ENTRY G0043 20141008 G031G004300000001 SUBENT G0043001 20141008 G031G004300100001 BIB 11 24 G004300100002 TITLE Low-energy dipole strength in 112,120Sn G004300100003 AUTHOR (B.Oezel-Tashenov, J.Enders, H.Lenske, A.M.Krumbholz, G004300100004 E.Litvinova, P.von Neumann-Cosel, I.Poltoratska, G004300100005 A.Richter, G.Rusev, D.Savran, N.Tsoneva) G004300100006 INSTITUTE (2GERTHD,2GERJLU,1USAWMU,1USAMSU,1USALAS,2GERGSI) G004300100007 (3BULBLA) G004300100008 (2TUKTUK) Nigde University, Nigde G004300100009 (2GERGER) Frankfurt Inst.for Advanced Studies,FrankfurtG004300100010 REFERENCE (J,PR/C,90,024304,2014) G004300100011 FACILITY (LINAC,2GERTHD) Electron linac S-DALINAC G004300100012 SAMPLE Isotopically enriched (>99%) metalic 112Sn and 120Sn G004300100013 (~2 g) sandwiched between 11B layers (total weight of G004300100014 ~1 g). G004300100015 DETECTOR (HPGE) at 90 deg and 130 deg G004300100016 ANALYSIS Photon flux was determined by known cross sections of G004300100017 11B excitations. G004300100018 Multipolarities=1 or 2 were determined by the G004300100019 intensity ratios W(90deg)/W(130deg)=0.7 or 2. G004300100020 REL-REF (I,,P.Mohr+,J,NIM/A,423,480,1999) Details of setup G004300100021 ERR-ANALYS (MISC-ERR) Statistical errors from the peak fit and G004300100022 systematic errors G004300100023 2(ERR-1) Uncertainty in photon flux normalization (~10%)G004300100024 (ERR-S) Statistical uncertainty G004300100025 HISTORY (20141008C) On G004300100026 ENDBIB 24 0 G004300100027 COMMON 1 3 G004300100028 ERR-1 G004300100029 PER-CENT G004300100030 10. G004300100031 ENDCOMMON 3 0 G004300100032 ENDSUBENT 31 0 G004300199999 SUBENT G0043002 20141008 G031G004300200001 BIB 5 13 G004300200002 REACTION 1(50-SN-112(G,0),,EN) G004300200003 2((50-SN-112(G,EL),,WID)*(50-SN-112(G,EL),,WID)/ G004300200004 (50-SN-112(G,TOT),,WID)) G004300200005 INC-SOURCE (BRST) E0=5.5, 7.0 and 9.5 MeV G004300200006 ANALYSIS Gamma(el)=Gamma(tot) assumed. G004300200007 Only the result obtained at E0=7.5 MeV irradiation G004300200008 was used when B(E1) at E0=9.5 MeV) is larger than G004300200009 B(E1) at E0=7.5 MeV) to exclude indirect population G004300200010 of the levels by feeding via inelastic transitions G004300200011 from higher-lying states, otherwise the results at G004300200012 E0=7.0 and 9.5 MeV irradiations were averaged. G004300200013 MISC-COL (MISC) B(E1) transition strength in 10E-3*e**2*fm**2 G004300200014 STATUS (TABLE) Table I of Phys.Rev.C90(2014)024304 G004300200015 ENDBIB 13 0 G004300200016 COMMON 2 3 G004300200017 SPIN J PARITY G004300200018 NO-DIM NO-DIM G004300200019 1. -1. G004300200020 ENDCOMMON 3 0 G004300200021 DATA 5 92 G004300200022 DATA 1DATA 2ERR-S 2MISC MISC-ERR G004300200023 MEV MILLI-EV MILLI-EV SEE TEXT SEE TEXT G004300200024 3433.9 162. 