMUNICATION TO BNL SIGMA CENTER 6193 1451 102
(1964). 6193 1451 103
JO64 G.D.JOANOU+C.A.STEVENS (GA), GA-5884 (1964). 6193 1451 104
JU71 E.T.JURNEY, PRIVATE COMMUNICATION (1971) 6193 1451 105
KA72 J.L.KAMMERDIENER,THESIS, UNIV.OF CAL.AT DAVIS (1972). 6193 1451 106
KE59 B.D.KERN ET AL.(NRD), NUCL.PHYS.10,226 (1959). 6193 1451 107
KI70 W.E.KINNEY+F.G.PEREY (ORL),ORNL-4516,(1970). 6193 1451 108
LA57 A.LANGSDORF ET AL., PHYS. REV. 107, 1077 (1957) 6193 1451 109
LI66 H.LISKIEN AND A.PAULSEN, NUCLEONICS 8,315 (1966). 6193 1451 110
MA57 M.H.MACGREGOR ET AL.(LRL), PHYS.REV.108,726(1957). 6193 1451 111
MA60 G.S.MANI ET AL.(HAR),NUCL.PHYS.19,535 (1960). 6193 1451 112
MA65 S.C.MATHUR ET AL.(TNC),NUCL.PHYS.73,561 (1965). 6193 1451 113
MA68 G.N.MASLOV ET AL.(RUS),SOV.J.AT.ENERGY 24,704 (1968). 6193 1451 114
MA69 R.E.MAERKER AND F.J.MUCKENTHALER, ORNL-4382 (1969). 6193 1451 115
ME52 A.W.MERRISON AND E.R.WIBLIN, PROC.ROY.SOC.(L) 215,278(1952)6193 1451 116
MI68 A.MITTLER ET AL.(KTY), BULL.AM.PHYS.SOC.13,1420 (1968). 6193 1451 117
OR71 V.J.ORPHAN AND C.G.HOOT, GULF-RT-A10743, (1971). 6193 1451 118
PA65 A.PAULSEN+H.LISKIEN (GEL),J.NUCL.ENERGY 19,907 (1965). 6193 1451 119
PE64 J.L.PERKIN (ALD),NUCL.PHYS.60,561 (1964). 6193 1451 120
PE72 F.G.PEREY ET AL., ORNL-4823 (1972). 6193 1451 121
PH52 D.D.PHILLIPS ET AL.(LAS), PHYS.REV.88,600 (1952). 6193 1451 122
PR60 J.T.PRUDHOMME ET AL.(TNC),AFSWC-TR-60-30 (1960). 6193 1451 123
RA70 N.C.RASMUSSEN ET AL., GA-10248 (1970) 6193 1451 124
SC61 H.W.SCHMITT+J.HALPERIN(ORL),PHYS.REV.121,827 (1961). 6193 1451 125
SC70 R.B.SCHWARTZ, PRIVATE COMMUNICATION (1970) 6193 1451 126
ST59 C.ST.PIERRE ET AL.(MON), PHYS.REV.115,999 (1959). 6193 1451 127
ST62 T.P.STUART ET AL., PHYS. REV. 125, 276 (1962) 6193 1451 128
ST65 P.H.STELSON+R.L.ROBINSON (ORL), NUCL.PHYS.68,97 (1965). 6193 1451 129
TA55 H.L.TAYLOR ET AL.(RIC), PHYS.REV.100,174 (1955). 6193 1451 130
TA70 S.TANAKA ET AL., NUCL.DATA FOR REACTORS (IAEA,1970),P317. 6193 1451 131
TH63 D.B.THOMPSON (LAS),PHYS.REV.129,1649 (1963). 6193 1451 132
TO62 J.H.TOWLE AND W.B.GILBOY, NUCL. PHYS. 39, 300 (1962) 6193 1451 133
