ENTRY B0113 20190123 B029B011300000001 SUBENT B0113001 20190123 B029B011300100001 BIB 11 46 B011300100002 TITLE Excitation functions for quasielastic transfer B011300100003 reactions induced with heavy ions in bismuth B011300100004 AUTHOR (D.Gardes, R.Bimbot, J.Maison, L.De Relihac, B011300100005 M.F.Rivet, A.Fleury, F.Hubert, Y.Llabador) B011300100006 INSTITUTE (2FR PAR,2FR GRA) B011300100007 REFERENCE (J,PR/C,18,1298,1978) B011300100008 FACILITY (ISOCY,2FR PAR) Alice ORSAY accelerator B011300100009 SAMPLE Natural elemental sample (1 to 1.5 mg/cm2 thick) B011300100010 evaporated onto an Al-foil. B011300100011 Additional Al foils served As catchers and were countedB011300100012 together with the target foils. B011300100013 METHOD (SITA,EDEG) Depending on the incident beam and energy, B011300100014 a single target or stacked targets were chosen. B011300100015 The incident energy was varied either by changing the B011300100016 acceleration parameters, or by using Al degraders. B011300100017 In the latter case, the energy reduction was B011300100018 calculated by means of the range-energy table of B011300100019 L.C.Northcliffe (1970). B011300100020 REL-REF (R,,L.C.Northcliffe+,J,ND/A,7,233,1970) B011300100021 range-energy table B011300100022 CRITIQUE The range-energy values of NORTHCLIFFE contain B011300100023 systematic errors (R.Bimbot et al., nucl.Instr.Meth. B011300100024 153(1978)161). It is unknown whether or not B011300100025 corrections for these errors were applied here. B011300100026 ERR-ANALYS (EN-ERR) Including B011300100027 - errors of the energy of the incident beam, B011300100028 - uncertainties on energy losses in Al degraders. B011300100029 This last error was estimated to be 15% of the energy B011300100030 loss. B011300100031 (ERR-T) The uncertainties on cross sections include, B011300100032 (ERR-1) beam flux measurement (2%), B011300100033 (ERR-2) target thickness and homogeneity (5%), B011300100034 (ERR-3,2.,10.) counting efficiencies for alpha, B011300100035 (ERR-4) counting efficiencies for gamma (4%), B011300100036 (ERR-5,5.,10.) branching ratios for gamma emitters, B011300100037 (ERR-6,5.,10.) statistical errors of activities. B011300100038 HISTORY (19800229C) Lakw B011300100039 (19940714A) Some corrections have been included by B011300100040 CAJAD. B011300100041 (19981229A) Reacion lines are corrected. Lower case. B011300100042 (20020111A) V.Mc-lane'S remarks are included B011300100043 (20180522U) On. Author corrected. B011300100044 (20190123A) So NDS. Corrected SF3: use X for 043.1. B011300100045 Deleted SF9=EXP from all subentries. B011300100046 Added STATUS in all subentries. B011300100047 (20190507A) So NDS. Delete SF5=IND from all subentries.B011300100048 ENDBIB 46 0 B011300100049 NOCOMMON 0 0 B011300100050 ENDSUBENT 49 0 B011300199999 SUBENT B0113002 20190123 B029B011300200001 BIB 7 16 B011300200002 REACTION (83-BI-209(6-C-12,X)83-BI-210-G,,SIG) B011300200003 COMMENT - by authors - alpha- and beta-decaying precursors may B011300200004 contribute, the cross sections are, however, probably B011300200005 small. B011300200006 RAD-DET (84-PO-210,A) B011300200007 DECAY-DATA (83-BI-210-G,5.01D) B011300200008 (84-PO-210,138.4D,A,5305.,1.) B011300200009 METHOD (EXTB,BCINT,STTA,SITA,CHSEP,EDEG,REC) B011300200010 Bi-210 was determined via Po-210. 48 hours after B011300200011 irradiation the target and catcher foils were dissolvedB011300200012 and Po-210 was separated by spontaneous deposition B011300200013 on Ag. Bi-210 remained in solution. Six days later, a B011300200014 second separation was performed giving Po-210 obtained B011300200015 from the decay of Bi-210. B011300200016 DETECTOR (IOCH) 2-pi ionization chamber B011300200017 STATUS (TABLE) Table II in Phys.Rev.C.18,1298,1978 B011300200018 ENDBIB 16 0 B011300200019 NOCOMMON 0 0 B011300200020 DATA 5 4 B011300200021 EN EN-ERR DATA DATA-MAX ERR-T B011300200022 MEV MEV MB MB MB B011300200023 68.5 4.5 1.3 B011300200024 74. 3.5 1.3 B011300200025 79. 3. 1.5 0.7 B011300200026 87. 2. 0.8 0.6 B011300200027 ENDDATA 6 0 B011300200028 ENDSUBENT 27 0 B011300299999 SUBENT B0113003 20190123 B029B011300300001 BIB 7 25 B011300300002 REACTION 1(83-BI-209(6-C-12,X)84-PO-210,(CUM),SIG) B011300300003 2(83-BI-209(6-C-12,X)84-PO-210,CUM,SIG) B011300300004 DECAY-DATA (84-PO-210,138.4D,A,5305.,1.) B011300300005 1(83-BI-210-G,5.01D) B011300300006 (85-AT-210,8.3HR,DG,245.,0.79,DG,1180.,1.) B011300300007 METHOD (EXTB,BCINT,STTA,SITA,CHSEP,EDEG,REC) B011300300008 COMMENT 1THE possible production of Po-210 from at-210 and B011300300009 Bi-210 was considered. The cross section for at-210 B011300300010 production was directly measured by its gamma ray B011300300011 emission, see under 'REL-REF'. Bi-210 was determined B011300300012 via Po-210. 48 hours after irradiation the target and B011300300013 catcher foils were dissolved and Po-210 was separated B011300300014 by spontaneous deposition on Ag. Bi-210 remained in B011300300015 solution. Six days later a second separation was B011300300016 performed giving Po-210 obtained from the decay of B011300300017 Bi-210. B011300300018 DETECTOR (IOCH) 2-pi ionization chamber B011300300019 REL-REF (N,B0126001,R.Bimbot+,J,NP/A,189,193,1972) B011300300020 from this earlier publication data on At-210 (As well B011300300021 As on At-211 and At-209) are cited in the present B011300300022 paper. B011300300023 STATUS (TABLE) Table II in Phys.Rev.C.18,1298,1978 B011300300024 1(DEP,B0113003) B011300300025 (DEP,B0113002) B011300300026 (DEP,B0126003) B011300300027 ENDBIB 25 0 B011300300028 NOCOMMON 0 0 B011300300029 DATA 7 4 B011300300030 EN EN-ERR DATA 1DATA-MAX 1ERR-T 1DATA 2B011300300031 ERR-T 2 B011300300032 MEV MEV MB MB MB MB B011300300033 MB B011300300034 68.5 4.5 20. 122.B011300300035 45. B011300300036 74. 3.5 20. 107.B011300300037 40. B011300300038 79. 3. 33. 30. 77.B011300300039 20. B011300300040 87. 2. 54. 40. 108.B011300300041 30. B011300300042 ENDDATA 12 0 B011300300043 ENDSUBENT 42 0 B011300399999 SUBENT B0113004 20190123 B029B011300400001 BIB 7 17 B011300400002 REACTION 1(83-BI-209(7-N-14,X)85-AT-211,,SIG) B011300400003 2(83-BI-209(7-N-14,X)86-RN-211,CUM,SIG) B011300400004 RAD-DET (84-PO-211-G,A) B011300400005 DECAY-DATA (86-RN-211,14.6HR,A,5850.,0.26) B011300400006 (85-AT-211,7.2HR,A,5868.,0.409) B011300400007 (84-PO-211-G,0.52SEC,A,7448.,1.) In equilibrium with B011300400008 at-211. B011300400009 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011300400010 ANALYSIS (DECAY) The decay curve of the 7.448 MeV alpha peak wasB011300400011 resolved into two components resulting from the B011300400012 exponential decay of At-211 and the accumulation of B011300400013 at-211 from Rn-211 if present. B011300400014 a direct analysis of the complex alpha peaks of Rn-211 B011300400015 and At-211 was obviously impossible As stated in B011300400016 earlier papers, see under 'comment'. B011300400017 DETECTOR (IOCH) 2-pi ionization chamber B011300400018 STATUS (TABLE) Table III in Phys.Rev.C.18,1298,1978 B011300400019 ENDBIB 17 0 B011300400020 NOCOMMON 0 0 B011300400021 DATA 6 18 B011300400022 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2B011300400023 MEV MEV MB MB MB MB B011300400024 61. 