ENTRY D4409 20201127 D130D440900000001 SUBENT D4409001 20201127 D130D440900100001 BIB 12 49 D440900100002 TITLE Additional excitation functions for radionuclides D440900100003 obtained by deuteron irradiation of Ta up to 50 MeV D440900100004 AUTHOR (A.Hermanne,F.Tarkanyi,S.Takacs,F.Ditroi) D440900100005 INSTITUTE (2BLGVUB,3HUNDEB) D440900100006 REFERENCE (J,NIM/B,481,82,2020) D440900100007 #doi:10.1016/j.nimb.2020.09.007 D440900100008 FACILITY (CYCLO,2BLGLVN) D440900100009 SAMPLE High purity metalic natural Ta foils 8.63 um D440900100010 and Al for beam monitoring 10.8 5um. D440900100011 DETECTOR (HPGE) Canberra D440900100012 (XHPGE) Canberra D440900100013 METHOD (ACTIV,EXTB,EDEG,GSPEC,MOSEP,STTA) D440900100014 The foils were arranged in a 20 times repeated sequenceD440900100015 of Ir(45.57 um) - Al(10.85 um) - Al(49.64 um) - D440900100016 Ta(8.63 um) - Al(10.85 um) - Al(49.64 um). D440900100017 Irradiation was done in a Faraday-cup like targetholderD440900100018 with 50 MeV, 100 nA deuteron beam for 60 minutes. D440900100019 Four series of gamma measuremets were performed with D440900100020 cooling times of 5-6 h, 24-48 h, 4-7 d and 60-80 d. D440900100021 Additional measurements with extended range Ge-detectorD440900100022 for X-rays were taken after 90-199 d cooling time. D440900100023 No chemical separation was applied. D440900100024 Decay data were taken from NUDAT2 and Lund/LBNL online D440900100025 data libraries. D440900100026 The 48.72 MeV initial beam energy and 100 nA beam D440900100027 intensity was adopted in the data analysis as a good D440900100028 agreement was found between the re-measured excitation D440900100029 function and the recommended monitor reactions. D440900100030 MONITOR (13-AL-27(D,X)11-NA-24,,SIG) D440900100031 (13-AL-27(D,X)11-NA-22,,SIG) D440900100032 MONIT-REF (,A.HERMANNE+,J,NDS,148,338,2018) D440900100033 ERR-ANALYS (EN-ERR)The uncertainty on the median energy in the D440900100034 foils includes the cumulative effects of uncertainty ofD440900100035 incident beam energy, uncertainty of energy loss of D440900100036 each foil due to thickness variation and straggling D440900100037 effects. Uncertainty of the primary incident beam D440900100038 energy was +- 0.2 MeV which increased up to +- 2.2 MeV D440900100039 in the last foil of the stack. D440900100040 (ERR-T)The uncertainty on the cross section values D440900100041 are estimated in the standard way as the square root D440900100042 of the quadratic summation of the independently D440900100043 contributing parameters. Uncertainty of time parametersD440900100044 is not included. D440900100045 (ERR-1)surface density of target nuclei(5 %), D440900100046 (ERR-2)incident charged particle flux (5 %) D440900100047 (ERR-3) detector efficiency (5 %) D440900100048 (ERR-4,1.0,5.0) decay and branching data(1.0-5.0 %) D440900100049 (ERR-S,1.0,8.0)statistical and peak fitting (1.0-8.0 %)D440900100050 HISTORY (20201127C) TS D440900100051 ENDBIB 49 0 D440900100052 COMMON 3 3 D440900100053 ERR-1 ERR-2 ERR-3 D440900100054 PER-CENT PER-CENT PER-CENT D440900100055 5. 