15. 11.5 1.1 G004300200025 4141.3 17. 4. 0.7 0.2 G004300200026 4162.3 44. 4. 1.8 0.2 G004300200027 4330.4 15. 3. 0.5 0.1 G004300200028 4726.5 12. 3. 0.3 0.1 G004300200029 4837.4 28. 5. 0.7 0.1 G004300200030 5057.1 134. 13. 3.0 0.3 G004300200031 5128.2 198. 20. 4.2 0.4 G004300200032 5246.2 166. 14. 3.3 0.3 G004300200033 5480.5 66. 11. 1.2 0.2 G004300200034 5502.6 86. 10. 1.5 0.2 G004300200035 5593.7 43. 7. 0.7 0.1 G004300200036 5617.6 39. 7. 0.6 0.1 G004300200037 5649.1 43. 7. 0.7 0.1 G004300200038 5666.4 23. 6. 0.4 0.1 G004300200039 5699.9 33. 7. 0.5 0.1 G004300200040 5748.6 66. 7. 1.0 0.1 G004300200041 5812.7 34. 8. 0.5 0.1 G004300200042 5860.7 159. 27. 2.3 0.4 G004300200043 5884.0 100. 16. 1.4 0.2 G004300200044 5924.1 112. 12. 1.5 0.2 G004300200045 5976.6 128. 14. 1.7 0.2 G004300200046 6005.0 244. 21. 3.2 0.3 G004300200047 6059.8 470. 44. 6.1 0.6 G004300200048 6080.9 73. 15. 0.9 0.2 G004300200049 6096.9 385. 23. 3.6 0.2 G004300200050 6129.0 115. 13. 1.4 0.2 G004300200051 6150.4 273. 28. 3.4 0.3 G004300200052 6168.3 98. 17. 1.2 0.2 G004300200053 6198.7 179. 18. 2.2 0.2 G004300200054 6224.3 315. 26. 3.7 0.3 G004300200055 6246.4 152. 20. 1.8 0.2 G004300200056 6259.1 130. 17. 1.5 0.2 G004300200057 6272.6 220. 21. 2.5 0.3 G004300200058 6313.3 251. 23. 2.9 0.3 G004300200059 6348.7 134. 17. 1.5 0.2 G004300200060 6388.1 663. 47. 7.3 0.5 G004300200061 6404.1 1686. 120. 18.4 1.3 G004300200062 6428.6 114. 18. 1.2 0.2 G004300200063 6450.0 109. 15. 1.2 0.2 G004300200064 6520.7 309. 33. 3.2 0.3 G004300200065 6550.1 54. 11. 0.6 0.1 G004300200066 6601.0 173. 23. 1.7 0.2 G004300200067 6679.9 74. 14. 0.7 0.1 G004300200068 6706.7 187. 24. 1.8 0.2 G004300200069 6715.0 156. 67. 1.5 0.6 G004300200070 6731.9 289. 51. 2.7 0.5 G004300200071 6795.5 185. 25. 1.7 0.2 G004300200072 6818.7 139. 23. 1.3 0.2 G004300200073 6824.2 194. 32. 1.7 0.3 G004300200074 6855.9 170. 25. 1.5 0.2 G004300200075 6871.2 189. 19. 1.7 0.2 G004300200076 6941.2 367. 41. 3.1 0.3 G004300200077 6961.5 362. 53. 3.1 0.5 G004300200078 6982.7 246. 30. 2.1 0.3 G004300200079 7009.8 62. 15. 0.5 0.1 G004300200080 7018.7 82. 16. 0.7 0.1 G004300200081 7025.8 86. 17. 0.7 0.1 G004300200082 7043.1 245. 42. 2.0 0.3 G004300200083 7092.8 524. 48. 4.2 0.4 G004300200084 7167.2 363. 42. 2.8 0.3 G004300200085 7198.2 578. 75. 