ENTRY G4069 20190218 G043G406900000001 SUBENT G4069001 20190218 G043G406900100001 BIB 11 17 G406900100002 TITLE Mass dependence of azimuthal asymmetry in the fission G406900100003 of 232Th and 233, 235, 236, 238U by polarized photons G406900100004 AUTHOR (V.V.Denyak,V.M.Khvastunov,S.A.Paschuk,H.R.Schelin) G406900100005 INSTITUTE (4UKRKFT) G406900100006 (3BZLBZL) Federal Univ. of Technology-Parana, Curitiba G406900100007 (3BZLBZL) Pele Pequeno Principe Research Inst.,CuritibaG406900100008 REFERENCE (J,EPJ/A,49,51,2013) G406900100009 #doi:10.1140/epja/i2013-13051-6 G406900100010 FACILITY (LINAC,4UKRKFT) LINAC-2000 G406900100011 INC-SOURCE (BRST,POLPS) G406900100012 DETECTOR (SIBAR) G406900100013 ERR-ANALYS (DATA-ERR) No information G406900100014 STATUS (TABLE) Correspond to Fig.5 of Eur.Phys.J.A 49(2013)51 G406900100015 ADD-RES The experimental asymmetry dependence on fragment G406900100016 mass for nuclei were presented. G406900100017 HISTORY (20190218C) UkrNDC G406900100018 (20190225R) Data received from V.Denyak G406900100019 ENDBIB 17 0 G406900100020 NOCOMMON 0 0 G406900100021 ENDSUBENT 20 0 G406900199999 SUBENT G4069002 20190218 G043G406900200001 BIB 2 3 G406900200002 REACTION (90-TH-232(G,F)MASS,SEC,FY,,BRA/REL) G406900200003 The distributions were normalized at the maxima. G406900200004 SAMPLE Natural, 500 micro-g/cm2 thickness G406900200005 ENDBIB 3 0 G406900200006 COMMON 1 3 G406900200007 EN-MAX G406900200008 MEV G406900200009 12. G406900200010 ENDCOMMON 3 0 G406900200011 DATA 3 14 G406900200012 MASS DATA DATA-ERR G406900200013 NO-DIM ARB-UNITS ARB-UNITS G406900200014 58.4 9.2 6.6 G406900200015 66.5 21.0 6.6 G406900200016 74.6 92.4 7.2 G406900200017 82.7 379. 14. G406900200018 90.0 444. 17. G406900200019 99.0 302. 16. G406900200020 106.7 165. 12. G406900200021 114.8 166. 12. G406900200022 122.9 261. 17. G406900200023 131.0 415. 18. G406900200024 139.3 406. 18. G406900200025 147.2 323. 18. G406900200026 156.2 38.0 6.6 G406900200027 164.3 7.2 7.2 G406900200028 ENDDATA 16 0 G406900200029 ENDSUBENT 28 0 G406900299999 SUBENT G4069003 20190218 G043G406900300001 BIB 2 3 G406900300002 REACTION (92-U-233(G,F)MASS,SEC,FY,,BRA/REL) G406900300003 The distributions were normalized at the maxima. G406900300004 SAMPLE (92-U-233,ENR=0.98) 115 micro-g/cm2 thickness G406900300005 ENDBIB 3 0 G406900300006 COMMON 1 3 G406900300007 EN-MAX G406900300008 MEV G406900300009 12. G406900300010 ENDCOMMON 3 0 G406900300011 DATA 3 22 G406900300012 MASS DATA DATA-ERR G406900300013 NO-DIM ARB-UNITS ARB-UNITS G406900300014 65.9 22.4 5.1 G406900300015 70.6 31.0 6.6 G406900300016 75.4 62.8 9.2 G406900300017 80.2 278. 19. G406900300018 84.9 804. 32. G406900300019 89.7 1804. 47. G406900300020 94.5 2466. 55. G406900300021 99.2 2354. 53. G406900300022 104.0 1730. 46. G406900300023 108.7 1164. 39. G406900300024 113.5 807. 34. G406900300025 118.3 899. 35. G406900300026 123.1 1215. 41. G406900300027 127.8 1674. 47. G406900300028 132.6 2359. 54. G406900300029 137.3 2549. 56. G406900300030 142.1 2235. 52. G406900300031 146.9 1371. 42. G406900300032 151.6 590. 28. G406900300033 156.4 242. 18. G406900300034 161.2 80. 