ENTRY 20146 20191116 22832014600000001
SUBENT 20146001 20191116 22832014600100001
BIB 15 53 2014600100002
TITLE Statistical properties of 45-Rh-104 level parameters 2014600100003
AUTHOR (P.Ribon, J.Girard, J.Trochon) 2014600100004
REFERENCE (J,NP/A,143,130,1970) (in French) Reson. parameters. 2014600100005
For Rh sig(tot) see priv.comm. Ribon 1961-1966 2014600100006
(see REL-REF) 2014600100007
(S,EANDC-50-S,(2),(165),1965) res.pars. until 760 eV. 2014600100008
Abstract was publ. in 65ANTWERP,,565(165),1965 2014600100009
(J,JPR,24,987,1963) - prelim. results 2014600100010
(J,CR,254,2546,1962) Strength function, until 370 eV, 2014600100011
superseded. 2014600100012
INSTITUTE (2FR SAC) 2014600100013
FACILITY (LINAC,2FR SAC) 45 MeV Saclay electron linear 2014600100014
accelerator. 2014600100015
INC-SOURCE (PHOTO) Photo-neutrons. 2014600100016
REL-REF (O,20148001,P.Ribon,R,CEA-N-1149,1969)) Rh exp. 2014600100017
details, cr.sections, res.pars same as NP/A,143,130. 2014600100018
(R,,B.N.Brockhouse,J,CJP,31,432,1953) - The resonance 2014600100019
parameters at 1.257 eV 2014600100020
(R,,D.I.Garber+,R,BNL-325,1957) Supplement Number 2. 2014600100021
- The resonance parameters at 1.257 eV 2014600100022
SAMPLE .Powder for transmission. 2014600100023
.Thin metal plate for scattering. 2014600100024
.Transmission in the energy range of 627 to 4216 eV 2014600100025
was done at 77 deg-K, others were at 293 deg-K. 2014600100026
METHOD (TOF,TRN) Time of flight, flight path = 53.7 and 2014600100027
103.7 m for transmission, and 32.7 m for scattering. 2014600100028
DETECTOR (SCIN) Boron 1 to 2 cm thick and 6 Na-I crystals 2014600100029
(dia 125 mm, height 50 mm) for transmission. 2014600100030
- Boron loaded liquid scintillator for 2014600100031
scattering. 2014600100032
ANALYSIS (SHAPE) Shape analysis on normalized transmission 2014600100033
data. For details see CEA-N-1149. 2014600100034
COMMENT .The resonance at 1.257 eV was not analyzed by author 2014600100035
but used for the averaged resonance parameters. 2014600100036
The following values were taken (see REL-REF): 2014600100037
Resonance parameters +- error in per-cent, 2014600100038
gamma 2g*gamma(n) gamma(gamma) spin momentum l2014600100039
156.+-3. 0.7800+-1.2 155.+-3. 1. 0. 2014600100040
.One resonance energy and 3 gamma(tot) error values 2014600100041
were misprinted. (Oral priv.comm. from Ribon). 2014600100042
STATUS (APRVD) approved by Ribon. 2014600100043
ERR-ANALYS (DATA-ERR) Standard deviation but at least doubled to 2014600100044
take into account errors on the parameters (such as 2014600100045
resolution, Doppler effect, ... ) introduced in the 2014600100046
analysis. 2014600100047
* Systematic errors were extensively discussed in 2014600100048
CEA-N-1149. 2014600100049
HISTORY (19711027C) 2014600100050
(20170424A) SD:Updated to new date formats,lower case. 2014600100051
Ref. syntax was corrected. Ref. CEA-N-1149 moved to 2014600100052
REL-REF. 2014600100053
(20191116U) SD: Ref. JPR,24,987,1963 added. 2014600100054
Ref. 65ANTWERP,525(72) deleted (only abstract). 2014600100055
ENDBIB 53 0 2014600100056
NOCOMMON 0 0 2014600100057
ENDSUBENT 56 0 2014600199999
SUBENT 20146002 20170424 22612014600200001
BIB 4 10 2014600200002
REACTION (45-RH-103(N,G),,WID) 2014600200003
FLAG (1.) Study was difficult or impossible because 2014600200004
of the presence of a near-by resonance. 2014600200005
(2.) Resonance level can be double because the 2014600200006
(gamma-width) is very large. 2014600200007
(3.) The value of (gamma-width) is probable. 2014600200008
STATUS (TABLE) Tbl.4 from Nucl.Phys. A143(1970)130. 2014600200009
HISTORY (20170424A) SD: STATUS was added. Data were update 2014600200010
according presentation in the Tbl. (meaningless zeros 2014600200011
from right side of the values were deleted). 2014600200012
ENDBIB 10 0 2014600200013
NOCOMMON 0 0 2014600200014
DATA 4 123 2014600200015
EN-RES DATA DATA-ERR FLAG 2014600200016
EV MILLI-EV PER-CENT NO-DIM 2014600200017
34.41 151. 8. 2014600200018
46.85 174. 7. 2014600200019
68.34 167. 5. 2014600200020
83.54 157. 50. 2014600200021
95.78 166. 6. 2014600200022
98.82 178. 11. 2014600200023
108.88 100. 80. 2014600200024
110.88 169. 8. 1. 2014600200025
114.08 175. 11. 2014600200026
125.62 168. 3. 2014600200027
154.31 191. 4. 2014600200028
179.43 174. 12. 2014600200029
187.23 172. 4. 2014600200030
199.83 600. 50. 2. 2014600200031
205.15 180. 60. 2014600200032
254.04 178. 7. 2014600200033
263.28 218. 25. 1. 2014600200034
272.40 174. 7. 2014600200035
290.06 159. 6. 2014600200036
312.76 220. 55. 2014600200037
319.88 177. 5. 2014600200038
