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 results 2014600100010 (J,CR,254,2546,1962) Strength function, until 370 eV, 2014600100011 superseded. 2014600100012 INSTITUTE (2FR SAC) 2014600100013 FACILITY (LINAC,2FR SAC) 45 MeV Saclay electron linear 2014600100014 accelerator. 2014600100015 INC-SOURCE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