5. 5. D440900100056 ENDCOMMON 3 0 D440900100057 ENDSUBENT 56 0 D440900199999 SUBENT D4409002 20201127 D130D440900200001 BIB 3 7 D440900200002 REACTION (73-TA-181(D,6N)74-W-177,,SIG) D440900200003 DECAY-DATA (74-W-177,2.20HR,DG,186.2,0.2261, D440900200004 DG,377.35,0.0434, D440900200005 DG,426.98,0.125, D440900200006 DG,1036.4,0.097) D440900200007 STATUS (TABLE)Data are from Table2 of D440900200008 Journal of Nucl. Instr. Methods/B,481,82,2020 D440900200009 ENDBIB 7 0 D440900200010 NOCOMMON 0 0 D440900200011 DATA 4 7 D440900200012 EN EN-ERR DATA ERR-T D440900200013 MEV MEV MB MB D440900200014 48.6 0.2 263.5 29. D440900200015 46.9 0.2 186.2 20. D440900200016 45.1 0.3 108.1 12. D440900200017 43.3 0.4 50.4 6. D440900200018 41.9 0.5 20.6 2. D440900200019 40.5 0.6 5.7 1. D440900200020 39.1 0.7 1.2 0. D440900200021 ENDDATA 9 0 D440900200022 ENDSUBENT 21 0 D440900299999 SUBENT D4409003 20201127 D130D440900300001 BIB 3 5 D440900300002 REACTION (73-TA-181(D,5N)74-W-178,,SIG) D440900300003 DECAY-DATA (74-W-178,21.6D)No gamma, activity was determined D440900300004 from its decay product 178mTa. D440900300005 STATUS (TABLE)Data are from Table2 of D440900300006 Journal of Nucl. Instr. Methods/B,481,82,2020 D440900300007 ENDBIB 5 0 D440900300008 NOCOMMON 0 0 D440900300009 DATA 4 16 D440900300010 EN EN-ERR DATA ERR-T D440900300011 MEV MEV MB MB D440900300012 48.6 0.2 481. 53. D440900300013 46.9 0.2 569. 63. D440900300014 45.1 0.3 570. 63. D440900300015 43.3 0.4 662. 73. D440900300016 41.9 0.5 633. 70. D440900300017 40.5 0.6 605. 67. D440900300018 39.1 0.7 530. 58. D440900300019 37.6 0.8 447. 49. D440900300020 36.1 0.9 312. 34. D440900300021 34.5 1.0 192. 21. D440900300022 32.9 1.1 99. 11. D440900300023 31.3 1.2 27. 3. D440900300024 29.5 1.3 6.45 0.71 D440900300025 27.7 1.4 2.19 0.24 D440900300026 25.8 1.5 0.64 0.07 D440900300027 23.8 1.6 0.53 0.06 D440900300028 ENDDATA 18 0 D440900300029 ENDSUBENT 28 0 D440900399999 SUBENT D4409004 20201127 D130D440900400001 BIB 3 6 D440900400002 REACTION (73-TA-181(D,2N)74-W-181,,SIG) D440900400003 DECAY-DATA (74-W-181,121.2D,XR,57.53,0.32, D440900400004 XR,56.28,0.187, D440900400005 XR,65.22,0.07) D440900400006 STATUS (TABLE)Data are from Table2 of D440900400007 Journal of Nucl. Instr. Methods/B,481,82,2020 D440900400008 ENDBIB 6 0 D440900400009 NOCOMMON 0 0 D440900400010 DATA 4 9 D440900400011 EN EN-ERR DATA ERR-T D440900400012 MEV MEV MB MB D440900400013 31.3 1.2 74. 8. D440900400014 29.5 1.3 83. 9. D440900400015 27.7 1.4 88. 10. D440900400016 25.8 1.5 126. 14. D440900400017 23.8 1.6 136. 