327.76 184. 35. 2014600200039
362.78 104. 91. 2014600200040
366.55 132. 21. 2014600200041
374.28 164. 50. 2014600200042
388.94 130. 80. 2014600200043
406.48 183. 7. 2014600200044
435.74 194. 10. 2014600200045
450.34 145. 30. 2014600200046
473.15 78. 92. 2. 2014600200047
486.81 31. 99. 1. 2014600200048
492.42 161. 30. 2014600200049
505.15 89. 96. 2014600200050
526.44 109. 81. 2014600200051
555.79 174. 7. 2014600200052
582.07 151. 26. 2014600200053
605.20 96. 83. 1. 2014600200054
621.12 380. 31. 2. 2014600200055
646.62 164. 19. 2014600200056
663.90 184. 25. 2014600200057
676.93 127. 62. 2014600200058
683.82 109. 58. 2014600200059
692.46 160. 24. 2014600200060
702.33 183. 12. 2014600200061
760.15 95. 99. 2014600200062
783.16 187. 18. 3. 2014600200063
797.08 262. 40. 2014600200064
831.36 192. 61. 2014600200065
845.77 170. 11. 2014600200066
895.58 129. 63. 2014600200067
914.49 149. 20. 2014600200068
930.04 148. 16. 2014600200069
955.71 204. 25. 2014600200070
1025.0 186. 82. 2014600200071
1077.1 173. 44. 2014600200072
1111.0 157. 26. 3. 2014600200073
1154.9 243. 18. 2014600200074
1190.4 177. 30. 3. 2014600200075
1196.7 224. 30. 2014600200076
1245.7 172. 83. 2014600200077
1272.4 185. 15. 2014600200078
1306.9 154. 20. 2014600200079
1326.0 173. 32. 3. 2014600200080
1365.5 184. 25. 2014600200081
1408.0 233. 40. 3. 2014600200082
1433.7 84. 99. 2014600200083
1487.1 156. 90. 2014600200084
1531.9 185. 97. 2014600200085
1544.0 122. 50. 2014600200086
1561.6 109. 99. 2014600200087
1567.7 138. 30. 2014600200088
1620.2 187. 20. 2014600200089
1671.4 80. 80. 2014600200090
1697.6 279. 14. 2014600200091
1737.0 123. 99. 2014600200092
1766.2 173. 77. 2014600200093
1796.3 195. 36. 2014600200094
1820.8 316. 17. 2. 2014600200095
1843.4 60. 99. 2014600200096
1905.1 149. 95. 2014600200097
1982.9 285. 30. 2014600200098
2010.2 99. 99. 2014600200099
2060.2 244. 38. 2014600200100
2102.4 164. 99. 2014600200101
2115.8 110. 75. 2014600200102
2179.8 57. 99. 2014600200103
2195.2 139. 50. 2014600200104
2260.2 261. 57. 3. 2014600200105
2296.7 273. 22. 2014600200106
2315.8 171. 98. 2014600200107
2333.1 1178. 27. 2. 2014600200108
2380.0 190. 95. 2014600200109
2410.1 507. 95. 2014600200110
2416.8 98. 98. 2014600200111
2434.1 810. 33. 2. 2014600200112
2461.4 273. 32. 2014600200113
2596.8 454. 99. 2014600200114
2606.0 157. 55. 2014600200115
2630.4 194. 55. 2014600200116
2668.9 1816. 47. 2. 2014600200117
2721.7 169. 99. 2014600200118
2793.3 43. 99. 2014600200119
2858.1 282. 95. 2014600200120
2881.7 310. 98. 2014600200121
2952.8 2210. 36. 2. 2014600200122
2998.8 160. 95. 2014600200123
3030.4 285. 48. 2014600200124
3084.3 107. 95. 2014600200125
3131.6 257. 40. 2014600200126
3168.6 161. 99. 2014600200127
3272.9 300. 90. 2014600200128
3305.0 394. 78. 3. 2014600200129
3396.2 220. 90. 2014600200130
3492.0 234. 90. 2014600200131
3512.5 237. 50. 2014600200132
3553.7 207. 55. 2014600200133
3597.2 305. 73. 3. 2014600200134
3646.2 52. 99. 2014600200135
3687.5 80. 99. 2014600200136
3853.8 960. 63. 3. 2014600200137
4059.4 1540. 42. 3. 2014600200138
4079.9 36. 99. 2014600200139
4140.3 30. 99. 2014600200140
ENDDATA 125 0 2014600200141
ENDSUBENT 140 0 2014600299999
SUBENT 20146003 20170424 22612014600300001
BIB 4 6 2014600300002
REACTION (45-RH-103(N,G),,WID,,AV) 2014600300003
ANALYSIS .For 27 resonances with errors less than 20%. 2014600300004
STATUS (TABLE) From the text on p.149 of 2014600300005
Nucl.Phys. A143(1970)130. 2014600300006
HISTORY (20170424A) SD: Meaningless zeros from right side of 2014600300007
the values were deleted. 2014600300008
ENDBIB 6 0 2014600300009
NOCOMMON 0 0 2014600300010
DATA 4 1 2014600300011
EN-MAX EN-MIN DATA DATA-ERR 2014600300012
MEV MEV MILLI-EV MILLI-EV 2014600300013
4.140E-03 1.2E-06 171. 3. 2014600300014
ENDDATA 3 0 2014600300015
ENDSUBENT 14 0 2014600399999
SUBENT 20146004 20170424 22612014600400001
BIB 4 8 2014600400002
REACTION (45-RH-103(N,EL),,WID,,2G) 2014600400003
FLAG (1.) Study was difficult or impossible because 2014600400004
of the presence of a near-by resonance. 2014600400005
(2.) Resonance level can be double because the 2014600400006
(gamma-width) is very large. 2014600400007
STATUS (TABLE) Tbl.4 from Nucl. Phys. A143(1970)130. 2014600400008
HISTORY (20170424A) SD: Meaningless zeros from right side of 2014600400009
the values were deleted. 2014600400010
ENDBIB 8 0 2014600400011
NOCOMMON 0 0 2014600400012
DATA 4 273 2014600400013
EN-RES DATA DATA-ERR FLAG 2014600400014
EV MILLI-EV PER-CENT NO-DIM 2014600400015
34.41 0.0238 2. 2014600400016
44.49 0.0058 10. 2014600400017
46.85 0.760 6. 2014600400018