3.5 0.0001 0.0001 B011300400025 66. 3. 0.0004 0.0001 B011300400026 69. 2.5 0.0044 0.001 B011300400027 69. 2. 0.016 0.002 0.0046 0.0006B011300400028 72. 2. 0.08 0.02 0.03 0.007B011300400029 73. 1.5 0.44 0.06 0.66 0.09B011300400030 77. 1.5 1.15 0.18 1.3 0.2B011300400031 81. 3.5 3.1 0.5 6.3 1.B011300400032 84. 3.5 5.4 0.9 9.5 1.5B011300400033 87. 3. 7.7 1.2 7.9 1.2B011300400034 91. 3. 9.5 1.5 10.7 1.7B011300400035 94. 2. 10. 1.6 15.8 2.5B011300400036 97. 2. 11. 1.7 21.6 3.4B011300400037 98. 2. 11. 1.2 18.6 2.7B011300400038 115. 9. 10.4 1.2 18.3 2.7B011300400039 129. 7. 13. 1.5 14.9 2.2B011300400040 143. 5. 12.2 1.4 18.3 2.7B011300400041 159. 3. 11.4 1.3 13.9 2.B011300400042 ENDDATA 20 0 B011300400043 ENDSUBENT 42 0 B011300499999 SUBENT B0113005 20190123 B029B011300500001 BIB 7 18 B011300500002 REACTION (83-BI-209(7-N-14,X)83-BI-210-G,,SIG) B011300500003 The authors assume the cross section mostly to be due B011300500004 to a one-neutron transfer reaction (6N+7P). B011300500005 COMMENT - by authors - alpha- and beta-decaying precursors may B011300500006 contribute, the cross sections are, however, probably B011300500007 small. B011300500008 RAD-DET (84-PO-210,A) B011300500009 DECAY-DATA (83-BI-210-G,5.01D) B011300500010 (84-PO-210,138.4D,A,5305.,1.) B011300500011 METHOD (EXTB,BCINT,STTA,SITA,CHSEP,EDEG,REC) B011300500012 Bi-210 was determined via Po-210. 48 hours after B011300500013 irradiation the target and catcher foils were dissolvedB011300500014 and Po-210 was separated by spontaneous deposition B011300500015 on Ag. Bi-210 remained in solution. Six days later, a B011300500016 second separation was performed giving Po-210 obtained B011300500017 from the decay of Bi-210. B011300500018 DETECTOR (IOCH) 2-pi ionization chamber B011300500019 STATUS (TABLE) Table III in Phys.Rev.C.18,1298,1978 B011300500020 ENDBIB 18 0 B011300500021 NOCOMMON 0 0 B011300500022 DATA 5 4 B011300500023 EN EN-ERR DATA DATA-MAX ERR-T B011300500024 MEV MEV MB MB MB B011300500025 77. 1.5 0.4 B011300500026 84. 3.5 3.6 1.8 B011300500027 91. 3. 8. 2.4 B011300500028 97. 2. 8.7 2.6 B011300500029 ENDDATA 6 0 B011300500030 ENDSUBENT 29 0 B011300599999 SUBENT B0113006 20190123 B029B011300600001 BIB 5 6 B011300600002 REACTION (83-BI-209(7-N-14,X)84-PO-210,CUM,SIG) B011300600003 DECAY-DATA (83-BI-210-G,5.01D) B011300600004 (84-PO-210,138.4D,A,5305.,1.) B011300600005 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011300600006 DETECTOR (IOCH) 2-pi ionization chamber B011300600007 STATUS (TABLE) Table III in Phys.Rev.C.18,1298,1978 B011300600008 ENDBIB 6 0 B011300600009 NOCOMMON 0 0 B011300600010 DATA 4 19 B011300600011 EN EN-ERR DATA ERR-T B011300600012 MEV MEV MB MB B011300600013 61. 3.5 0.4 0.09 B011300600014 65. 3. 0.6 1.2 B011300600015 66. 3. 1.6 0.33 B011300600016 69. 2.5 5.1 1. B011300600017 69. 2. 6.2 1.3 B011300600018 72. 2. 15. 3. B011300600019 73. 1.5 19. 4. B011300600020 77. 1.5 18. 3.6 B011300600021 81. 3.5 37. 8. B011300600022 84. 3.5 39. 8. B011300600023 87. 3. 49. 11. B011300600024 91. 3. 47. 11. B011300600025 94. 2. 57. 12. B011300600026 97. 2. 52. 12. B011300600027 98. 2. 52. 5. B011300600028 115. 9. 62. 5.7 B011300600029 129. 7. 72. 6.5 B011300600030 143. 5. 62. 6. B011300600031 159. 3. 80. 7. B011300600032 ENDDATA 21 0 B011300600033 ENDSUBENT 32 0 B011300699999 SUBENT B0113007 20190123 B029B011300700001 BIB 7 16 B011300700002 REACTION (83-BI-209(8-O-16,X)85-AT-211,,SIG) B011300700003 RAD-DET (84-PO-211-G,A) B011300700004 DECAY-DATA (86-RN-211,14.6HR,A,5850.,0.26) B011300700005 (85-AT-211,7.2HR,A,5868.,0.409) B011300700006 (84-PO-211-G,0.52SEC,A,7448.,1.) In equilibrium with B011300700007 at-211. B011300700008 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011300700009 ANALYSIS (DECAY) The decay curve of the 7.448 MeV alpha peak wasB011300700010 resolved into two components resulting from the B011300700011 exponential decay of At-211 and the accumulation of B011300700012 At-211 from Rn-211 if present. B011300700013 a direct analysis of the complex alpha peaks of Rn-211 B011300700014 and At-211 was obviously impossible As stated in B011300700015 earlier papers, see under 'comment'. B011300700016 DETECTOR (IOCH) 2-pi ionization chamber B011300700017 STATUS (TABLE) Table IV in Phys.Rev.C.18,1298,1978 B011300700018 ENDBIB 16 0 B011300700019 NOCOMMON 0 0 B011300700020 DATA 4 12 B011300700021 EN EN-ERR DATA ERR-T B011300700022 MEV MEV MB MB B011300700023 58. 5. 0.00027 0.00013 B011300700024 62. 4. 0.0004 0.0002 B011300700025 63. 7. 0.0005 0.00025 B011300700026 67. 4. 0.0011 0.0005 B011300700027 72. 6. 0.004 0.002 B011300700028 77. 2.5 0.05 0.01 B011300700029 77. 5. 0.1 0.015 B011300700030 82. 2. 6.3 1. B011300700031 83. 2. 7.4 1. B011300700032 88. 4. 24. 3. B011300700033 94. 3. 34.5 3.5 B011300700034 99. 2.5 33. 4. B011300700035 ENDDATA 14 0 B011300700036 ENDSUBENT 35 0 B011300799999 SUBENT B0113008 20190123 B029B011300800001 BIB 6 10 B011300800002 REACTION (83-BI-209(8-O-16,X)85-AT-210,(CUM),SIG) B011300800003 COMMENT - by authors - alpha- and beta-decaying precursors may B011300800004 contribute, the cross sections are, however, probably B011300800005 small. B011300800006 -by compiler - Rn-210 may contribute, its electron B011300800007 capture branch is 4%. B011300800008 DECAY-DATA (85-AT-210,8.3HR,DG,245.,0.79,DG,1180.,1.) B011300800009 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011300800010 DETECTOR (GELI) B011300800011 STATUS (TABLE) Table IV in Phys.Rev.C.18,1298,1978 B011300800012 ENDBIB 10 0 B011300800013 NOCOMMON 0 0 B011300800014 DATA 4 4 B011300800015 EN EN-ERR DATA ERR-T B011300800016 MEV MEV MB MB B011300800017 83. 2. 0.24 0.12 B011300800018 88. 4. 6.8 0.9 B011300800019 94. 3. 18.2 1.6 B011300800020 99. 2.5 22.6 2.2 B011300800021 ENDDATA 6 0 B011300800022 ENDSUBENT 21 0 B011300899999 SUBENT B0113009 20190123 B029B011300900001 BIB 7 18 B011300900002 REACTION (83-BI-209(8-O-16,X)83-BI-210-G,,SIG) B011300900003 The authors assume the cross section mostly to be due B011300900004 to a one-neutron transfer reaction (7N+8P) B011300900005 COMMENT - by authors - alpha- and beta-decaying precursors may B011300900006 contribute, the cross sections are, however, probably B011300900007 small. B011300900008 RAD-DET (84-PO-210,A) B011300900009 DECAY-DATA (83-BI-210-G,5.01D) B011300900010 (84-PO-210,138.4D,A,5305.,1.) B011300900011 METHOD (EXTB,BCINT,STTA,SITA,CHSEP,EDEG,REC) B011300900012 Bi-210 was determined via Po-210. 48 hours after B011300900013 irradiation the target and catcher foils were dissolvedB011300900014 and Po-210 was separated by spontaneous deposition B011300900015 on Ag. Bi-210 remained in solution. Six days later, a B011300900016 second separation was performed giving Po-210 obtained B011300900017 from the decay of Bi-210. B011300900018 DETECTOR (IOCH) 2-pi ionization chamber B011300900019 STATUS (TABLE) Table IV in Phys.Rev.C.18,1298,1978 B011300900020 ENDBIB 18 0 B011300900021 NOCOMMON 0 0 B011300900022 DATA 5 3 B011300900023 EN EN-ERR DATA DATA-MAX ERR-T B011300900024 MEV MEV MB MB MB B011300900025 83. 2. 0.5 B011300900026 88. 4. 1.5 B011300900027 99. 