15. D440900400018 21.6 1.7 186. 20. D440900400019 19.3 1.8 242. 27. D440900400020 16.8 2.0 398. 44. D440900400021 13.9 2.2 466. 51. D440900400022 ENDDATA 11 0 D440900400023 ENDSUBENT 22 0 D440900499999 SUBENT D4409005 20201127 D130D440900500001 BIB 3 5 D440900500002 REACTION (73-TA-181(D,X)73-TA-177,CUM,SIG) D440900500003 DECAY-DATA (73-TA-177,56.56HR,DG,112.95,0.072, D440900500004 DG,208.,0.0094) D440900500005 STATUS (TABLE)Data are from Table3 of D440900500006 Journal of Nucl. Instr. Methods/B,481,82,2020 D440900500007 ENDBIB 5 0 D440900500008 NOCOMMON 0 0 D440900500009 DATA 4 11 D440900500010 EN EN-ERR DATA ERR-T D440900500011 MEV MEV MB MB D440900500012 48.6 0.2 389.3 43. D440900500013 46.9 0.2 269.6 30. D440900500014 45.1 0.3 157.9 17. D440900500015 43.3 0.4 73.3 8. D440900500016 41.9 0.5 31. 3. D440900500017 40.5 0.6 10.4 1. D440900500018 39.1 0.7 3.5 0. D440900500019 37.6 0.8 1.1 0. D440900500020 36.1 0.9 1.1 0. D440900500021 34.5 1.0 1.8 0. D440900500022 32.9 1.1 1.5 0. D440900500023 ENDDATA 13 0 D440900500024 ENDSUBENT 23 0 D440900599999 SUBENT D4409006 20201127 D130D440900600001 BIB 3 6 D440900600002 REACTION (73-TA-181(D,X)73-TA-178-G,,SIG) D440900600003 DECAY-DATA (73-TA-178-G,2.36HR,DG,213.4,0.81, D440900600004 DG,325.,0.94, D440900600005 DG,331.6,0.312) D440900600006 STATUS (TABLE)Data are from Table3 of D440900600007 Journal of Nucl. Instr. Methods/B,481,82,2020 D440900600008 ENDBIB 6 0 D440900600009 NOCOMMON 0 0 D440900600010 DATA 4 20 D440900600011 EN EN-ERR DATA ERR-T D440900600012 MEV MEV MB MB D440900600013 48.6 0.2 44. 5. D440900600014 46.9 0.2 36. 4. D440900600015 45.1 0.3 28. 3. D440900600016 43.3 0.4 20. 2. D440900600017 41.9 0.5 14. 2. D440900600018 40.5 0.6 10. 1.1 D440900600019 39.1 0.7 7. 0.8 D440900600020 37.6 0.8 4.7 0.5 D440900600021 36.1 0.9 3.2 0.4 D440900600022 34.5 1.0 2.5 0.3 D440900600023 32.9 1.1 1.7 0.2 D440900600024 31.3 1.2 1.2 0.1 D440900600025 29.5 1.3 0.9 0.1 D440900600026 27.7 1.4 0.58 0.06 D440900600027 25.8 1.5 0.41 0.05 D440900600028 23.8 1.6 0.33 0.04 D440900600029 21.6 1.7 0.43 0.05 D440900600030 19.3 1.8 0.31 0.03 D440900600031 16.8 2.0 0.35 0.04 D440900600032 13.9 2.2 0.38 0.04 D440900600033 ENDDATA 22 0 D440900600034 ENDSUBENT 33 0 D440900699999 SUBENT D4409007 20201127 D130D440900700001 BIB 3 5 D440900700002 REACTION (73-TA-181(D,X)73-TA-180-G,,SIG) D440900700003 DECAY-DATA (73-TA-180-G,8.154HR,DG,93.,0.045, D440900700004 DG,103.6,0.0087) D440900700005 STATUS (TABLE)Data are from Table3 of D440900700006 Journal of Nucl. Instr. Methods/B,481,82,2020 D440900700007 ENDBIB 5 0 D440900700008 NOCOMMON 0 0 D440900700009 DATA 4 20 D440900700010 EN EN-ERR DATA ERR-T D440900700011 MEV MEV MB MB D440900700012 48.6 0.2 120.24 13. D440900700013 46.9 0.2 127.42 14. D440900700014 45.1 0.3 127.48 14. D440900700015 43.3 0.4 134.81 