51.85 0.002 60. 2014600400019
68.34 0.2960 2. 2014600400020
83.54 0.0159 12. 2014600400021
95.78 3.6200 4. 2014600400022
98.82 0.1074 3.5 2014600400023
108.88 0.0170 16. 2014600400024
110.88 0.253 2.6 1. 2014600400025
114.08 0.166 3.5 2014600400026
125.62 11.10 2.5 2014600400027
154.31 98.15 1.5 2014600400028
179.43 0.270 3. 2014600400029
187.23 57.5 2.3 2014600400030
199.83 0.095 13. 2. 2014600400031
205.15 0.150 6. 2014600400032
251.37 0.230 10. 1. 2014600400033
254.04 53.0 2. 2014600400034
263.28 2.02 6. 1. 2014600400035
264.38 0.82 8. 1. 2014600400036
272.40 88.7 2. 2014600400037
290.06 29.1 2.4 2014600400038
312.76 0.290 10. 2014600400039
316.46 0.060 35. 1. 2014600400040
319.88 140.0 2. 2014600400041
321.79 1.95 22. 1. 2014600400042
327.76 1.17 6. 2014600400043
354.13 0.182 14. 2014600400044
362.78 0.630 5.5 2014600400045
366.55 3.3 4. 2014600400046
374.28 0.800 6.5 2014600400047
376.70 0.250 14. 1. 2014600400048
388.94 0.440 9. 2014600400049
406.48 14.90 3. 2014600400050
427.95 0.185 14. 2014600400051
433.08 2.08 13. 1. 2014600400052
435.74 308. 2. 2014600400053
444.27 0.46 16. 2014600400054
447.52 0.27 21. 2014600400055
450.34 6.29 7. 2014600400056
473.15 1.80 6. 2. 2014600400057
486.81 1.90 5.5 1. 2014600400058
489.56 0.31 15. 2014600400059
492.42 4.55 4.5 2014600400060
505.15 0.88 10. 2014600400061
526.44 1.23 6.5 2014600400062
547.25 0.17 30. 2014600400063
555.79 140.7 2.3 2014600400064
582.07 4.45 5. 2014600400065
602.94 0.60 15. 2014600400066
605.20 3.95 5. 1. 2014600400067
608.10 0.31 22. 2014600400068
621.12 10.3 7. 2. 2014600400069
645.09 1.67 28. 1. 2014600400070
646.62 98.5 4. 2014600400071
663.90 10.7 6.5 2014600400072
676.93 4.05 6. 2014600400073
683.82 5.65 6. 2014600400074
692.46 128.2 4. 2014600400075
699.15 2.5 20. 1. 2014600400076
702.33 430. 2.5 2014600400077
727.73 1.40 15. 2014600400078
742.17 3.57 9. 2014600400079
758.15 1.41 25. 2014600400080
760.15 5.0 12. 2014600400081
783.16 31.0 5.5 2014600400082
797.08 5.82 20. 2014600400083
828.10 0.35 50. 2014600400084
831.36 4.76 8. 2014600400085
845.77 230. 3.5 2014600400086
868.71 1.04 20. 2014600400087
886.04 0.933 20. 2014600400088
895.58 13.3 11. 2014600400089
914.49 74.5 5. 2014600400090
930.04 88.2 5. 2014600400091
955.71 39.2 6.5 2014600400092
990.77 1.39 20. 2014600400093
1002.0 2.04 15. 2014600400094
1008.0 0.50 70. 2014600400095
1025.0 4.45 10. 2014600400096
1028.4 3.66 10. 2014600400097
1066.4 0.60 60. 2014600400098
1071.9 1.20 24. 2014600400099
1077.1 16.9 7. 2014600400100
1082.8 1.28 22. 2014600400101
1093.4 1.06 27. 2014600400102
1100.0 1.54 20. 2014600400103
1111.0 43.4 5. 2014600400104
1122.6 0.80 40. 2014600400105
1152.0 1.93 30. 2014600400106
1154.9 153. 5. 2014600400107
1190.4 50.6 6.5 2014600400108
1196.7 300. 5.5 2014600400109
1201.9 5.45 20. 2014600400110
1205.4 1.7 33. 2014600400111
1212.4 4.37 14. 2014600400112
1245.7 7.50 8. 2014600400113
1261.5 1.70 20. 2014600400114
1272.4 600. 3.5 2014600400115
1276.5 5. 70. 1. 2014600400116
1278.8 9.4 20. 1. 2014600400117
1287.0 5. 15. 1. 2014600400118
1306.9 142.5 5.5 2014600400119
1326.0 57.2 7. 2014600400120
1355.1 3.4 17. 2014600400121
1365.5 84. 6. 2014600400122
1380.8 5.03 14. 2014600400123
1393.6 6.17 12. 2014600400124
1408.0 46.8 8. 2014600400125
1410.9 4.8 21. 1. 2014600400126
1433.7 16.3 10. 2014600400127
1453.7 4.95 14. 2014600400128
1464.5 1.17 40. 2014600400129
1483.5 16.3 12. 2014600400130
1487.1 57. 19. 2014600400131
1513.6 1.4 40. 2014600400132
1531.9 15.1 9. 2014600400133
1544. 254. 5.5 2014600400134
1552.6 9.1 14. 2014600400135
1561.6 22.8 10. 2014600400136
1567.7 198. 6.5 2014600400137
1614.3 3.8 20. 2014600400138
1620.2 414. 4.5 2014600400139
1650.2 2.4 30. 2014600400140
1665.6 5.5 17. 2014600400141
1671.4 86.5 7. 2014600400142
1697.6 437. 4.5 2014600400143
1712.5 2.5 40. 2014600400144
1737.0 27.3 11. 2014600400145
1751.5 2.15 40. 2014600400146
1766.2 31.1 10. 2014600400147
1784.5 5.3 19. 2014600400148
1796.3 127. 8. 2014600400149
1806.0 2.1 50. 2014600400150
1820.8 668. 5. 2. 2014600400151
1832.0 1.8 80. 2014600400152
1837.2 8.7 22. 2014600400153
1843.4 90. 10. 2014600400154
1849.2 4.6 30. 2014600400155
1885.2 3.5 30. 2014600400156
1892.4 3.6 30. 2014600400157
1905.1 35. 11. 2014600400158
1920.4 7.0 18. 2014600400159
1941.8 12.1 14. 2014600400160
1954.2 8.6 16. 2014600400161
1967.3 5.2 22. 2014600400162
1982.9 268. 5.5 2014600400163
1996.7 4.6 30. 2014600400164
2010.2 29. 12. 2014600400165
2021.9 2.9 47. 2014600400166
2034.5 2. 60. 2014600400167
2039.9 7.1 18. 2014600400168
2060.2 98. 7.5 2014600400169
2082.5 8.3 17. 2014600400170
2085.9 35.1 10. 2014600400171