2.5 2.8 2.8 B011300900028 ENDDATA 5 0 B011300900029 ENDSUBENT 28 0 B011300999999 SUBENT B0113010 20190123 B029B011301000001 BIB 6 20 B011301000002 REACTION 1(83-BI-209(8-O-16,X)84-PO-210,(CUM),SIG) B011301000003 2(83-BI-209(8-O-16,X)84-PO-210,CUM,SIG) B011301000004 DECAY-DATA (84-PO-210,138.4D,A,5305.,1.) B011301000005 1(83-BI-210-G,5.01D) B011301000006 (85-AT-210,8.3HR,DG,245.,0.79,DG,1180.,1.) B011301000007 METHOD (EXTB,BCINT,STTA,SITA,CHSEP,EDEG,REC) B011301000008 DETECTOR (IOCH) 2-pi ionization chamber B011301000009 COMMENT 1THE possible production of Po-210 from At-210 and B011301000010 Bi-210 was considered. The cross section for At-210 B011301000011 production was directly measured by its gamma ray B011301000012 emission. Bi-210 was determined via Po-210. 48 hours B011301000013 after irradiation the target and catcher foils were B011301000014 dissolved and Po-210 was separated by spontaneous B011301000015 deposition on Ag. Bi-210 remained in solution. Six B011301000016 days later a second separation was performed giving B011301000017 Po-210 obtained from the decay of Bi-210. B011301000018 STATUS (TABLE) Table IV in Phys.Rev.C.18,1298,1978 B011301000019 1(DEP,B0113010) B011301000020 (DEP,B0113008) B011301000021 (DEP,B0113009) B011301000022 ENDBIB 20 0 B011301000023 NOCOMMON 0 0 B011301000024 DATA 6 5 B011301000025 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2B011301000026 MEV MEV MB MB MB MB B011301000027 77. 5. 0.008 0.001 0.008 0.001B011301000028 82. 2. 0.05 0.005 0.05 0.005B011301000029 83. 2. 31. 9. 31. 9.B011301000030 88. 4. 57. 11. 64. 10.B011301000031 94. 3. 51. 15. 69. 14.B011301000032 ENDDATA 7 0 B011301000033 ENDSUBENT 32 0 B011301099999 SUBENT B0113011 20190123 B029B011301100001 BIB 9 20 B011301100002 REACTION (83-BI-209(9-F-19,X)85-AT-211,,SIG) B011301100003 RAD-DET (84-PO-211-G,A) B011301100004 DECAY-DATA (86-RN-211,14.6HR,A,5850.,0.26) B011301100005 (85-AT-211,7.2HR,A,5868.,0.409) B011301100006 (84-PO-211-G,0.52SEC,A,7448.,1.) In equilibrium with B011301100007 at-211. B011301100008 FACILITY (VDGT,2FR PAR). For IRRADIATIONS with energies at and B011301100009 below 109 MeV B011301100010 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011301100011 ANALYSIS (DECAY) The decay curve of the 7.448 MeV alpha peak wasB011301100012 resolved into two components resulting from the B011301100013 exponential decay of At-211 and the accumulation of B011301100014 At-211 from Rn-211 if present. B011301100015 a direct analysis of the complex alpha peaks of Rn-211 B011301100016 and At-211 was obviously impossible As stated in B011301100017 earlier papers, see under 'comment'. B011301100018 DETECTOR (IOCH) 2-pi ionization chamber B011301100019 ERR-ANALYS The energy of the F-19 beam of the tandem accelerator B011301100020 was measured with an accuracy better than 0.1%. B011301100021 STATUS (TABLE) Table V in Phys.Rev.C.18,1298,1978 B011301100022 ENDBIB 20 0 B011301100023 NOCOMMON 0 0 B011301100024 DATA 4 17 B011301100025 EN EN-ERR DATA ERR-T B011301100026 MEV MEV MB MB B011301100027 78.7 0.3 0.001 0.0005 B011301100028 81.6 0.3 0.006 0.002 B011301100029 83.7 0.3 0.016 0.004 B011301100030 87. 0.3 0.22 0.04 B011301100031 89. 0.3 0.39 0.04 B011301100032 91.5 0.3 1.88 0.26 B011301100033 94. 0.3 2.5 0.3 B011301100034 99. 0.3 5. 0.4 B011301100035 104.5 0.3 15.5 1.7 B011301100036 109. 0.3 19. 3. B011301100037 109. 14. 18.2 1.5 B011301100038 119. 13. 25.9 2.1 B011301100039 132.5 13. 21.1 1.7 B011301100040 151.5 10. 23. 1.8 B011301100041 169.5 7. 26.4 2. B011301100042 184. 3.7 24.1 2. B011301100043 185.5 3.7 23. 1.8 B011301100044 ENDDATA 19 0 B011301100045 ENDSUBENT 44 0 B011301199999 SUBENT B0113012 20190123 B029B011301200001 BIB 8 14 B011301200002 REACTION (83-BI-209(9-F-19,X)85-AT-210,(CUM),SIG) B011301200003 COMMENT - by authors - alpha- and beta-decaying precursors may B011301200004 contribute, the cross sections are, however, probably B011301200005 small. B011301200006 - by compiler - Rn-210 may contribute, its electron B011301200007 capture branch is 4%. B011301200008 DECAY-DATA (85-AT-210,8.3HR,DG,245.,0.79,DG,1180.,1.) B011301200009 FACILITY (VDGT,2FR PAR). For IRRADIATIONS with energies at and B011301200010 below 109 MeV. B011301200011 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011301200012 DETECTOR (GELI) B011301200013 ERR-ANALYS The energy of the F-19 beam of the tandem accelerator B011301200014 was measured with an accuracy better than 0.1%. B011301200015 STATUS (TABLE) Table V in Phys.Rev.C.18,1298,1978 B011301200016 ENDBIB 14 0 B011301200017 NOCOMMON 0 0 B011301200018 DATA 4 10 B011301200019 EN EN-ERR DATA ERR-T B011301200020 MEV MEV MB MB B011301200021 94. 0.3 0.16 0.13 B011301200022 99. 0.3 0.51 0.15 B011301200023 104.5 0.3 2.9 0.2 B011301200024 109. 0.3 4.2 0.2 B011301200025 109. 14. 7.5 0.9 B011301200026 119. 13. 12. 1.5 B011301200027 132.5 13. 17. 4. B011301200028 151.5 10. 24.6 1. B011301200029 169.5 7. 31.6 1. B011301200030 185.5 3.7 31.4 1. B011301200031 ENDDATA 12 0 B011301200032 ENDSUBENT 31 0 B011301299999 SUBENT B0113013 20190123 B029B011301300001 BIB 6 14 B011301300002 REACTION 1(83-BI-209(9-F-19,X)85-AT-209,,SIG) B011301300003 2(83-BI-209(9-F-19,X)85-AT-208,,SIG) B011301300004 3(83-BI-209(9-F-19,X)85-AT-207,,SIG) B011301300005 COMMENT - by authors - alpha- and beta-decaying precursors may B011301300006 contribute, the cross sections are, however, probably B011301300007 small. B011301300008 DECAY-DATA1(85-AT-209,5.42HR,A,5660.,0.041, B011301300009 DG,545.,0.62, B011301300010 DG,782.,0.58) B011301300011 2(85-AT-208,1.63HR,DG,660.,0.92,DG,685.,0.99) B011301300012 3(85-AT-207,1.8HR,DG,814.,1.) B011301300013 METHOD (EXTB,BCINT,SITA,REC) B011301300014 DETECTOR (GELI) B011301300015 STATUS (TABLE) Table V in Phys.Rev.C.18,1298,1978 B011301300016 ENDBIB 14 0 B011301300017 NOCOMMON 0 0 B011301300018 DATA 8 1 B011301300019 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2B011301300020 DATA 3ERR-T 3 B011301300021 MEV MEV MB MB MB MB B011301300022 MB MB B011301300023 185.5 3.7 45. 7. 16. 2.B011301300024 10. 5. B011301300025 ENDDATA 6 0 B011301300026 ENDSUBENT 25 0 B011301399999 SUBENT B0113014 20190123 B029B011301400001 BIB 7 13 B011301400002 REACTION 1(83-BI-209(9-F-19,X)84-PO-210,CUM,SIG) B011301400003 2(83-BI-209(9-F-19,X)84-PO-210,CUM,SIG) B011301400004 DECAY-DATA (84-PO-210,138.4D,A,5305.,1.) B011301400005 2(85-AT-210,8.3HR,DG,245.,0.79,DG,1180.,1.) B011301400006 FACILITY (VDGT,2FR PAR). For IRRADIATIONS with energies at and B011301400007 below 109 MeV. B011301400008 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011301400009 DETECTOR (IOCH) 2-pi ionization chamber B011301400010 ERR-ANALYS The energy of the F-19 beam of the tandem accelerator B011301400011 was measured with an accuracy better than 0.1%. B011301400012 STATUS (TABLE) Table V in Phys.Rev.C.18,1298,1978 B011301400013 2(DEP,B0113014) B011301400014 (DEP,B0113012) B011301400015 ENDBIB 13 0 B011301400016 NOCOMMON 0 0 B011301400017 DATA 8 18 B011301400018 EN EN-ERR DATA 1ERR-T 1DATA-MAX 1DATA 2B011301400019 ERR-T 2DATA-MAX 2 B011301400020 MEV MEV MB MB MB MB B011301400021 MB MB B011301400022 67.5 0.3 0.06 B011301400023 0.06 B011301400024 78.7 0.3 1.65 0.4 1.65B011301400025 0.4 B011301400026 81.6 0.3 2.9 0.7 2.9B011301400027 0.7 B011301400028 83.7 0.3 3.6 0.9 3.6B011301400029 0.9 B011301400030 87. 