11. G406900300035 166.0 35.1 6.0 G406900300036 ENDDATA 24 0 G406900300037 ENDSUBENT 36 0 G406900399999 SUBENT G4069004 20190218 G043G406900400001 BIB 2 3 G406900400002 REACTION (92-U-235(G,F)MASS,SEC,FY,,BRA/REL) G406900400003 The distributions were normalized at the maxima. G406900400004 SAMPLE (92-U-235,ENR=0.98) 225 micro-g/cm2 thickness G406900400005 ENDBIB 3 0 G406900400006 COMMON 1 3 G406900400007 EN-MAX G406900400008 MEV G406900400009 12. G406900400010 ENDCOMMON 3 0 G406900400011 DATA 3 18 G406900400012 MASS DATA DATA-ERR G406900400013 NO-DIM ARB-UNITS ARB-UNITS G406900400014 60.9 50.1 3.8 G406900400015 67.3 75.8 4.9 G406900400016 73.6 182.0 7.9 G406900400017 80.0 525. 14. G406900400018 86.3 1206. 21. G406900400019 92.6 1915. 27. G406900400020 99.0 1997. 27. G406900400021 105.3 1484. 24. G406900400022 111.7 919. 20. G406900400023 118.0 724. 19. G406900400024 124.3 1046. 22. G406900400025 130.7 1628. 26. G406900400026 137.0 2087. 29. G406900400027 143.4 1968. 28. G406900400028 149.7 1258. 22. G406900400029 156.0 445. 14. G406900400030 162.4 80.3 8.6 G406900400031 168.7 5.0 1.0 G406900400032 ENDDATA 20 0 G406900400033 ENDSUBENT 32 0 G406900499999 SUBENT G4069005 20190218 G043G406900500001 BIB 2 3 G406900500002 REACTION (92-U-236(G,F)MASS,SEC,FY,,BRA/REL) G406900500003 The distributions were normalized at the maxima. G406900500004 SAMPLE (92-U-236,ENR=0.98) 186 micro-g/cm2 thickness G406900500005 ENDBIB 3 0 G406900500006 COMMON 1 3 G406900500007 EN-MAX G406900500008 MEV G406900500009 9. G406900500010 ENDCOMMON 3 0 G406900500011 DATA 3 25 G406900500012 MASS DATA DATA-ERR G406900500013 NO-DIM ARB-UNITS ARB-UNITS G406900500014 57.5 157. 13. G406900500015 62.3 210. 15. G406900500016 67.1 218. 17. G406900500017 71.8 322. 20. G406900500018 76.6 811. 34. G406900500019 81.4 1917. 53. G406900500020 86.2 4017. 78. G406900500021 90.9 6352. 96. G406900500022 95.7 6611. 101. G406900500023 100.5 5473. 93. G406900500024 105.5 3654. 79. G406900500025 110.0 1897. 65. G406900500026 114.8 1367. 58. G406900500027 119.6 1437. 64. G406900500028 124.4 2224. 72. G406900500029 129.1 3447. 83. G406900500030 133.9 4655. 93. G406900500031 138.7 5505. 99. G406900500032 143.5 5806. 100. G406900500033 148.2 4794. 92. G406900500034 153.0 3009. 73. G406900500035 157.8 1359. 51. G406900500036 162.6 419. 34. G406900500037 167.3 244. 26. G406900500038 172.1 45. 12. G406900500039 ENDDATA 27 0 G406900500040 ENDSUBENT 39 0 G406900599999 SUBENT G4069006 20190218 G043G406900600001 BIB 2 3 G406900600002 REACTION (92-U-238(G,F)MASS,SEC,FY,,BRA/REL) G406900600003 The distributions were normalized at the maxima. G406900600004 SAMPLE (92-U-238,NAT=0.992742) 233 micro-g/cm2 thickness G406900600005 ENDBIB 3 0 G406900600006 COMMON 1 3 G406900600007 EN-MAX G406900600008 MEV G406900600009 9. G406900600010 ENDCOMMON 3 0 G406900600011 DATA 3 17 G406900600012 MASS DATA DATA-ERR G406900600013 NO-DIM ARB-UNITS ARB-UNITS G406900600014 74.3 6.3 1.5 G406900600015 80.5 33.5 3.7 G406900600016 86.7 181.1 8.7 G406900600017 92.9 470. 13. G406900600018 99.1 635. 16. G406900600019 105.3 540. 15. G406900600020 111.5 292. 12. G406900600021 117.7 221. 11. G406900600022 123.9 318. 13. G406900600023 130.1 457. 14. G406900600024 136.3 614. 16. G406900600025 142.5 594. 16. G406900600026 148.7 391. 13. G406900600027 154.9 181.7 9.3 G406900600028 161.1 68.9 5.9 G406900600029 167.3 40.4 5.4 G406900600030 173.5 11.3 6.4 G406900600031 ENDDATA 19 0 G406900600032 ENDSUBENT 31 0 G406900699999 ENDENTRY 6 0 G406999999999