2102.4 39.0 12. 2014600400172
2115.8 232. 7. 2014600400173
2151.7 5.1 30. 2014600400174
2161.9 27.5 12. 2014600400175
2179.8 59.5 13. 2014600400176
2195.2 182. 8. 2014600400177
2244.5 20. 15. 2014600400178
2249.0 13.4 18. 2014600400179
2260.2 76.5 12. 2014600400180
2278.5 2.66 54. 2014600400181
2296.7 580. 5.5 2014600400182
2315.8 75.7 13. 2014600400183
2333.1 91.6 10. 2. 2014600400184
2355.6 10.9 21. 2014600400185
2365.9 28.7 15. 2014600400186
2380.0 90. 13. 2014600400187
2395.8 16.3 20. 2014600400188
2410.1 28. 18. 2014600400189
2416.8 191. 11. 2014600400190
2434.1 90. 13. 2. 2014600400191
2461.4 385. 8.5 2014600400192
2479.3 3.2 70. 2014600400193
2510.9 7.1 34. 2014600400194
2516.8 16.7 21. 2014600400195
2530.1 11. 26. 2014600400196
2536.3 24.2 19. 2014600400197
2549.5 28.4 18. 2014600400198
2596.8 49.2 15. 2014600400199
2606.0 613. 8. 2014600400200
2630.4 330. 9. 2014600400201
2656.9 22.8 27. 2014600400202
2661.4 19.7 29. 2014600400203
2668.9 84. 12. 2. 2014600400204
2695.6 13.6 29. 2014600400205
2701.5 41.0 20. 2014600400206
2721.7 137. 15. 2014600400207
2731.1 62. 22. 2014600400208
2740.8 30. 23. 2014600400209
2763.4 17. 25. 2014600400210
2787.0 9. 40. 2014600400211
2793.3 260. 10. 2014600400212
2816.5 3. 60. 2014600400213
2843.1 8.8 40. 2014600400214
2850.4 24. 24. 2014600400215
2858.1 174. 14. 2014600400216
2871.8 10. 60. 2014600400217
2881.7 100. 16. 2014600400218
2887.5 11. 44. 2014600400219
2891.5 6. 60. 2014600400220
2902.4 12. 33. 2014600400221
2916.8 19. 22. 2014600400222
2952.8 90. 11. 2. 2014600400223
2968.0 25. 30. 1. 2014600400224
2973.0 48. 19. 1. 2014600400225
2983.9 79. 32. 2014600400226
2998.8 185. 13. 2014600400227
3030.4 255. 10. 2014600400228
3049.6 43. 19. 2014600400229
3063.7 87. 17. 2014600400230
3075.3 10. 40. 2014600400231
3084.3 340. 10. 2014600400232
3113.0 5. 50. 2014600400233
3131.6 575. 8. 2014600400234
3140.5 22. 30. 2014600400235
3156.2 38. 24. 2014600400236
3168.6 99. 20. 2014600400237
3191.7 30. 25. 2014600400238
3198.3 12. 40. 2014600400239
3212.3 7. 45. 2014600400240
3227.5 20. 28. 2014600400241
3257.7 9. 45. 2014600400242
3264.0 10. 45. 2014600400243
3272.9 293. 10. 2014600400244
3286.2 7. 50. 2014600400245
3305.0 141. 17. 2014600400246
3323.2 95. 18. 2014600400247
3330.0 5. 70. 2014600400248
3354.1 75. 19. 2014600400249
3361.0 14. 37. 2014600400250
3396.2 754. 7. 2014600400251
3413.7 25. 40. 2014600400252
3439.7 50. 20. 2014600400253
3461.0 15. 35. 2014600400254
3468.6 34. 22. 2014600400255
3492.0 233. 13. 2014600400256
3512.5 500. 9. 2014600400257
3537.7 9. 45. 2014600400258
3553.7 622. 8. 2014600400259
3597.2 245. 14. 2014600400260
3646.2 374. 12. 2014600400261
3664.5 22. 40. 2014600400262
3687.5 590. 10. 2014600400263
3713.6 49. 30. 2014600400264
3727.3 20. 40. 2014600400265
3752.4 89. 23. 2014600400266
3772.2 65. 30. 2014600400267
3779.0 10. 80. 2014600400268
3786.7 100. 23. 2014600400269
3798.2 20. 40. 2014600400270
3837.0 20. 40. 2014600400271
3853.8 240. 16. 2014600400272
3874.2 110. 25. 2014600400273
3884.3 133. 22. 2014600400274
3908.9 115. 29. 2014600400275
3926.5 20. 60. 2014600400276
3937.0 40. 50. 2014600400277
3947.1 330. 18. 2014600400278
3965.7 73. 35. 2014600400279
3982.7 20. 60. 2014600400280
3994.0 80. 35. 2014600400281
4014.6 64. 38. 2014600400282
4040.3 30. 45. 2014600400283
4059.4 400. 18. 2014600400284
4079.9 950. 13. 2014600400285
4105.2 61. 47. 2014600400286
4127.5 30. 45. 2014600400287
4140.3 1200. 13. 2014600400288
ENDDATA 275 0 2014600400289
ENDSUBENT 288 0 2014600499999
SUBENT 20146005 20170424 22612014600500001
BIB 4 8 2014600500002
REACTION (45-RH-103(N,TOT),,WID) 2014600500003
FLAG (1.) Study was difficult or impossible because 2014600500004
of the presence of a near-by resonance. 2014600500005
(2.) Resonance level can be double because the 2014600500006
(gamma-width) is very large. 2014600500007
STATUS (TABLE) Tbl.4 from Nucl. Phys. A143(1970)130. 2014600500008
HISTORY (20170424A) SD: Meaningless zeros from right side of 2014600500009
the values were deleted. 2014600500010
ENDBIB 8 0 2014600500011
NOCOMMON 0 0 2014600500012
DATA 4 123 2014600500013
EN-RES DATA DATA-ERR FLAG 2014600500014
EV MILLI-EV PER-CENT NO-DIM 2014600500015
34.41 151. 8. 2014600500016
46.85 175. 7. 2014600500017
68.34 167. 5. 2014600500018
83.54 157. 50. 2014600500019
95.78 173. 6. 2014600500020
98.82 178. 11. 2014600500021
108.88 100. 80. 2014600500022
110.88 169. 8. 1. 2014600500023
114.08 175. 11. 2014600500024
125.62 175. 3. 2014600500025
154.31 388. 2. 2014600500026
179.43 174. 12. 2014600500027
187.23 210. 3. 2014600500028
199.83 600. 50. 2. 2014600500029