0.3 15.7 1.6 15.7B011301400031 1.6 B011301400032 89. 0.3 14.7 1.5 14.7B011301400033 1.5 B011301400034 91.5 0.3 31.3 1.5 31.3B011301400035 1.5 B011301400036 94. 0.3 26.5 4. 26.3B011301400037 4. B011301400038 99. 0.3 32.3 3. 31.8B011301400039 3. B011301400040 104.5 0.3 70.7 4. 68.B011301400041 4. B011301400042 109. 0.3 76.6 4. 72.4B011301400043 4. B011301400044 109. 14. 79. 4. 71.5B011301400045 5. B011301400046 119. 13. 101. 5.5 89.B011301400047 7. B011301400048 132.5 13. 98. 6. 81.B011301400049 10. B011301400050 151.5 10. 110. 7. 85.B011301400051 10. B011301400052 169.5 7. 155. 8.5 123.B011301400053 9.5 B011301400054 184. 3.7 151. 8.5 120.B011301400055 9. B011301400056 185.5 3.7 128. 8. 97.B011301400057 9. B011301400058 ENDDATA 40 0 B011301400059 ENDSUBENT 58 0 B011301499999 SUBENT B0113015 20190123 B029B011301500001 BIB 7 17 B011301500002 REACTION 1(83-BI-209(10-NE-20,X)85-AT-211,,SIG) B011301500003 2(83-BI-209(10-NE-20,X)86-RN-211,,SIG) B011301500004 RAD-DET (84-PO-211-G,A) B011301500005 DECAY-DATA (86-RN-211,14.6HR,A,5850.,0.26) B011301500006 (85-AT-211,7.2HR,A,5868.,0.409) B011301500007 (84-PO-211-G,0.52SEC,A,7448.,1.) In equilibrium with B011301500008 at-211. B011301500009 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011301500010 ANALYSIS (DECAY) The decay curve of the 7.448 MeV alpha peak wasB011301500011 resolved into two components resulting from the B011301500012 exponential decay of At-211 and the accumulation of B011301500013 At-211 from Rn-211 if present. B011301500014 A direct analysis of the complex alpha peaks of Rn-211 B011301500015 and At-211 was obviously impossible As stated in B011301500016 earlier papers, see under 'comment'. B011301500017 DETECTOR (IOCH) 2-pi ionization chamber B011301500018 STATUS (TABLE) Table VI in Phys.Rev.C.18,1298,1978 B011301500019 ENDBIB 17 0 B011301500020 NOCOMMON 0 0 B011301500021 DATA 6 11 B011301500022 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2B011301500023 MEV MEV MB MB MB MB B011301500024 97. 18. 3.05 0.25 0.03 0.03B011301500025 111. 16. 24.5 3. 3.3 0.4B011301500026 141. 12. 38.4 2.3 9. 0.5B011301500027 161. 10. 33.3 2. 13.7 0.8B011301500028 172. 8. 31.2 1.6 13.3 0.7B011301500029 178. 7. 27.4 1.4 9.7 0.5B011301500030 183. 6. 27.7 1.7 13.7 0.7B011301500031 188. 6. 28. 1.5 12.1 0.6B011301500032 198. 4. 23.2 1. 11.1 0.5B011301500033 201. 4. 37.8 3. 14.5 1.B011301500034 203. 4.5 23.2 1. 11.6 0.5B011301500035 ENDDATA 13 0 B011301500036 ENDSUBENT 35 0 B011301599999 SUBENT B0113016 20190123 B029B011301600001 BIB 5 11 B011301600002 REACTION 1(83-BI-209(10-NE-20,X)85-AT-210,,SIG) B011301600003 2(83-BI-209(10-NE-20,X)85-AT-209,,SIG) B011301600004 3(83-BI-209(10-NE-20,X)85-AT-208,,SIG) B011301600005 DECAY-DATA1(85-AT-210,8.3HR,DG,245.,0.79,DG,1180.,1.) B011301600006 2(85-AT-209,5.42HR,A,5660.,0.041, B011301600007 DG,545.,0.62, B011301600008 DG,782.,0.58) B011301600009 3(85-AT-208,1.63HR,DG,660.,0.92,DG,685.,0.99) B011301600010 METHOD (EXTB,BCINT,SITA,REC) B011301600011 DETECTOR (GELI) B011301600012 STATUS (TABLE) Table VI in Phys.Rev.C.18,1298,1978 B011301600013 ENDBIB 11 0 B011301600014 NOCOMMON 0 0 B011301600015 DATA 8 1 B011301600016 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2B011301600017 DATA 3ERR-T 3 B011301600018 MEV MEV MB MB MB MB B011301600019 MB MB B011301600020 201. 4. 26. 2. 90. 3.B011301600021 38. 10. B011301600022 ENDDATA 6 0 B011301600023 ENDSUBENT 22 0 B011301699999 SUBENT B0113017 20190123 B029B011301700001 BIB 5 7 B011301700002 REACTION (83-BI-209(10-NE-20,X)84-PO-210,CUM,SIG) B011301700003 The cumulative cross sections include the formation B011301700004 of Po-210, At-210 and Bi-210. B011301700005 DECAY-DATA (84-PO-210,138.4D,A,5305.,1.) B011301700006 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011301700007 DETECTOR (IOCH) 2-pi ionization chamber B011301700008 STATUS (TABLE) Table VI in Phys.Rev.C.18,1298,1978 B011301700009 ENDBIB 7 0 B011301700010 NOCOMMON 0 0 B011301700011 DATA 4 7 B011301700012 EN EN-ERR DATA ERR-T B011301700013 MEV MEV MB MB B011301700014 97. 18. 5.1 0.6 B011301700015 111. 16. 41. 2.5 B011301700016 123. 14. 81. 6. B011301700017 141. 12. 89.6 10. B011301700018 161. 10. 98.6 6. B011301700019 177. 7. 134. 12. B011301700020 192. 5. 113. 10. B011301700021 ENDDATA 9 0 B011301700022 ENDSUBENT 21 0 B011301799999 SUBENT B0113018 20190123 B029B011301800001 BIB 8 22 B011301800002 REACTION (83-BI-209(18-AR-40,X)85-AT-211,,SIG) B011301800003 RAD-DET (84-PO-211-G,A) B011301800004 DECAY-DATA (86-RN-211,14.6HR,A,5850.,0.26) B011301800005 (85-AT-211,7.2HR,A,5868.,0.409) B011301800006 (84-PO-211-G,0.52SEC,A,7448.,1.) In equilibrium with B011301800007 At-211. B011301800008 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011301800009 ANALYSIS (DECAY) The decay curve of the 7.448 MeV alpha peak wasB011301800010 resolved into two components resulting from the B011301800011 exponential decay of At-211 and the accumulation of B011301800012 At-211 from Rn-211 if present. B011301800013 a direct analysis of the complex alpha peaks of Rn-211 B011301800014 and At-211 was obviously impossible As stated in B011301800015 earlier papers, see under 'comment'. B011301800016 DETECTOR (IOCH) 2-pi ionization chamber B011301800017 FLAG (1.) These data supersede earlier values (see SUBENTRY B011301800018 B0034002). Corrections applied to the energies were B011301800019 due to a systematic error in calculating the energy B011301800020 from the respective cyclotron parameters, corrections B011301800021 to the cross sections were due to a better calculation B011301800022 of SELFABSORPTION in the catcher foils. B011301800023 STATUS (TABLE) Table VII in Phys.Rev.C.18,1298,1978 B011301800024 ENDBIB 22 0 B011301800025 NOCOMMON 0 0 B011301800026 DATA 5 29 B011301800027 EN EN-ERR DATA ERR-T FLAG B011301800028 MEV MEV MB MB NO-DIM B011301800029 181. 7. 0.13 0.03 B011301800030 182. 9. 0.013 0.005 B011301800031 186. 8. 0.54 0.07 B011301800032 190. 6. 1.23 0.15 B011301800033 191. 7. 1.77 0.6 1. B011301800034 191. 19. 0.58 0.09 B011301800035 192. 7. 0.48 0.09 B011301800036 193. 5. 7. 0.7 B011301800037 201. 4. 15.4 1. B011301800038 202. 4. 15.6 1. B011301800039 203. 6. 13.6 1. B011301800040 206. 9. 14.7 2.5 1. B011301800041 207. 5. 13.9 1.3 B011301800042 209. 17. 11.7 1.5 B011301800043 215. 4. 17.5 1.5 B011301800044 217. 16. 20. 2.7 B011301800045 221. 7. 21. 2.2 1. B011301800046 223. 15. 16.6 2.1 B011301800047 226. 11. 20.7 3.9 1. B011301800048 233. 5. 22.5 2.2 1. B011301800049 236. 13. 21.8 3. B011301800050 241. 9. 23. 2.5 1. B011301800051 249. 12. 27.5 3.6 B011301800052 260. 7. 24. 2. 1. B011301800053 265. 10. 25.4 3. B011301800054 272. 9. 23.4 4.3 B011301800055 280. 8. 23.5 3. B011301800056 286. 7. 21.9 3. B011301800057 294. 6. 