TO67 J.H.TOWLE+R.O.OWENS(ALD),NUCL.PHYS.A100,257 (1967). 6193 1451 134
TS61 K.TSUKADA ET AL., PHYSICS OF FAST AND INTERMEDIATE 6193 1451 135
REACTORS, VIENNA (1961). 6193 1451 136
WI63 D.WINTERHALTER (ZAG), NUCL.PHYS.43,339(1963). 6193 1451 137
YO72 P.G.YOUNG, LASL MEMO T-2-99 TO THE NORM. AND STANDARDS 6193 1451 138
SUBCOMMITTEE OF CSEWG, (1972). 6193 1451 139
THIS MATERIAL HAS BEEN PROCESSED BY INTEND 6193 1451 140
1 451 144 6193 1451 141
2 151 4 6193 1451 142
3 103 210 6193 1451 143
3 107 210 6193 1451 144
6193 1 0 145
6193 0 0 146
1.30270+ 4 2.67500+ 1 0 0 1 06193 2151 147
1.30270+ 4 1.00000+ 0 0 0 1 06193 2151 148
1.00000- 5 1.00000+ 3 0 0 0 06193 2151 149
2.50000+ 0 3.27520- 1 0 0 0 06193 2151 150
6193 2 0 151
6193 0 0 152
1.30270+ 4 2.67500+ 1 0 99 0 06193 3103 153
0.00000+ 0-1.82780+ 6 0 0 1 6216193 3103 154
621 1 6193 3103 155
1.00000- 4 0.00000+ 0 1.05000- 4 0.00000+ 0 1.10000- 4 0.00000+ 06193 3103 156
1.15000- 4 0.00000+ 0 1.20000- 4 0.00000+ 0 1.27500- 4 0.00000+ 06193 3103 157
1.35000- 4 0.00000+ 0 1.42500- 4 0.00000+ 0 1.50000- 4 0.00000+ 06193 3103 158
1.60000- 4 0.00000+ 0 1.70000- 4 0.00000+ 0 1.80000- 4 0.00000+ 06193 3103 159
1.90000- 4 0.00000+ 0 2.00000- 4 0.00000+ 0 2.10000- 4 0.00000+ 06193 3103 160
2.20000- 4 0.00000+ 0 2.30000- 4 0.00000+ 0 2.40000- 4 0.00000+ 06193 3103 161
2.55000- 4 0.00000+ 0 2.70000- 4 0.00000+ 0 2.80000- 4 0.00000+ 06193 3103 162
3.00000- 4 0.00000+ 0 3.20000- 4 0.00000+ 0 3.40000- 4 0.00000+ 06193 3103 163
3.60000- 4 0.00000+ 0 3.80000- 4 0.00000+ 0 4.00000- 4 0.00000+ 06193 3103 164
4.25000- 4 0.00000+ 0 4.50000- 4 0.00000+ 0 4.75000- 4 0.00000+ 06193 3103 165
5.00000- 4 0.00000+ 0 5.25000- 4 0.00000+ 0 5.50000- 4 0.00000+ 06193 3103 166
5.75000- 4 0.00000+ 0 6.00000- 4 0.00000+ 0 6.30000- 4 0.00000+ 06193 3103 167
6.60000- 4 0.00000+ 0 6.90000- 4 0.00000+ 0 7.20000- 4 0.00000+ 06193 3103 168
7.60000- 4 0.00000+ 0 8.00000- 4 0.00000+ 0 8.40000- 4 0.00000+ 06193 3103 169
8.80000- 4 0.00000+ 0 9.20000- 4 0.00000+ 0 9.60000- 4 0.00000+ 06193 3103 170
1.00000- 3 0.00000+ 0 1.05000- 3 0.00000+ 0 1.10000- 3 0.00000+ 06193 3103 171