15. D440900700016 41.9 0.5 136.6 15. D440900700017 40.5 0.6 140.7 15. D440900700018 39.1 0.7 151.85 17. D440900700019 37.6 0.8 152.08 17. D440900700020 36.1 0.9 140.61 15. D440900700021 34.5 1.0 139.7 15. D440900700022 32.9 1.1 136.9 15. D440900700023 31.3 1.2 130.1 14. D440900700024 29.5 1.3 105.47 12. D440900700025 27.7 1.4 94.83 10. D440900700026 25.8 1.5 70.67 8. D440900700027 23.8 1.6 47.87 5. D440900700028 21.6 1.7 31.64 3. D440900700029 19.3 1.8 24.82 3. D440900700030 16.8 2.0 29.41 3. D440900700031 13.9 2.2 13.38 1. D440900700032 ENDDATA 22 0 D440900700033 ENDSUBENT 32 0 D440900799999 SUBENT D4409008 20201127 D130D440900800001 BIB 3 6 D440900800002 REACTION (73-TA-181(D,P)73-TA-182,,SIG) D440900800003 DECAY-DATA (73-TA-182-G,114.74D,DG,1121.,0.3524, D440900800004 DG,1221.,0.2723, D440900800005 DG,1189.,0.1649) D440900800006 STATUS (TABLE)Data are from Table3 of D440900800007 Journal of Nucl. Instr. Methods/B,481,82,2020 D440900800008 ENDBIB 6 0 D440900800009 NOCOMMON 0 0 D440900800010 DATA 4 20 D440900800011 EN EN-ERR DATA ERR-T D440900800012 MEV MEV MB MB D440900800013 48.6 0.2 27. 3. D440900800014 46.9 0.2 27. 3. D440900800015 45.1 0.3 29. 3. D440900800016 43.3 0.4 32. 3. D440900800017 41.9 0.5 34. 4. D440900800018 40.5 0.6 33. 4. D440900800019 39.1 0.7 38. 4. D440900800020 37.6 0.8 41. 4. D440900800021 36.1 0.9 43. 5. D440900800022 34.5 1.0 48. 5. D440900800023 32.9 1.1 53. 6. D440900800024 31.3 1.2 57. 6. D440900800025 29.5 1.3 61. 7. D440900800026 27.7 1.4 70. 8. D440900800027 25.8 1.5 79. 9. D440900800028 23.8 1.6 89. 10. D440900800029 21.6 1.7 108. 12. D440900800030 19.3 1.8 131. 14. D440900800031 16.8 2.0 158. 17. D440900800032 13.9 2.2 183. 20. D440900800033 ENDDATA 22 0 D440900800034 ENDSUBENT 33 0 D440900899999 SUBENT D4409009 20201127 D130D440900900001 BIB 3 5 D440900900002 REACTION (73-TA-181(D,X)72-HF-175,,SIG) D440900900003 DECAY-DATA (72-HF-175,70.0D,DG,343.8,0.84, D440900900004 DG,433.,0.0144) D440900900005 STATUS (TABLE)Data are from Table2 of D440900900006 Journal of Nucl. Instr. Methods/B,481,82,2020 D440900900007 ENDBIB 5 0 D440900900008 NOCOMMON 0 0 D440900900009 DATA 4 9 D440900900010 EN EN-ERR DATA ERR-T D440900900011 MEV MEV MB MB D440900900012 48.6 0.2 14.0 1.8 D440900900013 46.9 0.2 11.4 1.5 D440900900014 45.1 0.3 8.2 1.1 D440900900015 43.3 0.4 5.7 0.7 D440900900016 41.9 0.5 3.5 0.5 D440900900017 40.5 0.6 2.1 0.3 D440900900018 39.1 0.7 0.95 0.14 D440900900019 37.6 0.8 0.43 0.06 D440900900020 36.1 0.9 0.07 0.01 D440900900021 ENDDATA 11 0 D440900900022 ENDSUBENT 21 0 D440900999999 SUBENT D4409010 20201127 D130D440901000001 BIB 3 5 D440901000002 REACTION (73-TA-181(D,X)72-HF-179-M2,,SIG) D440901000003 DECAY-DATA (72-HF-179-M2,25.05D,DG,362.,0.396, D440901000004 DG,453.,0.68) D440901000005 STATUS (TABLE)Data are from Table2 of D440901000006 