20.6 2.7 B011301800058 ENDDATA 31 0 B011301800059 ENDSUBENT 58 0 B011301899999 SUBENT B0113019 20190123 B029B011301900001 BIB 6 10 B011301900002 REACTION (83-BI-209(18-AR-40,X)85-AT-210,(CUM),SIG) B011301900003 COMMENT - by authors - alpha- and beta-decaying precursors may B011301900004 contribute, the cross sections are, however, probably B011301900005 small. B011301900006 - by compiler - Rn-210 may contribute, its electron B011301900007 capture branch is 4%. B011301900008 DECAY-DATA (85-AT-210,8.3HR,DG,245.,0.79,DG,1180.,1.) B011301900009 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011301900010 DETECTOR (GELI) B011301900011 STATUS (TABLE) Table VII in Phys.Rev.C.18,1298,1978 B011301900012 ENDBIB 10 0 B011301900013 NOCOMMON 0 0 B011301900014 DATA 4 12 B011301900015 EN EN-ERR DATA ERR-T B011301900016 MEV MEV MB MB B011301900017 191. 19. 1.7 0.4 B011301900018 201. 4. 5.7 1.1 B011301900019 209. 17. 8.7 1.7 B011301900020 217. 16. 13.3 4. B011301900021 223. 15. 11. 2.2 B011301900022 236. 13. 18. 5. B011301900023 249. 12. 25.3 5. B011301900024 265. 10. 20.3 4. B011301900025 272. 9. 26.5 6. B011301900026 280. 8. 23.4 4.7 B011301900027 286. 7. 23.3 4.8 B011301900028 294. 6. 20.8 4. B011301900029 ENDDATA 14 0 B011301900030 ENDSUBENT 29 0 B011301999999 SUBENT B0113020 20190123 B029B011302000001 BIB 5 7 B011302000002 REACTION (83-BI-209(18-AR-40,X)85-AT-209,,SIG) B011302000003 DECAY-DATA (85-AT-209,5.42HR,A,5660.,0.041, B011302000004 DG,545.,0.62, B011302000005 DG,782.,0.58) B011302000006 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011302000007 DETECTOR (GELI) B011302000008 STATUS (TABLE) Table VII in Phys.Rev.C.18,1298,1978 B011302000009 ENDBIB 7 0 B011302000010 NOCOMMON 0 0 B011302000011 DATA 5 11 B011302000012 EN EN-ERR DATA DATA-MAX ERR-T B011302000013 MEV MEV MB MB MB B011302000014 191. 19. 0.2 B011302000015 209. 17. 4.2 0.8 B011302000016 217. 16. 12.4 2.5 B011302000017 223. 15. 6.7 1.3 B011302000018 236. 13. 15.5 3.3 B011302000019 249. 12. 23.8 4.7 B011302000020 265. 10. 23. 4.6 B011302000021 272. 9. 29.7 3.6 B011302000022 280. 8. 27. 5.4 B011302000023 286. 7. 30.5 3.2 B011302000024 294. 6. 26.5 5. B011302000025 ENDDATA 13 0 B011302000026 ENDSUBENT 25 0 B011302099999 SUBENT B0113021 20190123 B029B011302100001 BIB 5 5 B011302100002 REACTION (83-BI-209(18-AR-40,X)85-AT-208,,SIG) B011302100003 DECAY-DATA (85-AT-208,1.63HR,DG,660.,0.92,DG,685.,0.99) B011302100004 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011302100005 DETECTOR (GELI) B011302100006 STATUS (TABLE) Table VII in Phys.Rev.C.18,1298,1978 B011302100007 ENDBIB 5 0 B011302100008 NOCOMMON 0 0 B011302100009 DATA 5 8 B011302100010 EN EN-ERR DATA DATA-MAX ERR-T B011302100011 MEV MEV MB MB MB B011302100012 223. 15. 1.55 0.33 B011302100013 236. 13. 5. B011302100014 249. 12. 6.6 1.3 B011302100015 265. 10. 7.1 1.4 B011302100016 272. 9. 16. 2. B011302100017 280. 8. 8. 1.6 B011302100018 286. 7. 10.5 1.5 B011302100019 294. 6. 9.8 1.9 B011302100020 ENDDATA 10 0 B011302100021 ENDSUBENT 20 0 B011302199999 SUBENT B0113022 20190123 B029B011302200001 BIB 5 5 B011302200002 REACTION (83-BI-209(18-AR-40,X)85-AT-207,,SIG) B011302200003 DECAY-DATA (85-AT-207,1.8HR,DG,814.,1.) B011302200004 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011302200005 DETECTOR (GELI) B011302200006 STATUS (TABLE) Table VII in Phys.Rev.C.18,1298,1978 B011302200007 ENDBIB 5 0 B011302200008 NOCOMMON 0 0 B011302200009 DATA 5 7 B011302200010 EN EN-ERR DATA DATA-MAX ERR-T B011302200011 MEV MEV MB MB MB B011302200012 209. 17. 0.8 B011302200013 223. 15. 0.6 B011302200014 249. 12. 2.55 0.7 B011302200015 265. 10. 2. 0.6 B011302200016 280. 8. 3.6 1. B011302200017 286. 7. 6.4 1.3 B011302200018 294. 6. 1.9 0.6 B011302200019 ENDDATA 9 0 B011302200020 ENDSUBENT 19 0 B011302299999 SUBENT B0113023 20190123 B029B011302300001 BIB 7 16 B011302300002 REACTION (83-BI-209(18-AR-40,X)86-RN-211,,SIG) B011302300003 RAD-DET (84-PO-211-G,A) B011302300004 DECAY-DATA (86-RN-211,14.6HR,A,5850.,0.26) B011302300005 (85-AT-211,7.2HR,A,5868.,0.409) B011302300006 (84-PO-211-G,0.52SEC,A,7448.,1.) In equilibrium with B011302300007 At-211. B011302300008 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011302300009 ANALYSIS (DECAY) The decay curve of the 7.448 MeV alpha peak wasB011302300010 resolved into two components resulting from the B011302300011 exponential decay of At-211 and the accumulation of B011302300012 At-211 from Rn-211 if present. B011302300013 a direct analysis of the complex alpha peaks of Rn-211 B011302300014 and At-211 was obviously impossible As stated in B011302300015 earlier papers, see under 'comment'. B011302300016 DETECTOR (IOCH) 2-pi ionization chamber B011302300017 STATUS (TABLE) Table VII in Phys.Rev.C.18,1298,1978 B011302300018 ENDBIB 16 0 B011302300019 NOCOMMON 0 0 B011302300020 DATA 5 9 B011302300021 EN EN-ERR DATA DATA-MAX ERR-T B011302300022 MEV MEV MB MB MB B011302300023 191. 19. 0.04 B011302300024 202. 4. 1.03 0.17 B011302300025 217. 16. 1.2 0.25 B011302300026 221. 7. 3.5 0.6 B011302300027 236. 13. 3.9 0.6 B011302300028 241. 9. 3.9 0.9 B011302300029 260. 7. 6.2 2. B011302300030 272. 9. 5.72 0.9 B011302300031 286. 7. 8.3 1.4 B011302300032 ENDDATA 11 0 B011302300033 ENDSUBENT 32 0 B011302399999 SUBENT B0113024 20190123 B029B011302400001 BIB 5 10 B011302400002 REACTION 1(83-BI-209(18-AR-40,X)84-PO-210,(CUM),SIG) B011302400003 2(83-BI-209(18-AR-40,X)84-PO-210,CUM,SIG) B011302400004 DECAY-DATA (84-PO-210,138.4D,A,5305.,1.) B011302400005 1(83-BI-210-G,5.01D) B011302400006 (85-AT-210,8.3HR,DG,245.,0.79,DG,1180.,1.) B011302400007 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011302400008 DETECTOR (IOCH) 2-pi ionization chamber B011302400009 STATUS (TABLE) Table VII in Phys.Rev.C.18,1298,1978 B011302400010 1(DEP,B0113024) B011302400011 (DEP,B0113019) B011302400012 ENDBIB 10 0 B011302400013 NOCOMMON 0 0 B011302400014 DATA 6 9 B011302400015 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2B011302400016 MEV MEV MB MB MB MB B011302400017 181. 7. 1.8 0.13 1.8 0.13B011302400018 190. 6. 16.9 5. 17.9 4.3B011302400019 191. 19. 0.6 0.6 2.3 0.3B011302400020 201. 4. 19.1 4.5 24.8 3.2B011302400021 202. 4. 35.5 12. 41.5 8.B011302400022 217. 16. 41.6 11. 55. 7.B011302400023 236. 13. 56.6 13. 74.7 8.B011302400024 272. 9. 63.7 16. 90. 10.B011302400025 286. 7. 75.5 16. 98. 11.B011302400026 ENDDATA 11 0 B011302400027 ENDSUBENT 26 0 B011302499999 SUBENT B0113025 20190123 B029B011302500001 BIB 8 28 B011302500002 REACTION (83-BI-209(20-CA-40,X)85-AT-211,,SIG) B011302500003 RAD-DET (84-PO-211-G,A) B011302500004 DECAY-DATA (86-RN-211,14.6HR,A,5850.,0.26) B011302500005 (85-AT-211,7.2HR,A,5868.,0.409) B011302500006 (84-PO-211-G,0.52SEC,A,7448.,1.) In equilibrium with B011302500007 At-211. B011302500008 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011302500009 ANALYSIS (DECAY) The decay curve of the 7.448 MeV alpha peak wasB011302500010 resolved into two components resulting from the B011302500011 exponential decay of at-211 and the accumulation of B011302500012 At-211 from Rn-211 if present. B011302500013 A direct analysis of the complex alpha peaks of Rn-211 B011302500014 and At-211 was obviously impossible As stated in B011302500015 earlier papers, see under 'comment'. B011302500016 DETECTOR (IOCH) 2-pi ionization chamber B011302500017 FLAG (2.) The purity of the Ca-40 beam was tested in a B011302500018 subsequent experiment by irradiating a thick Al-foil. B011302500019 In case of a contamination with Ar-40 ions an activity B011302500020 of Ar-41 could Be measured. The cross section for the B011302500021 production of this NUCLIDE being very small with Ca-40 B011302500022 projectiles, and much larger with Ar-40 ions. The B011302500023 method is sensitive to a 1% Ar-40 contamination B011302500024 (3.) The incident energy of the projectiles was B011302500025 determined by the scattered proton technique, thus B011302500026 lowering the energy error to about 0.5%. B011302500027 (4.) The value of 0.0015 given in the paper is probablyB011302500028 a misprint + see flag(3.) B011302500029 STATUS (TABLE) Table VIII in Phys.Rev.C.18,1298,1978 B011302500030 ENDBIB 28 0 B011302500031 NOCOMMON 0 0 B011302500032 DATA 6 28 B011302500033 EN EN-ERR DATA DATA-MAX ERR-T FLAG B011302500034 MEV MEV MB MB MB NO-DIM B011302500035 174. 