1.15000- 3 0.00000+ 0 1.20000- 3 0.00000+ 0 1.27500- 3 0.00000+ 06193 3103 172
1.35000- 3 0.00000+ 0 1.42500- 3 0.00000+ 0 1.50000- 3 0.00000+ 06193 3103 173
1.60000- 3 0.00000+ 0 1.70000- 3 0.00000+ 0 1.80000- 3 0.00000+ 06193 3103 174
1.90000- 3 0.00000+ 0 2.00000- 3 0.00000+ 0 2.10000- 3 0.00000+ 06193 3103 175
2.20000- 3 0.00000+ 0 2.30000- 3 0.00000+ 0 2.40000- 3 0.00000+ 06193 3103 176
2.55000- 3 0.00000+ 0 2.70000- 3 0.00000+ 0 2.80000- 3 0.00000+ 06193 3103 177
3.00000- 3 0.00000+ 0 3.20000- 3 0.00000+ 0 3.40000- 3 0.00000+ 06193 3103 178
3.60000- 3 0.00000+ 0 3.80000- 3 0.00000+ 0 4.00000- 3 0.00000+ 06193 3103 179
4.25000- 3 0.00000+ 0 4.50000- 3 0.00000+ 0 4.75000- 3 0.00000+ 06193 3103 180
5.00000- 3 0.00000+ 0 5.25000- 3 0.00000+ 0 5.50000- 3 0.00000+ 06193 3103 181
5.75000- 3 0.00000+ 0 6.00000- 3 0.00000+ 0 6.30000- 3 0.00000+ 06193 3103 182
6.60000- 3 0.00000+ 0 6.90000- 3 0.00000+ 0 7.20000- 3 0.00000+ 06193 3103 183
7.60000- 3 0.00000+ 0 8.00000- 3 0.00000+ 0 8.40000- 3 0.00000+ 06193 3103 184
8.80000- 3 0.00000+ 0 9.20000- 3 0.00000+ 0 9.60000- 3 0.00000+ 06193 3103 185
1.00000- 2 0.00000+ 0 1.05000- 2 0.00000+ 0 1.10000- 2 0.00000+ 06193 3103 186
1.15000- 2 0.00000+ 0 1.20000- 2 0.00000+ 0 1.27500- 2 0.00000+ 06193 3103 187
1.35000- 2 0.00000+ 0 1.42500- 2 0.00000+ 0 1.50000- 2 0.00000+ 06193 3103 188
1.60000- 2 0.00000+ 0 1.70000- 2 0.00000+ 0 1.80000- 2 0.00000+ 06193 3103 189
1.90000- 2 0.00000+ 0 2.00000- 2 0.00000+ 0 2.10000- 2 0.00000+ 06193 3103 190
2.20000- 2 0.00000+ 0 2.30000- 2 0.00000+ 0 2.40000- 2 0.00000+ 06193 3103 191
2.55000- 2 0.00000+ 0 2.70000- 2 0.00000+ 0 2.80000- 2 0.00000+ 06193 3103 192
3.00000- 2 0.00000+ 0 3.20000- 2 0.00000+ 0 3.40000- 2 0.00000+ 06193 3103 193
3.60000- 2 0.00000+ 0 3.80000- 2 0.00000+ 0 4.00000- 2 0.00000+ 06193 3103 194
4.25000- 2 0.00000+ 0 4.50000- 2 0.00000+ 0 4.75000- 2 0.00000+ 06193 3103 195
5.00000- 2 0.00000+ 0 5.25000- 2 0.00000+ 0 5.50000- 2 0.00000+ 06193 3103 196
5.75000- 2 0.00000+ 0 6.00000- 2 0.00000+ 0 6.30000- 2 0.00000+ 06193 3103 197
6.60000- 2 0.00000+ 0 6.90000- 2 0.00000+ 0 7.20000- 2 0.00000+ 06193 3103 198