4.4 0.6 G004300200086 7228.1 164. 27. 1.2 0.2 G004300200087 7311.1 138. 28. 1.0 0.2 G004300200088 7389.9 183. 30. 1.3 0.2 G004300200089 7438.6 275. 42. 1.9 0.3 G004300200090 7444.1 233. 37. 1.6 0.3 G004300200091 7468.3 186. 45. 1.3 0.3 G004300200092 7531.3 429. 62. 2.9 0.4 G004300200093 7537.2 770. 82. 5.2 0.6 G004300200094 7559.1 323. 43. 2.1 0.3 G004300200095 7594.5 205. 31. 1.3 0.2 G004300200096 7615.3 257. 41. 1.7 0.3 G004300200097 7859.5 207. 35. 1.2 0.2 G004300200098 7904.7 196. 40. 1.1 0.2 G004300200099 7936.7 272. 39. 1.6 0.2 G004300200100 7988.2 606. 62. 3.4 0.3 G004300200101 8020.7 412. 67. 2.3 0.4 G004300200102 8051.6 396. 60. 2.2 0.3 G004300200103 8069.6 482. 65. 2.6 0.4 G004300200104 8194.5 518. 75. 2.7 0.4 G004300200105 8218.2 262. 48. 1.4 0.2 G004300200106 8253.6 177. 38. 0.9 0.2 G004300200107 8448.6 147. 41. 0.7 0.2 G004300200108 8568.9 166. 43. 0.8 0.2 G004300200109 8600.4 118. 35. 0.5 0.2 G004300200110 8750.2 249. 56. 1.1 0.2 G004300200111 8823.4 278. 64. 1.2 0.3 G004300200112 9050.5 413. 108. 1.6 0.4 G004300200113 9095.3 268. 65. 1.0 0.2 G004300200114 9150.1 240. 75. 0.9 0.3 G004300200115 9329.8 599. 138. 2.1 0.5 G004300200116 ENDDATA 94 0 G004300200117 ENDSUBENT 116 0 G004300299999 SUBENT G0043003 20141008 G031G004300300001 BIB 5 12 G004300300002 REACTION 1(50-SN-120(G,0),,EN) G004300300003 2((50-SN-120(G,EL),,WID)*(50-SN-120(G,EL),,WID)/ G004300300004 (50-SN-120(G,TOT),,WID)) G004300300005 INC-SOURCE (BRST) E0=7.5 and 9.1 MeV G004300300006 ANALYSIS Gamma(el)=Gamma(tot) assumed. G004300300007 B(E1) from E0=7.5 MeV and 9.1 MeV irradiation are G004300300008 close to one except for the lowest E1 transition G004300300009 populating the 3.279 MeV state (i.e., no feeding), G004300300010 therefore the results at E0=7.0 and 9.5 MeV G004300300011 irradiations were averaged. G004300300012 MISC-COL (MISC) B(E1) transition strength in 10E-3*e**2*fm**2 G004300300013 STATUS (TABLE) Table II of Phys.Rev.C90(2014)024304 G004300300014 ENDBIB 12 0 G004300300015 COMMON 2 3 G004300300016 SPIN J PARITY G004300300017 NO-DIM NO-DIM G004300300018 1. -1. G004300300019 ENDCOMMON 3 0 G004300300020 DATA 5 73 G004300300021 DATA 1DATA 2ERR-S 2MISC MISC-ERR G004300300022 MEV MILLI-EV MILLI-EV SEE TEXT SEE TEXT G004300300023 3279.4 137. 14. 8.6 0.9 G004300300024 4251.0 73. 10. 2.7 0.4 G004300300025 4564.8 36. 8. 1.0 0.2 G004300300026 4679.7 52. 10. 1.5 0.3 G004300300027 4939.0 36. 8. 0.9 0.2 G004300300028 5245.4 22. 7. 0.4 0.1 G004300300029 5354.4 37. 13. 0.7 0.2 G004300300030 5408.2 54. 13. 1.0 0.2 G004300300031 5447.2 126. 