4. 0.0037 B011302500036 174. 7. 0.003 0.0015 B011302500037 180. 9. 0.009 B011302500038 186. 2. 0.097 0.015 4.B011302500039 187. 7. 0.057 0.022 2.B011302500040 189. 7. 0.044 0.023 B011302500041 192. 7. 0.28 0.12 2.B011302500042 193. 7. 0.1 0.04 2.B011302500043 195. 6. 0.37 0.04 B011302500044 195. 8. 1.45 0.24 B011302500045 196. 0.3 0.95 0.14 3.B011302500046 196. 0.3 1.06 0.1 3.B011302500047 197. 6. 0.33 0.04 2.B011302500048 198. 6. 0.17 0.05 B011302500049 199. 11. 0.5 0.14 2.B011302500050 202. 6. 1.3 0.2 B011302500051 202. 5. 0.53 0.16 B011302500052 204. 5. 1.15 0.26 2.B011302500053 204. 5. 2.2 0.4 B011302500054 205. 7. 9.02 1.8 B011302500055 211. 4. 3. 0.3 2.B011302500056 213. 4. 7.6 1.2 B011302500057 214. 4. 11.9 2.5 B011302500058 218. 13. 14.2 1.6 2.B011302500059 225. 4. 14.5 1.6 B011302500060 226. 4. 14.9 1. B011302500061 249. 5. 15.6 1.3 B011302500062 275. 5. 13.8 1.5 B011302500063 ENDDATA 30 0 B011302500064 ENDSUBENT 63 0 B011302599999 SUBENT B0113026 20190123 B029B011302600001 BIB 6 12 B011302600002 REACTION (83-BI-209(20-CA-40,X)85-AT-210,,SIG) B011302600003 DECAY-DATA (85-AT-210,8.3HR,DG,245.,0.79,DG,1180.,1.) B011302600004 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011302600005 DETECTOR (GELI) B011302600006 FLAG (1.) The purity of the Ca-40 beam was tested in a B011302600007 subsequent experiment by irradiating a thick Al-foil. B011302600008 In case of a contamination with Ar-40 ions an activity B011302600009 of Ar-41 could Be measured. The cross section for the B011302600010 production of this NUCLIDE being very small with Ca-40 B011302600011 projectiles, and much larger with Ar-40 ions. The B011302600012 method is sensitive to a 1% Ar-40 contamination. B011302600013 STATUS (TABLE) Table VIII in Phys.Rev.C.18,1298,1978 B011302600014 ENDBIB 12 0 B011302600015 NOCOMMON 0 0 B011302600016 DATA 5 7 B011302600017 EN EN-ERR DATA ERR-T FLAG B011302600018 MEV MEV MB MB NO-DIM B011302600019 199. 11. 8.4 2.5 1. B011302600020 205. 7. 24.4 5. B011302600021 218. 13. 33. 3. 1. B011302600022 225. 4. 27.5 5.5 B011302600023 226. 4. 31.3 4. B011302600024 249. 5. 30.2 3. B011302600025 275. 5. 31.5 3. B011302600026 ENDDATA 9 0 B011302600027 ENDSUBENT 26 0 B011302699999 SUBENT B0113027 20190123 B029B011302700001 BIB 6 14 B011302700002 REACTION (83-BI-209(20-CA-40,X)85-AT-209,,SIG) B011302700003 DECAY-DATA (85-AT-209,5.42HR,A,5660.,0.041, B011302700004 DG,545.,0.62, B011302700005 DG,782.,0.58) B011302700006 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011302700007 DETECTOR (GELI) B011302700008 FLAG (1.) The purity of the Ca-40 beam was tested in a B011302700009 subsequent experiment by irradiating a thick Al-foil. B011302700010 In case of a contamination with Ar-40 ions an activity B011302700011 of Ar-41 could Be measured. The cross section for the B011302700012 production of this NUCLIDE being very small with Ca-40 B011302700013 projectiles, and much larger with Ar-40 ions. The B011302700014 method is sensitive to a 1% Ar-40 contamination. B011302700015 STATUS (TABLE) Table VIII in Phys.Rev.C.18,1298,1978 B011302700016 ENDBIB 14 0 B011302700017 NOCOMMON 0 0 B011302700018 DATA 5 7 B011302700019 EN EN-ERR DATA ERR-T FLAG B011302700020 MEV MEV MB MB NO-DIM B011302700021 199. 11. 0.62 0.18 1. B011302700022 205. 7. 10.9 2.2 B011302700023 218. 13. 29. 3.5 1. B011302700024 225. 4. 35. 7. B011302700025 226. 4. 39. 6.5 B011302700026 249. 5. 44.5 7. B011302700027 275. 5. 49. 6. B011302700028 ENDDATA 9 0 B011302700029 ENDSUBENT 28 0 B011302799999 SUBENT B0113028 20190123 B029B011302800001 BIB 7 15 B011302800002 REACTION (83-BI-209(20-CA-40,23N+18P)85-AT-208,,SIG) B011302800003 COMMENT - by authors - alpha- and beta-decaying precursors may B011302800004 contribute, the cross sections are, however, probably B011302800005 small. B011302800006 DECAY-DATA (85-AT-208,1.63HR,DG,660.,0.92,DG,685.,0.99) B011302800007 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011302800008 DETECTOR (GELI) B011302800009 FLAG (1.) The purity of the Ca-40 beam was tested in a B011302800010 subsequent experiment by irradiating a thick Al-foil. B011302800011 In case of a contamination with Ar-40 ions an activity B011302800012 of Ar-41 could Be measured. The cross section for the B011302800013 production of this NUCLIDE being very small with Ca-40 B011302800014 projectiles, and much larger with Ar-40 ions. The B011302800015 method is sensitive to a 1% Ar-40 contamination. B011302800016 STATUS (TABLE) Table VIII in Phys.Rev.C.18,1298,1978 B011302800017 ENDBIB 15 0 B011302800018 NOCOMMON 0 0 B011302800019 DATA 5 5 B011302800020 EN EN-ERR DATA ERR-T FLAG B011302800021 MEV MEV MB MB NO-DIM B011302800022 199. 11. 0.95 0.3 1. B011302800023 225. 4. 14.3 2.9 B011302800024 226. 4. 17.3 3.5 B011302800025 249. 5. 21. 1. B011302800026 275. 5. 38. 7. B011302800027 ENDDATA 7 0 B011302800028 ENDSUBENT 27 0 B011302899999 SUBENT B0113029 20190123 B029B011302900001 BIB 5 5 B011302900002 REACTION (83-BI-209(20-CA-40,X)85-AT-207,,SIG) B011302900003 DECAY-DATA (85-AT-207,1.8HR,DG,814.,1.) B011302900004 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011302900005 DETECTOR (GELI) B011302900006 STATUS (TABLE) Table VIII in Phys.Rev.C.18,1298,1978 B011302900007 ENDBIB 5 0 B011302900008 NOCOMMON 0 0 B011302900009 DATA 4 4 B011302900010 EN EN-ERR DATA ERR-T B011302900011 MEV MEV MB MB B011302900012 225. 4. 7.9 1.6 B011302900013 226. 4. 8.5 1.7 B011302900014 249. 5. 10.3 2.4 B011302900015 275. 5. 10. 3. B011302900016 ENDDATA 6 0 B011302900017 ENDSUBENT 16 0 B011302999999 SUBENT B0113030 20190123 B029B011303000001 BIB 8 23 B011303000002 REACTION (83-BI-209(20-CA-40,X)86-RN-211,,SIG) B011303000003 RAD-DET (84-PO-211-G,A) B011303000004 DECAY-DATA (86-RN-211,14.6HR,A,5850.,0.26) B011303000005 (85-AT-211,7.2HR,A,5868.,0.409) B011303000006 (84-PO-211-G,0.52SEC,A,7448.,1.) In equilibrium with B011303000007 at-211. B011303000008 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011303000009 ANALYSIS (DECAY) The decay curve of the 7.448 MeV alpha peak wasB011303000010 resolved into two components resulting from the B011303000011 exponential decay of at-211 and the accumulation of B011303000012 at-211 from Rn-211 if present. B011303000013 a direct analysis of the complex alpha peaks of Rn-211 B011303000014 and at-211 was obviously impossible As stated in B011303000015 earlier papers, see under 'comment'. B011303000016 DETECTOR (IOCH) 2-pi ionization chamber B011303000017 FLAG (3.) The purity of the Ca-40 beam was tested in a B011303000018 subsequent experiment by irradiating a thick Al-foil. B011303000019 In case of a contamination with Ar-40 ions an activity B011303000020 of Ar-41 could Be measured. The cross section for the B011303000021 production of this NUCLIDE being very small with Ca-40 B011303000022 projectiles, and much larger with Ar-40 ions. The B011303000023 method is sensitive to a 1% Ar-40 contamination. B011303000024 STATUS (TABLE) Table VIII in Phys.Rev.C.18,1298,1978 B011303000025 ENDBIB 23 0 B011303000026 NOCOMMON 0 0 B011303000027 DATA 6 10 B011303000028 EN EN-ERR DATA DATA-MAX ERR-T FLAG B011303000029 MEV MEV MB MB MB NO-DIM B011303000030 196. 