7.60000- 2 0.00000+ 0 8.00000- 2 0.00000+ 0 8.40000- 2 0.00000+ 06193 3103 199
8.80000- 2 0.00000+ 0 9.20000- 2 0.00000+ 0 9.60000- 2 0.00000+ 06193 3103 200
1.00000- 1 0.00000+ 0 1.05000- 1 0.00000+ 0 1.10000- 1 0.00000+ 06193 3103 201
1.15000- 1 0.00000+ 0 1.20000- 1 0.00000+ 0 1.27500- 1 0.00000+ 06193 3103 202
1.35000- 1 0.00000+ 0 1.42500- 1 0.00000+ 0 1.50000- 1 0.00000+ 06193 3103 203
1.60000- 1 0.00000+ 0 1.70000- 1 0.00000+ 0 1.80000- 1 0.00000+ 06193 3103 204
1.90000- 1 0.00000+ 0 2.00000- 1 0.00000+ 0 2.10000- 1 0.00000+ 06193 3103 205
2.20000- 1 0.00000+ 0 2.30000- 1 0.00000+ 0 2.40000- 1 0.00000+ 06193 3103 206
2.55000- 1 0.00000+ 0 2.70000- 1 0.00000+ 0 2.80000- 1 0.00000+ 06193 3103 207
3.00000- 1 0.00000+ 0 3.20000- 1 0.00000+ 0 3.40000- 1 0.00000+ 06193 3103 208
3.60000- 1 0.00000+ 0 3.80000- 1 0.00000+ 0 4.00000- 1 0.00000+ 06193 3103 209
4.25000- 1 0.00000+ 0 4.50000- 1 0.00000+ 0 4.75000- 1 0.00000+ 06193 3103 210
5.00000- 1 0.00000+ 0 5.25000- 1 0.00000+ 0 5.50000- 1 0.00000+ 06193 3103 211
5.75000- 1 0.00000+ 0 6.00000- 1 0.00000+ 0 6.30000- 1 0.00000+ 06193 3103 212
6.60000- 1 0.00000+ 0 6.90000- 1 0.00000+ 0 7.20000- 1 0.00000+ 06193 3103 213
7.60000- 1 0.00000+ 0 8.00000- 1 0.00000+ 0 8.40000- 1 0.00000+ 06193 3103 214
8.80000- 1 0.00000+ 0 9.20000- 1 0.00000+ 0 9.60000- 1 0.00000+ 06193 3103 215
1.00000+ 0 0.00000+ 0 1.05000+ 0 0.00000+ 0 1.10000+ 0 0.00000+ 06193 3103 216
1.15000+ 0 0.00000+ 0 1.20000+ 0 0.00000+ 0 1.27500+ 0 0.00000+ 06193 3103 217
1.35000+ 0 0.00000+ 0 1.42500+ 0 0.00000+ 0 1.50000+ 0 0.00000+ 06193 3103 218
1.60000+ 0 0.00000+ 0 1.70000+ 0 0.00000+ 0 1.80000+ 0 0.00000+ 06193 3103 219
1.90000+ 0 0.00000+ 0 2.00000+ 0 0.00000+ 0 2.10000+ 0 0.00000+ 06193 3103 220
2.20000+ 0 0.00000+ 0 2.30000+ 0 0.00000+ 0 2.40000+ 0 0.00000+ 06193 3103 221
2.55000+ 0 0.00000+ 0 2.70000+ 0 0.00000+ 0 2.80000+ 0 0.00000+ 06193 3103 222
3.00000+ 0 0.00000+ 0 3.20000+ 0 0.00000+ 0 3.40000+ 0 0.00000+ 06193 3103 223
3.60000+ 0 0.00000+ 0 3.80000+ 0 0.00000+ 0 4.00000+ 0 0.00000+ 06193 3103 224
4.25000+ 0 0.00000+ 0 4.50000+ 0 0.00000+ 0 4.75000+ 0 0.00000+ 06193 3103 225