205.15 180. 60. 2014600500030
254.04 213. 5. 2014600500031
263.28 220. 25. 1. 2014600500032
272.40 233. 5. 2014600500033
290.06 178. 5. 2014600500034
312.76 220. 55. 2014600500035
319.88 275. 3. 2014600500036
327.76 185. 35. 2014600500037
362.78 105. 90. 2014600500038
366.55 135. 20. 2014600500039
374.28 165. 50. 2014600500040
388.94 130. 80. 2014600500041
406.48 193. 6. 2014600500042
435.74 400. 4. 2014600500043
450.34 151. 29. 2014600500044
473.15 80. 90. 2. 2014600500045
486.81 33. 95. 1. 2014600500046
492.42 166. 29. 2014600500047
505.15 90. 95. 2014600500048
526.44 110. 80. 2014600500049
555.79 268. 4. 2014600500050
582.07 155. 25. 2014600500051
605.20 100. 80. 1. 2014600500052
621.12 390. 30. 2. 2014600500053
646.62 230. 12. 2014600500054
663.90 195. 24. 2014600500055
676.93 130. 60. 2014600500056
683.82 120. 55. 2014600500057
692.46 246. 15. 2014600500058
702.33 470. 4. 2014600500059
760.15 100. 95. 2014600500060
783.16 218. 15. 2014600500061
797.08 268. 39. 2014600500062
831.36 197. 60. 2014600500063
845.77 323. 5. 2014600500064
895.58 142. 57. 2014600500065
914.49 298. 9. 2014600500066
930.04 207. 11. 2014600500067
955.71 282. 18. 2014600500068
1025.0 190. 80. 2014600500069
1077.1 190. 40. 2014600500070
1111.0 200. 20. 2014600500071
1154.9 346. 12. 2014600500072
1190.4 228. 23. 2014600500073
1196.7 824. 7. 2014600500074
1245.7 180. 80. 2014600500075
1272.4 600. 4. 2014600500076
1306.9 249. 12. 2014600500077
1326.0 230. 24. 2014600500078
1365.5 240. 19. 2014600500079
1408.0 280. 33. 2014600500080
1433.7 100. 95. 2014600500081
1487.1 270. 54. 2014600500082
1531.9 200. 90. 2014600500083
1544.0 630. 8. 2014600500084
1561.6 125. 95. 2014600500085
1567.7 270. 15. 2014600500086
1620.2 463. 7. 2014600500087
1671.4 253. 25. 2014600500088
1697.6 570. 6. 2014600500089
1737.0 150. 90. 2014600500090
1766.2 204. 65. 2014600500091
1796.3 280. 24. 2014600500092
1820.8 762. 6. 2. 2014600500093
1843.4 120. 77. 2014600500094
1905.1 219. 80. 2014600500095
1982.9 821. 10. 2014600500096
2010.2 128. 98. 2014600500097
2060.2 440. 21. 2014600500098
2102.4 203. 80. 2014600500099
2115.8 574. 13. 2014600500100
2179.8 97. 95. 2014600500101
2195.2 260. 26. 2014600500102
2260.2 338. 44. 2014600500103
2296.7 660. 8. 2014600500104
2315.8 322. 56. 2014600500105
2333.1 1270. 25. 2. 2014600500106
2380.0 280. 65. 2014600500107
2410.1 535. 90. 2014600500108
2416.8 480. 35. 2014600500109
2434.1 900. 30. 2. 2014600500110
2461.4 530. 15. 2014600500111
2596.8 504. 95. 2014600500112
2606.0 565. 15. 2014600500113
2630.4 414. 25. 2014600500114
2668.9 1900. 45. 2. 2014600500115
2721.7 306. 57. 2014600500116
2793.3 216. 45. 2014600500117
2858.1 630. 40. 2014600500118
2881.7 510. 60. 2014600500119
2952.8 2300. 35. 2. 2014600500120
2998.8 530. 36. 2014600500121
3030.4 455. 30. 2014600500122
3084.3 330. 31. 2014600500123
3131.6 640. 15. 2014600500124
3168.6 260. 90. 2014600500125
3272.9 885. 22. 2014600500126
3305.0 535. 57. 2014600500127
3396.2 1730. 10. 2014600500128
3492.0 700. 32. 2014600500129
3512.5 570. 20. 2014600500130
3553.7 620. 18. 2014600500131
3597.2 550. 40. 2014600500132
3646.2 800. 27. 2014600500133
3687.5 1260. 19. 2014600500134
3853.8 1200. 50. 2014600500135
4059.4 1940. 33. 2014600500136
4079.9 670. 27. 2014600500137
4140.3 830. 23. 2014600500138
ENDDATA 125 0 2014600500139
ENDSUBENT 138 0 2014600599999
SUBENT 20146006 20170424 22612014600600001
BIB 4 43 2014600600002
REACTION (45-RH-103(N,0),,J) 2014600600003
FLAG (1.) Assigned by the possible values of (gamma- 2014600600004
width) in the analysis of transmission data. 2014600600005
(2.) Probable. Assigned by the possible values 2014600600006
of (gamma-width) in the analysis of transmission data.2014600600007
(3.) Uncertain. Assigned by the possible values 2014600600008
of (gamma-width) in the analysis of transmission data.2014600600009
(4.) Probable. Assigned by the possible values 2014600600010
of (gamma-width) in the analysis of transmission data 2014600600011
and the value of chi-square, dependent on supposed 2014600600012
interference. 2014600600013
(5.) Uncertain. Assigned by the possible values 2014600600014
of (gamma-width) in the analysis of transmission data 2014600600015
and the value of chi-square, dependent on supposed 2014600600016
interference. 2014600600017
(6.) Assigned by the possible values of (gamma- 2014600600018
width) in the analysis of transmission data 2014600600019
and by the scattering data analysis. 2014600600020
(7.) Probable. Assigned by the possible values 2014600600021
of (gamma-width) in the analysis of transmission data 2014600600022