Journal of Nucl. Instr. Methods/B,481,82,2020 D440901000007 ENDBIB 5 0 D440901000008 NOCOMMON 0 0 D440901000009 DATA 4 19 D440901000010 EN EN-ERR DATA ERR-T D440901000011 MEV MEV MB MB D440901000012 48.6 0.2 0.22 0.02 D440901000013 46.9 0.2 0.17 0.02 D440901000014 45.1 0.3 0.18 0.02 D440901000015 43.3 0.4 0.2 0.02 D440901000016 41.9 0.5 0.14 0.02 D440901000017 40.5 0.6 0.2 0.02 D440901000018 39.1 0.7 0.11 0.01 D440901000019 37.6 0.8 0.1 0.01 D440901000020 36.1 0.9 0.11 0.01 D440901000021 34.5 1.0 0.1 0.01 D440901000022 32.9 1.1 0.18 0.02 D440901000023 31.3 1.2 0.12 0.01 D440901000024 29.5 1.3 0.23 0.02 D440901000025 27.7 1.4 0.09 0.01 D440901000026 25.8 1.5 0.18 0.02 D440901000027 23.8 1.6 0.15 0.02 D440901000028 21.6 1.7 0.18 0.02 D440901000029 19.3 1.8 0.16 0.02 D440901000030 16.8 2.0 0.12 0.01 D440901000031 ENDDATA 21 0 D440901000032 ENDSUBENT 31 0 D440901099999 SUBENT D4409011 20201127 D130D440901100001 BIB 3 6 D440901100002 REACTION (73-TA-181(D,X)72-HF-180-M,,SIG) D440901100003 DECAY-DATA (72-HF-180-M,5.53HR,DG,332.27,0.94, D440901100004 DG,443.16,0.817, D440901100005 DG,500.69,0.142) D440901100006 STATUS (TABLE)Data are from Table2 of D440901100007 Journal of Nucl. Instr. Methods/B,481,82,2020 D440901100008 ENDBIB 6 0 D440901100009 NOCOMMON 0 0 D440901100010 DATA 4 12 D440901100011 EN EN-ERR DATA ERR-T D440901100012 MEV MEV MB MB D440901100013 48.6 0.2 0.96 0.14 D440901100014 46.9 0.2 0.7 0.11 D440901100015 45.1 0.3 0.66 0.1 D440901100016 43.3 0.4 0.6 0.09 D440901100017 41.9 0.5 0.54 0.08 D440901100018 40.5 0.6 0.32 0.05 D440901100019 39.1 0.7 0.3 0.05 D440901100020 37.6 0.8 0.3 0.05 D440901100021 36.1 0.9 0.24 0.04 D440901100022 34.5 1.0 0.18 0.03 D440901100023 32.9 1.1 0.16 0.02 D440901100024 31.3 1.2 0.15 0.02 D440901100025 ENDDATA 14 0 D440901100026 ENDSUBENT 25 0 D440901199999 SUBENT D4409012 20201127 D130D440901200001 BIB 3 6 D440901200002 REACTION (73-TA-181(D,2P)72-HF-181,,SIG) D440901200003 DECAY-DATA (72-HF-181,42.39D,DG,133.,0.433, D440901200004 DG,345.9,0.152, D440901200005 DG,482.,0.805) D440901200006 STATUS (TABLE)Data are from Table2 of D440901200007 Journal of Nucl. Instr. Methods/B,481,82,2020 D440901200008 ENDBIB 6 0 D440901200009 NOCOMMON 0 0 D440901200010 DATA 4 13 D440901200011 EN EN-ERR DATA ERR-T D440901200012 MEV MEV MB MB D440901200013 48.6 0.2 1.02 0.15 D440901200014 46.9 0.2 0.84 0.13 D440901200015 45.1 0.3 0.67 0.1 D440901200016 43.3 0.4 0.76 0.11 D440901200017 41.9 0.5 0.62 0.09 D440901200018 40.5 0.6 0.48 0.07 D440901200019 39.1 0.7 0.5 0.07 D440901200020 37.6 0.8 0.42 0.06 D440901200021 36.1 0.9 0.32 0.05 D440901200022 34.5 1.0 0.3 0.04 D440901200023 32.9 1.1 0.17 0.03 D440901200024 31.3 1.2 0.22 0.03 D440901200025 29.5 1.3 0.07 0.01 D440901200026 ENDDATA 15 0 D440901200027 ENDSUBENT 26 0 D440901299999 ENDENTRY 12 0 D440999999999