21. 2.2 0.4 G004300300032 5638.0 109. 18. 1.8 0.3 G004300300033 5647.8 172. 23. 2.7 0.4 G004300300034 5685.2 78. 20. 1.2 0.3 G004300300035 5697.3 67. 17. 1.0 0.3 G004300300036 5753.0 35. 13. 0.5 0.2 G004300300037 5758.0 42. 15. 0.6 0.2 G004300300038 5818.0 127. 25. 1.8 0.4 G004300300039 5882.1 280. 40. 3.9 0.6 G004300300040 5895.4 198. 26. 2.8 0.4 G004300300041 5927.7 165. 25. 2.3 0.3 G004300300042 5940.7 230. 44. 3.1 0.6 G004300300043 5950.2 139. 35. 1.9 0.5 G004300300044 5989.8 203. 38. 2.7 0.5 G004300300045 6001.7 168. 48. 2.2 0.6 G004300300046 6076.2 82. 21. 1.1 0.3 G004300300047 6093.5 110. 24. 1.4 0.3 G004300300048 6127.1 248. 35. 3.1 0.4 G004300300049 6152.5 127. 23. 1.6 0.3 G004300300050 6252.4 255. 48. 3.0 0.6 G004300300051 6267.0 350. 44. 4.1 0.5 G004300300052 6285.8 160. 31. 1.8 0.3 G004300300053 6305.9 270. 37. 3.1 0.4 G004300300054 6332.6 363. 54. 4.1 0.6 G004300300055 6344.9 370. 50. 4.2 0.6 G004300300056 6353.7 259. 38. 2.9 0.4 G004300300057 6375.0 118. 23. 1.3 0.3 G004300300058 6397.0 240. 40. 2.6 0.4 G004300300059 6408.3 456. 55. 5.0 0.6 G004300300060 6432.3 142. 28. 1.5 0.3 G004300300061 6443.7 299. 52. 3.2 0.6 G004300300062 6469.7 375. 62. 4.0 0.7 G004300300063 6485.8 409. 67. 4.3 0.7 G004300300064 6520.7 186. 32. 1.9 0.3 G004300300065 6539.5 219. 40. 2.2 0.4 G004300300066 6644.3 438. 68. 4.3 0.7 G004300300067 6691.0 206. 41. 2.0 0.4 G004300300068 6727.3 238. 55. 2.2 0.5 G004300300069 6898.9 508. 163. 4.6 1.5 G004300300070 6914.8 374. 58. 3.2 0.5 G004300300071 6990.4 376. 68. 3.2 0.6 G004300300072 7009.9 480. 98. 4.0 0.8 G004300300073 7025.0 216. 41. 1.8 0.3 G004300300074 7031.5 176. 35. 1.5 0.3 G004300300075 7038.9 160. 38. 1.3 0.3 G004300300076 7061.9 164. 48. 1.3 0.4 G004300300077 7095.6 242. 65. 1.9 0.5 G004300300078 7144.5 259. 58. 2.0 0.5 G004300300079 7235.1 495. 64. 3.7 0.5 G004300300080 7255.1 465. 88. 3.5 0.7 G004300300081 7460.1 175. 33. 1.2 0.2 G004300300082 7543.1 172. 49. 1.1 0.3 G004300300083 7569.2 309. 140. 2.0 0.9 G004300300084 7624.9 190. 40. 1.2 0.3 G004300300085 7701.2 229. 57. 1.4 0.4 G004300300086 7889.0 312. 62. 1.8 0.4 G004300300087 7958.6 523. 93. 3.0 0.5 G004300300088 7975.6 606. 98. 3.4 0.6 G004300300089 7994.5 237. 48. 1.3 0.3 G004300300090 8044.3 120. 30. 0.7 0.2 G004300300091 8079.7 258. 100. 1.4 0.5 G004300300092 8318.3 498. 96. 2.5 0.5 G004300300093 8399.5 450. 100. 2.2 0.5 G004300300094 8478.3 304. 80. 1.4 0.4 G004300300095 8554.9 447. 139. 2.0 0.6 G004300300096 ENDDATA 75 0 G004300300097 ENDSUBENT 96 0 G004300399999 ENDENTRY 3 0 G004399999999