and by the scattering data analysis. 2014600600023
(8.) Assigned by the possible values of (gamma- 2014600600024
width) in the analysis of transmission data, by the 2014600600025
value of chi-square,dependent on supposed interference2014600600026
and by the scattering data analysis. 2014600600027
(9.) Assigned by the value of chi-square, 2014600600028
dependent on supposed interference 2014600600029
and by the scattering data analysis. 2014600600030
(10.) Probable.Assigned by the value of chi-square2014600600031
dependent on supposed interference. 2014600600032
(11.) Assigned by analysis of scattering data. 2014600600033
(12.) Probable. Assigned by analysis of scattering2014600600034
data. 2014600600035
(13.) Uncertain.Assigned by analysis of scattering2014600600036
data. 2014600600037
(14.). Assigned by the possible values of (gamma- 2014600600038
width) in the analysis of transmission data and by the2014600600039
scattering data analysis. 2014600600040
Resonance level can be double because the (gamma- 2014600600041
width) is very large. 2014600600042
STATUS (TABLE) Tbl.4 from Nucl. Phys. A143(1970)130. 2014600600043
HISTORY (20170424A) SD: Meaningless zeros from right side of 2014600600044
the values were deleted. 2014600600045
ENDBIB 43 0 2014600600046
NOCOMMON 0 0 2014600600047
DATA 3 64 2014600600048
EN-RES DATA FLAG 2014600600049
EV NO-DIM NO-DIM 2014600600050
46.85 0. 12. 2014600600051
95.78 0. 11. 2014600600052
125.62 1. 11. 2014600600053
154.31 0. 6. 2014600600054
187.23 1. 8. 2014600600055
254.04 1. 8. 2014600600056
272.40 1. 8. 2014600600057
290.06 1. 8. 2014600600058
319.88 1. 6. 2014600600059
406.48 1. 9. 2014600600060
435.74 1. 6. 2014600600061
555.79 1. 6. 2014600600062
646.62 1. 8. 2014600600063
676.93 1. 10. 2014600600064
683.82 0. 10. 2014600600065
692.46 1. 8. 2014600600066
702.33 1. 6. 2014600600067
845.77 1. 6. 2014600600068
914.49 0. 6. 2014600600069
930.04 1. 6. 2014600600070
955.71 0. 4. 2014600600071
1154.9 1. 8. 2014600600072
1196.7 0. 2. 2014600600073
1272.4 1. 6. 2014600600074
1306.9 1. 1. 2014600600075
1365.5 1. 11. 2014600600076
1487.1 0. 4. 2014600600077
1544.0 0. 8. 2014600600078
1561.6 1. 10. 2014600600079
1567.7 1. 6. 2014600600080
1620.2 1. 6. 2014600600081
1671.4 0. 12. 2014600600082
1697.6 1. 1. 2014600600083
1796.3 1. 8. 2014600600084
1820.8 1. 14. 2014600600085
1843.4 1. 8. 2014600600086
1905.1 0. 13. 2014600600087
1982.9 0. 7. 2014600600088
2060.2 0. 7. 2014600600089
2115.8 0. 7. 2014600600090
2179.8 1. 5. 2014600600091
2195.2 1. 1. 2014600600092
2296.7 1. 6. 2014600600093
2315.8 0. 3. 2014600600094
2416.8 0. 3. 2014600600095
2461.4 1. 1. 2014600600096
2606.0 1. 1. 2014600600097
2630.4 1. 1. 2014600600098
2793.3 1. 1. 2014600600099
2858.1 0. 3. 2014600600100
2881.7 0. 3. 2014600600101
2998.8 0. 3. 2014600600102
3030.4 1. 2. 2014600600103
3084.3 1. 2014600600104
3131.6 1. 2014600600105
3272.9 0. 3. 2014600600106
3396.2 0. 2. 2014600600107
3492.0 0. 3. 2014600600108
3512.5 1. 1. 2014600600109
3553.7 1. 1. 2014600600110
3646.2 0. 3. 2014600600111
3687.5 0. 3. 2014600600112
4079.9 1. 1. 2014600600113
4140.3 1. 1. 2014600600114
ENDDATA 66 0 2014600600115
ENDSUBENT 114 0 2014600699999
SUBENT 20146007 20170424 22612014600700001
BIB 4 25 2014600700002
REACTION (45-RH-103(N,0),,L) 2014600700003
FLAG (1.) L=0 because (2g * n-width) is very large. 2014600700004
(2.) L was assigned by chi square method. 2014600700005
(3.) Probable. Assigned by chi square method. 2014600700006
(4.) Uncertain. Assigned by chi square method. 2014600700007
(5.) Assigned by chi square and resonance shape. 2014600700008
(6.) Probable. by chi square and resonance shape.2014600700009
Resonance level can be double because the (gamma- 2014600700010
width) is very large. 2014600700011
(7.) Assigned by the resonance shape. 2014600700012
(8.) Uncertain. Assigned by the resonance shape. 2014600700013
(9.) L=1 probable because resonance is very small2014600700014
(10.) l=1 probable because resonance is very small2014600700015
resonance level can be double because the (gamma- 2014600700016
width) is very large. 2014600700017
(11.) L was assigned by Chi-square method. 2014600700018
Resonance level can be double because the (gamma- 2014600700019
width) is very large. 2014600700020
(12.) L was assigned by Chi-square method. 2014600700021
Study was difficult or impossible because of the 2014600700022
presence of a near-by resonance. 2014600700023
STATUS (TABLE) Tbl.4 from Nucl. Phys. A143(1970)130. 2014600700024
HISTORY (20170424A) SD: STATUS was added. Data were update 2014600700025
according presentation in the Tbl. (meaningless zeros 2014600700026