0.3 0.036 B011303000031 204. 5. 0.2 0.04 B011303000032 205. 7. 2.7 0.4 B011303000033 213. 4. 2.2 0.5 B011303000034 214. 4. 5.7 1.1 B011303000035 218. 13. 5.1 0.6 3.B011303000036 225. 4. 7.3 1.4 B011303000037 226. 4. 8.7 1. B011303000038 249. 5. 10. 0.9 B011303000039 275. 5. 12.1 1.3 B011303000040 ENDDATA 12 0 B011303000041 ENDSUBENT 40 0 B011303099999 SUBENT B0113031 20190123 B029B011303100001 BIB 6 19 B011303100002 REACTION (83-BI-209(20-CA-40,X)84-PO-210,(CUM),SIG) B011303100003 DECAY-DATA (84-PO-210,138.4D,A,5305.,1.) B011303100004 (83-BI-210-G,5.01D) B011303100005 (85-AT-210,8.3HR,DG,245.,0.79,DG,1180.,1.) B011303100006 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011303100007 DETECTOR (IOCH) 2-pi ionization chamber B011303100008 FLAG (2.) The purity of the Ca-40 beam was tested in a B011303100009 subsequent experiment by irradiating a thick Al-foil. B011303100010 In case of a contamination with Ar-40 ions an activity B011303100011 of Ar-41 could Be measured. The cross section for the B011303100012 production of this NUCLIDE being very small with Ca-40 B011303100013 projectiles, and much larger with Ar-40 ions. The B011303100014 method is sensitive to a 1% Ar-40 contamination. B011303100015 (4.) The incident energy of the projectiles was B011303100016 determined by the scattered proton technique, thus B011303100017 lowering the energy error to about 0.5%. B011303100018 STATUS (TABLE) Table VIII in Phys.Rev.C.18,1298,1978 B011303100019 (DEP,B0113031) B011303100020 (DEP,B0113026) B011303100021 ENDBIB 19 0 B011303100022 NOCOMMON 0 0 B011303100023 DATA 7 12 B011303100024 EN EN-ERR DATA DATA-MAX DATA-APRX ERR-T B011303100025 FLAG B011303100026 MEV MEV MB MB MB MB B011303100027 NO-DIM B011303100028 180. 9. 1. B011303100029 2. B011303100030 187. 7. 2.14 0.2B011303100031 2. B011303100032 195. 8. 10. 2.B011303100033 B011303100034 196. 0.3 10. 2.B011303100035 4. B011303100036 196. 0.3 8. 2.B011303100037 4. B011303100038 205. 7. 21. 5.B011303100039 B011303100040 214. 4. 23. 5.B011303100041 B011303100042 218. 13. 36. 10.B011303100043 2. B011303100044 225. 4. 42. 12.B011303100045 B011303100046 226. 4. 48. 12.B011303100047 B011303100048 249. 5. 53. 11.B011303100049 B011303100050 275. 5. 61. 13.B011303100051 B011303100052 ENDDATA 28 0 B011303100053 ENDSUBENT 52 0 B011303199999 SUBENT B0113032 20190123 B029B011303200001 BIB 7 17 B011303200002 REACTION 1(83-BI-209(26-FE-56,X)85-AT-211,,SIG) B011303200003 2(83-BI-209(26-FE-56,X)86-RN-211,,SIG) B011303200004 RAD-DET (84-PO-211-G,A) B011303200005 DECAY-DATA (86-RN-211,14.6HR,A,5850.,0.26) B011303200006 (85-AT-211,7.2HR,A,5868.,0.409) B011303200007 (84-PO-211-G,0.52SEC,A,7448.,1.) In equilibrium with B011303200008 at-211. B011303200009 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011303200010 ANALYSIS (DECAY) The decay curve of the 7.448 MeV alpha peak wasB011303200011 resolved into two components resulting from the B011303200012 exponential decay of at-211 and the accumulation of B011303200013 At-211 from Rn-211 if present. B011303200014 A direct analysis of the complex alpha peaks of Rn-211 B011303200015 and at-211 was obviously impossible As stated in B011303200016 earlier papers, see under 'comment'. B011303200017 DETECTOR (IOCH) 2-pi ionization chamber B011303200018 STATUS (TABLE) Table IX in Phys.Rev.C.18,1298,1978 B011303200019 ENDBIB 17 0 B011303200020 NOCOMMON 0 0 B011303200021 DATA 6 17 B011303200022 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2B011303200023 MEV MEV MB MB MB MB B011303200024 263. 11. 0.013 0.006 B011303200025 266. 4. 0.055 0.03 B011303200026 266. 10. 0.094 0.03 B011303200027 273. 10. 0.4 0.1 B011303200028 276. 2. 1. 0.07 B011303200029 280. 8. 1.2 0.3 B011303200030 282. 9. 3.1 0.8 B011303200031 284. 1. 4. 0.3 B011303200032 286. 8. 5.9 0.9 B011303200033 291. 7. 7.4 1. 1.5 0.2B011303200034 298. 6. 10.5 1.9 B011303200035 304. 6. 7.1 1. 4.4 0.6B011303200036 308. 10. 9.3 1.2 4.9 0.6B011303200037 317. 9. 9. 1.2 4.9 0.6B011303200038 328. 7. 9.3 1.2 5.7 0.7B011303200039 371. 12. 10.5 1.9 7.9 1.5B011303200040 396. 8. 12. 2. B011303200041 ENDDATA 19 0 B011303200042 ENDSUBENT 41 0 B011303299999 SUBENT B0113033 20190123 B029B011303300001 BIB 5 5 B011303300002 REACTION (83-BI-209(26-FE-56,X)85-AT-210,,SIG) B011303300003 DECAY-DATA (85-AT-210,8.3HR,DG,245.,0.79,DG,1180.,1.) B011303300004 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011303300005 DETECTOR (GELI) B011303300006 STATUS (TABLE) Table IX in Phys.Rev.C.18,1298,1978 B011303300007 ENDBIB 5 0 B011303300008 NOCOMMON 0 0 B011303300009 DATA 4 9 B011303300010 EN EN-ERR DATA ERR-T B011303300011 MEV MEV MB MB B011303300012 280. 8. 1.2 0.3 B011303300013 286. 8. 1.07 0.3 B011303300014 291. 7. 9.6 1.2 B011303300015 298. 6. 14.3 3. B011303300016 304. 6. 7. 2. B011303300017 308. 10. 16.5 3. B011303300018 317. 9. 15.8 3. B011303300019 328. 7. 17. 2. B011303300020 371. 12. 19.6 5. B011303300021 ENDDATA 11 0 B011303300022 ENDSUBENT 21 0 B011303399999 SUBENT B0113034 20190123 B029B011303400001 BIB 5 7 B011303400002 REACTION (83-BI-209(26-FE-56,X)85-AT-209,,SIG) B011303400003 DECAY-DATA (85-AT-209,5.42HR,A,5660.,0.041, B011303400004 DG,545.,0.62, B011303400005 DG,782.,0.58) B011303400006 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011303400007 DETECTOR (GELI) B011303400008 STATUS (TABLE) Table IX in Phys.Rev.C.18,1298,1978 B011303400009 ENDBIB 7 0 B011303400010 NOCOMMON 0 0 B011303400011 DATA 4 8 B011303400012 EN EN-ERR DATA ERR-T B011303400013 MEV MEV MB MB B011303400014 286. 8. 2.1 1. B011303400015 291. 7. 12. 3. B011303400016 298. 6. 17.5 3.9 B011303400017 304. 6. 13. 3.7 B011303400018 308. 10. 27.6 3. B011303400019 317. 9. 25.5 3.2 B011303400020 328. 7. 31. 4. B011303400021 371. 12. 25.4 7.8 B011303400022 ENDDATA 10 0 B011303400023 ENDSUBENT 22 0 B011303499999 SUBENT B0113035 20190123 B029B011303500001 BIB 5 5 B011303500002 REACTION (83-BI-209(26-FE-56,X)85-AT-208,,SIG) B011303500003 DECAY-DATA (85-AT-208,1.63HR,DG,660.,0.92,DG,685.,0.99) B011303500004 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011303500005 DETECTOR (GELI) B011303500006 STATUS (TABLE) Table IX in Phys.Rev.C.18,1298,1978 B011303500007 ENDBIB 5 0 B011303500008 NOCOMMON 0 0 B011303500009 DATA 4 5 B011303500010 EN EN-ERR DATA ERR-T B011303500011 MEV MEV MB MB B011303500012 298. 6. 13.8 3.5 B011303500013 304. 6. 4.6 2. B011303500014 317. 9. 18.7 3. B011303500015 328. 7. 16. 2.6 B011303500016 371. 12. 