5.00000+ 0 0.00000+ 0 5.25000+ 0 0.00000+ 0 5.50000+ 0 0.00000+ 06193 3103 226
5.75000+ 0 0.00000+ 0 6.00000+ 0 0.00000+ 0 6.30000+ 0 0.00000+ 06193 3103 227
6.60000+ 0 0.00000+ 0 6.90000+ 0 0.00000+ 0 7.20000+ 0 0.00000+ 06193 3103 228
7.60000+ 0 0.00000+ 0 8.00000+ 0 0.00000+ 0 8.40000+ 0 0.00000+ 06193 3103 229
8.80000+ 0 0.00000+ 0 9.20000+ 0 0.00000+ 0 9.60000+ 0 0.00000+ 06193 3103 230
1.00000+ 1 0.00000+ 0 1.05000+ 1 0.00000+ 0 1.10000+ 1 0.00000+ 06193 3103 231
1.15000+ 1 0.00000+ 0 1.20000+ 1 0.00000+ 0 1.27500+ 1 0.00000+ 06193 3103 232
1.35000+ 1 0.00000+ 0 1.42500+ 1 0.00000+ 0 1.50000+ 1 0.00000+ 06193 3103 233
1.60000+ 1 0.00000+ 0 1.70000+ 1 0.00000+ 0 1.80000+ 1 0.00000+ 06193 3103 234
1.90000+ 1 0.00000+ 0 2.00000+ 1 0.00000+ 0 2.10000+ 1 0.00000+ 06193 3103 235
2.20000+ 1 0.00000+ 0 2.30000+ 1 0.00000+ 0 2.40000+ 1 0.00000+ 06193 3103 236
2.55000+ 1 0.00000+ 0 2.70000+ 1 0.00000+ 0 2.80000+ 1 0.00000+ 06193 3103 237
3.00000+ 1 0.00000+ 0 3.20000+ 1 0.00000+ 0 3.40000+ 1 0.00000+ 06193 3103 238
3.60000+ 1 0.00000+ 0 3.80000+ 1 0.00000+ 0 4.00000+ 1 0.00000+ 06193 3103 239
4.25000+ 1 0.00000+ 0 4.50000+ 1 0.00000+ 0 4.75000+ 1 0.00000+ 06193 3103 240
5.00000+ 1 0.00000+ 0 5.25000+ 1 0.00000+ 0 5.50000+ 1 0.00000+ 06193 3103 241
5.75000+ 1 0.00000+ 0 6.00000+ 1 0.00000+ 0 6.30000+ 1 0.00000+ 06193 3103 242
6.60000+ 1 0.00000+ 0 6.90000+ 1 0.00000+ 0 7.20000+ 1 0.00000+ 06193 3103 243
7.60000+ 1 0.00000+ 0 8.00000+ 1 0.00000+ 0 8.40000+ 1 0.00000+ 06193 3103 244
8.80000+ 1 0.00000+ 0 9.20000+ 1 0.00000+ 0 9.60000+ 1 0.00000+ 06193 3103 245
1.00000+ 2 0.00000+ 0 1.05000+ 2 0.00000+ 0 1.10000+ 2 0.00000+ 06193 3103 246
1.15000+ 2 0.00000+ 0 1.20000+ 2 0.00000+ 0 1.27500+ 2 0.00000+ 06193 3103 247
1.35000+ 2 0.00000+ 0 1.42500+ 2 0.00000+ 0 1.50000+ 2 0.00000+ 06193 3103 248
1.60000+ 2 0.00000+ 0 1.70000+ 2 0.00000+ 0 1.80000+ 2 0.00000+ 06193 3103 249
1.90000+ 2 0.00000+ 0 2.00000+ 2 0.00000+ 0 2.10000+ 2 0.00000+ 06193 3103 250
2.20000+ 2 0.00000+ 0 2.30000+ 2 0.00000+ 0 2.40000+ 2 0.00000+ 06193 3103 251
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