from right side of the values were deleted). 2014600700027
ENDBIB 25 0 2014600700028
NOCOMMON 0 0 2014600700029
DATA 3 118 2014600700030
EN-RES DATA FLAG 2014600700031
EV NO-DIM NO-DIM 2014600700032
34.41 1. 2. 2014600700033
44.49 1. 9. 2014600700034
46.85 0. 2014600700035
51.85 1. 9. 2014600700036
68.34 0. 2. 2014600700037
83.54 1. 3. 2014600700038
95.78 0. 2014600700039
98.82 1. 2. 2014600700040
108.88 1. 9. 2014600700041
114.08 1. 2. 2014600700042
125.62 0. 2014600700043
154.31 0. 2014600700044
179.43 1. 2. 2014600700045
187.23 0. 2014600700046
199.83 1. 10. 2014600700047
205.15 1. 3. 2014600700048
254.04 0. 2014600700049
272.40 0. 2014600700050
290.06 0. 2014600700051
312.76 1. 4. 2014600700052
319.88 0. 2014600700053
327.76 0. 2. 2014600700054
354.13 1. 9. 2014600700055
362.78 0. 2. 2014600700056
366.55 1. 2. 2014600700057
374.28 1. 3. 2014600700058
388.94 1. 2. 2014600700059
406.48 0. 2014600700060
427.95 1. 9. 2014600700061
435.74 0. 2014600700062
444.27 1. 9. 2014600700063
447.52 1. 9. 2014600700064
473.15 1. 11. 2014600700065
486.81 0. 12. 2014600700066
489.56 1. 9. 2014600700067
492.42 1. 2. 2014600700068
505.15 1. 2. 2014600700069
526.44 1. 2. 2014600700070
547.25 1. 9. 2014600700071
555.79 0. 2014600700072
582.07 1. 2. 2014600700073
602.94 1. 9. 2014600700074
608.10 1. 9. 2014600700075
621.12 1. 6. 2014600700076
646.62 0. 2014600700077
676.93 0. 2014600700078
683.82 0. 2014600700079
692.46 0. 2014600700080
702.33 0. 2014600700081
783.16 0. 1. 2014600700082
797.08 0. 7. 2014600700083
828.10 1. 9. 2014600700084
845.77 0. 2014600700085
895.58 1. 2. 2014600700086
914.49 0. 2014600700087
930.04 0. 2014600700088
955.71 0. 2014600700089
1008.0 1. 9. 2014600700090
1066.4 1. 9. 2014600700091
1111.0 0. 2014600700092
1154.9 0. 2014600700093
1190.4 0. 2014600700094
1196.7 0. 2014600700095
1245.7 0. 7. 2014600700096
1272.4 0. 2014600700097
1306.9 0. 2014600700098
1326.0 0. 2014600700099
1365.5 0. 2014600700100
1393.6 0. 8. 2014600700101
1408.0 0. 7. 2014600700102
1433.7 0. 7. 2014600700103
1483.5 1. 5. 2014600700104
1487.1 0. 2014600700105
1531.9 0. 7. 2014600700106
1544.0 0. 2014600700107
1561.6 0. 2014600700108
1567.7 0. 2014600700109
1620.2 0. 2014600700110
1671.4 0. 2014600700111
1697.6 0. 2014600700112
1737.0 0. 7. 2014600700113
1766.2 0. 7. 2014600700114
1796.3 0. 2014600700115
1820.8 0. 2014600700116
1843.4 0. 2014600700117
1905.1 0. 2014600700118
1982.9 0. 2014600700119
2010.2 0. 7. 2014600700120
2060.2 0. 2014600700121
2115.8 0. 2014600700122
2179.8 0. 2014600700123
2195.2 0. 2014600700124
2260.2 0. 2014600700125
2296.7 0. 2014600700126
2315.8 0. 2014600700127
2416.8 0. 2014600700128
2461.4 0. 2014600700129
2606.0 0. 2014600700130
2630.4 0. 2014600700131
2793.3 0. 2014600700132
2858.1 0. 2014600700133
2881.7 0. 2014600700134
2998.8 0. 2014600700135
3030.4 0. 2014600700136
3084.3 0. 2014600700137
3131.6 0. 2014600700138
3272.9 0. 2014600700139
3305.0 0. 2014600700140
3396.2 0. 2014600700141
3492.0 0. 2014600700142
3512.5 0. 2014600700143
3553.7 0. 2014600700144
3597.2 0. 2014600700145
3646.2 0. 2014600700146
3687.5 0. 2014600700147
4059.4 0. 2014600700148
4079.9 0. 2014600700149
4140.3 0. 2014600700150
ENDDATA 120 0 2014600700151
ENDSUBENT 150 0 2014600799999
SUBENT 20146008 20170424 22612014600800001
BIB 4 8 2014600800002
REACTION (45-RH-103(N,EL)45-RH-103,,RAD) 2014600800003
Effective nuclear radius. 2014600800004
ANALYSIS .From the contribution of remote resonances. 2014600800005
STATUS (TABLE) From the text on p.136 of 2014600800006
Nucl.Phys. A143(1970)130. 2014600800007
HISTORY (20170424A) SD: STATUS was added. Data were update 2014600800008
according presentation in the Tbl. (meaningless zeros 2014600800009
from right side of the values were deleted). 2014600800010
ENDBIB 8 0 2014600800011
NOCOMMON 0 0 2014600800012
DATA 4 1 2014600800013
EN-MAX EN-MIN DATA DATA-ERR 2014600800014
MEV MEV FERMI FERMI 2014600800015
4.0E-03 0. 6.56 6.E-02 2014600800016
ENDDATA 3 0 2014600800017
ENDSUBENT 16 0 2014600899999
SUBENT 20146009 20170424 22612014600900001
BIB 4 9 2014600900002
REACTION (45-RH-103(N,EL),,STF) 2014600900003
ANALYSIS .Obtained by the distribution and by a histogram of the2014600900004
sum of the reduced neutron-widths. 2014600900005
.From 159 resonances. 2014600900006
STATUS (TABLE) From the text on p.142 of 2014600900007
Nucl.Phys. A143(1970)130. 2014600900008
HISTORY (20170424A) SD: STATUS was added. Data were update 2014600900009
according presentation in the Tbl. (meaningless zeros 2014600900010
from right side of the values were deleted). 2014600900011
ENDBIB 9 0 2014600900012
COMMON 1 3 2014600900013
MOMENTUM L 2014600900014
NO-DIM 2014600900015
0. 2014600900016
ENDCOMMON 3 0 2014600900017
DATA 5 1 2014600900018
EN-RES-MAX EN-RES-MIN DATA +DATA-ERR -DATA-ERR 2014600900019
MEV MEV NO-DIM NO-DIM NO-DIM 2014600900020
4.140E-03 1.2E-06 5.4E-05 7.E-06 6.E-06 2014600900021
ENDDATA 3 0 2014600900022
ENDSUBENT 21 0 2014600999999
SUBENT 20146010 20170424 22612014601000001
BIB 4 9 2014601000002
REACTION (45-RH-103(N,EL),,STF) 2014601000003
Spin-dependent S-wave function. 2014601000004
ANALYSIS .Strength function was obtained by the distribution of 2014601000005
the reduced neutron-widths. 2014601000006
STATUS (TABLE) From the text on p.143 of 2014601000007
Nucl.Phys. A143(1970)130. 2014601000008
HISTORY (20170424A) SD: STATUS was added. Data were update 2014601000009
according presentation in the Tbl. (meaningless zeros 2014601000010
from right side of the values were deleted). 2014601000011
ENDBIB 9 0 2014601000012
COMMON 1 3 2014601000013
MOMENTUM L 2014601000014
NO-DIM 2014601000015
0. 2014601000016
ENDCOMMON 3 0 2014601000017
DATA 6 2 2014601000018
EN-RES-MAX EN-RES-MIN SPIN J DATA +DATA-ERR -DATA-ERR 2014601000019
MEV MEV NO-DIM NO-DIM NO-DIM NO-DIM 2014601000020
4.140E-03 1.2E-06 0. 4.2E-05 1.1E-05 1.0E-052014601000021
4.140E-03 1.2E-06 1. 6.3E-05 1.2E-05 1.0E-052014601000022
ENDDATA 4 0 2014601000023
ENDSUBENT 22 0 2014601099999
SUBENT 20146011 20170424 22612014601100001
BIB 4 9 2014601100002
REACTION (45-RH-103(N,EL),,STF) 2014601100003
Spin-dependent S-wave function. 2014601100004
ANALYSIS .Strength function was obtained by a histogram of 2014601100005
the sum of the reduced neutron widths. 2014601100006
STATUS (TABLE) From the text on p.143 of 2014601100007
Nucl.Phys. A143(1970)130. 2014601100008
HISTORY (20170424A) SD: STATUS was added. Data were update 2014601100009
according presentation in the Tbl. (meaningless zeros 2014601100010
from right side of the values were deleted). 2014601100011
ENDBIB 9 0 2014601100012
COMMON 1 3 2014601100013
MOMENTUM L 2014601100014
NO-DIM 2014601100015
0.0 2014601100016
ENDCOMMON 3 0 2014601100017
DATA 6 2 2014601100018
EN-RES-MAX EN-RES-MIN SPIN J DATA +DATA-ERR -DATA-ERR 2014601100019
MEV MEV NO-DIM NO-DIM NO-DIM NO-DIM 2014601100020
4.140E-03 1.2E-06 0. 4.4E-05 1.2E-05 1.0E-052014601100021
4.140E-03 1.2E-06 1. 5.8E-05 1.0E-05 1.0E-052014601100022
ENDDATA 4 0 2014601100023
ENDSUBENT 22 0 2014601199999
SUBENT 20146012 20170424 22612014601200001
BIB 5 12 2014601200002
REACTION (45-RH-103(N,EL),,STF) 2014601200003
P-wave strength function from about 65 resonances for 2014601200004
each region of 700 eV. 2014601200005
ANALYSIS .Strength function was obtained by a histogram of 2014601200006
the sum of the reduced neutron widths. 2014601200007
CORRECTION .Corrected for missing p-wave resonances and for 2014601200008
possibly included S-wave resonances. 2014601200009
STATUS (TABLE) From the text on p.142-143 of 2014601200010
Nucl.Phys. A143(1970)130. 2014601200011
HISTORY (20170424A) SD: STATUS was added. Data were update 2014601200012
according presentation in the Tbl. (meaningless zeros 2014601200013
from right side of the values were deleted). 2014601200014
ENDBIB 12 0 2014601200015
COMMON 1 3 2014601200016
MOMENTUM L 2014601200017
NO-DIM 2014601200018
1. 2014601200019
ENDCOMMON 3 0 2014601200020
DATA 5 3 2014601200021
EN-RES-MAX EN-RES-MIN DATA +DATA-ERR -DATA-ERR 2014601200022
MEV MEV NO-DIM NO-DIM NO-DIM 2014601200023
7.0E-04 3.40E-05 6.2E-04 2014601200024
1.35E-03 3.40E-05 6.E-04 1.5E-04 1.8E-04 2014601200025
1.35E-03 7.00E-04 4.2E-04 2014601200026
ENDDATA 5 0 2014601200027
ENDSUBENT 26 0 2014601299999
SUBENT 20146013 20170424 22612014601300001
BIB 4 9 2014601300002
REACTION (45-RH-103(N,0),,D) 2014601300003
ANALYSIS .Obtained from the distribution of (g*reduced n-width) 2014601300004
with nu = 1 and with nu adjusted. (Nu = deg.of freed.)2014601300005
.From 159 resonances. 2014601300006
STATUS (TABLE) From the text on p.143 of 2014601300007
Nucl.Phys. A143(1970)130. 2014601300008
HISTORY (20170424A) SD: STATUS was added. Data were update 2014601300009
according presentation in the Tbl. (meaningless zeros 2014601300010
from right side of the values were deleted). 2014601300011
ENDBIB 9 0 2014601300012
COMMON 1 3 2014601300013
MOMENTUM L 2014601300014
NO-DIM 2014601300015
0.0 2014601300016
ENDCOMMON 3 0 2014601300017
DATA 4 1 2014601300018
EN-RES-MAX EN-RES-MIN DATA DATA-ERR 2014601300019
MEV MEV EV EV 2014601300020
4.140E-03 1.2E-06 27. 2. 2014601300021
ENDDATA 3 0 2014601300022
ENDSUBENT 21 0 2014601399999
ENDENTRY 13 0 2014699999999