5.3 1.4 B011303500017 ENDDATA 7 0 B011303500018 ENDSUBENT 17 0 B011303599999 SUBENT B0113036 20190123 B029B011303600001 BIB 5 10 B011303600002 REACTION 1(83-BI-209(26-FE-56,X)84-PO-210,(CUM),SIG) B011303600003 2(83-BI-209(26-FE-56,X)84-PO-210,CUM,SIG) B011303600004 DECAY-DATA (84-PO-210,138.4D,A,5305.,1.) B011303600005 1(83-BI-210-G,5.01D) B011303600006 (85-AT-210,8.3HR,DG,245.,0.79,DG,1180.,1.) B011303600007 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011303600008 DETECTOR (IOCH) 2-pi ionization chamber B011303600009 STATUS (TABLE) Table IX in Phys.Rev.C.18,1298,1978 B011303600010 1(DEP,B0113036) B011303600011 (DEP,B0113033) B011303600012 ENDBIB 10 0 B011303600013 NOCOMMON 0 0 B011303600014 DATA 6 11 B011303600015 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2B011303600016 MEV MEV MB MB MB MB B011303600017 266. 4. 0.95 0.5 0.95 0.5B011303600018 276. 2. 2.5 1.2 2.5 1.2B011303600019 282. 9. 4.8 3. 5.8 3.B011303600020 284. 1. 12.4 6. 13.4 5.B011303600021 291. 7. 18. 9. 27.5 8.B011303600022 304. 6. 30. 15. 37. 13.B011303600023 308. 10. 45. 13. 62. 10.B011303600024 317. 9. 45. 13. 60. 10.B011303600025 328. 7. 43. 12. 60. 10.B011303600026 371. 12. 66. 20. 86. 15.B011303600027 396. 8. 70. 20. 90. 15.B011303600028 ENDDATA 13 0 B011303600029 ENDSUBENT 28 0 B011303699999 SUBENT B0113037 20190123 B029B011303700001 BIB 8 19 B011303700002 REACTION (83-BI-209(29-CU-63,X)85-AT-211,,SIG) B011303700003 RAD-DET (84-PO-211-G,A) B011303700004 DECAY-DATA (86-RN-211,14.6HR,A,5850.,0.26) B011303700005 (85-AT-211,7.2HR,A,5868.,0.409) B011303700006 (84-PO-211-G,0.52SEC,A,7448.,1.) In equilibrium with B011303700007 at-211. B011303700008 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011303700009 ANALYSIS (DECAY) The decay curve of the 7.448 MeV alpha peak wasB011303700010 resolved into two components resulting from the B011303700011 exponential decay of at-211 and the accumulation of B011303700012 at-211 from Rn-211 if present. B011303700013 a direct analysis of the complex alpha peaks of Rn-211 B011303700014 and at-211 was obviously impossible As stated in B011303700015 earlier papers, see under 'comment'. B011303700016 DETECTOR (IOCH) 2-pi ionization chamber B011303700017 FLAG (1.) The incident energy of the projectiles was B011303700018 determined by the scattered proton technique, thus B011303700019 lowering the energy error to about 0.5%. B011303700020 STATUS (TABLE) Table X in Phys.Rev.C.18,1298,1978 B011303700021 ENDBIB 19 0 B011303700022 NOCOMMON 0 0 B011303700023 DATA 5 16 B011303700024 EN EN-ERR DATA ERR-T FLAG B011303700025 MEV MEV MB MB NO-DIM B011303700026 295. 3. 0.03 0.01 1. B011303700027 301. 13. 0.017 0.008 B011303700028 305. 11. 0.24 0.12 B011303700029 309. 2. 1.28 0.26 1. B011303700030 309. 12. 0.12 0.04 B011303700031 317. 10. 3.9 0.7 B011303700032 321. 10. 2.84 0.35 B011303700033 321. 16. 1.53 0.16 B011303700034 324. 9. 9.3 2.7 B011303700035 328. 9. 5.9 1. B011303700036 336. 8. 7.9 0.8 B011303700037 338. 7. 9.4 1.7 B011303700038 345. 7. 10.3 1. B011303700039 355. 11. 9.7 0.7 B011303700040 377. 8. 10.4 0.75 B011303700041 410. 9. 8.7 0.9 B011303700042 ENDDATA 18 0 B011303700043 ENDSUBENT 42 0 B011303799999 SUBENT B0113038 20190123 B029B011303800001 BIB 5 5 B011303800002 REACTION (83-BI-209(29-CU-63,X)85-AT-210,,SIG) B011303800003 DECAY-DATA (85-AT-210,8.3HR,DG,245.,0.79,DG,1180.,1.) B011303800004 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011303800005 DETECTOR (GELI) B011303800006 STATUS (TABLE) Table X in Phys.Rev.C.18,1298,1978 B011303800007 ENDBIB 5 0 B011303800008 NOCOMMON 0 0 B011303800009 DATA 4 6 B011303800010 EN EN-ERR DATA ERR-T B011303800011 MEV MEV MB MB B011303800012 328. 9. 9.6 1.5 B011303800013 336. 8. 9.1 1.7 B011303800014 345. 7. 13.6 1.9 B011303800015 355. 11. 17. 2.5 B011303800016 377. 8. 17.9 2.3 B011303800017 410. 9. 20. 3.3 B011303800018 ENDDATA 8 0 B011303800019 ENDSUBENT 18 0 B011303899999 SUBENT B0113039 20190123 B029B011303900001 BIB 5 7 B011303900002 REACTION (83-BI-209(29-CU-63,X)85-AT-209,,SIG) B011303900003 DECAY-DATA (85-AT-209,5.42HR,A,5660.,0.041, B011303900004 DG,545.,0.62, B011303900005 DG,782.,0.58) B011303900006 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011303900007 DETECTOR (GELI) B011303900008 STATUS (TABLE) Table X in Phys.Rev.C.18,1298,1978 B011303900009 ENDBIB 7 0 B011303900010 NOCOMMON 0 0 B011303900011 DATA 4 6 B011303900012 EN EN-ERR DATA ERR-T B011303900013 MEV MEV MB MB B011303900014 328. 9. 5.8 1.8 B011303900015 336. 8. 10.8 1.4 B011303900016 345. 7. 22.2 4.5 B011303900017 355. 11. 22.7 3.6 B011303900018 377. 8. 31.6 6. B011303900019 410. 9. 29.6 3.8 B011303900020 ENDDATA 8 0 B011303900021 ENDSUBENT 20 0 B011303999999 SUBENT B0113040 20190123 B029B011304000001 BIB 5 5 B011304000002 REACTION (83-BI-209(29-CU-63,X)85-AT-208,,SIG) B011304000003 DECAY-DATA (85-AT-208,1.63HR,DG,660.,0.92,DG,685.,0.99) B011304000004 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011304000005 DETECTOR (GELI) B011304000006 STATUS (TABLE) Table X in Phys.Rev.C.18,1298,1978 B011304000007 ENDBIB 5 0 B011304000008 NOCOMMON 0 0 B011304000009 DATA 4 6 B011304000010 EN EN-ERR DATA ERR-T B011304000011 MEV MEV MB MB B011304000012 328. 9. 1.8 0.5 B011304000013 336. 8. 4.1 1. B011304000014 345. 7. 10.8 1.4 B011304000015 355. 11. 16.8 4.4 B011304000016 377. 8. 23.4 7. B011304000017 410. 9. 11.9 2. B011304000018 ENDDATA 8 0 B011304000019 ENDSUBENT 18 0 B011304099999 SUBENT B0113041 20190123 B029B011304100001 BIB 7 16 B011304100002 REACTION (83-BI-209(29-CU-63,X)86-RN-211,,SIG) B011304100003 RAD-DET (84-PO-211-G,A) B011304100004 DECAY-DATA (86-RN-211,14.6HR,A,5850.,0.26) B011304100005 (85-AT-211,7.2HR,A,5868.,0.409) B011304100006 (84-PO-211-G,0.52SEC,A,7448.,1.) In equilibrium with B011304100007 at-211. B011304100008 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011304100009 ANALYSIS (DECAY) The decay curve of the 7.448 MeV alpha peak wasB011304100010 resolved into two components resulting from the B011304100011 exponential decay of at-211 and the accumulation of B011304100012 at-211 from Rn-211 if present. B011304100013 a direct analysis of the complex alpha peaks of Rn-211 B011304100014 and at-211 was obviously impossible As stated in B011304100015 earlier papers, see under 'comment'. B011304100016 DETECTOR (IOCH) 2-pi ionization chamber B011304100017 STATUS (TABLE) Table X in Phys.Rev.C.18,1298,1978 B011304100018 ENDBIB 16 0 B011304100019 NOCOMMON 0 0 B011304100020 DATA 4 6 B011304100021 EN EN-ERR DATA ERR-T B011304100022 MEV MEV MB MB B011304100023 317. 10. 0.68 0.12 B011304100024 321. 16. 0.4 0.04 B011304100025 338. 7. 4.4 0.8 B011304100026 355. 11. 6.5 1.3 B011304100027 377. 8. 5.9 0.4 B011304100028 410. 9. 7.3 0.8 B011304100029 ENDDATA 8 0 B011304100030 ENDSUBENT 29 0 B011304199999 SUBENT B0113042 20190123 B029B011304200001 BIB 6 13 B011304200002 REACTION 1(83-BI-209(29-CU-63,X)84-PO-210,(CUM),SIG) B011304200003 2(83-BI-209(29-CU-63,X)84-PO-210,CUM,SIG) B011304200004 DECAY-DATA (84-PO-210,138.4D,A,5305.,1.) B011304200005 1(83-BI-210-G,5.01D) B011304200006 (85-AT-210,8.3HR,DG,245.,0.79,DG,1180.,1.) B011304200007 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011304200008 DETECTOR (IOCH) 2-pi ionization chamber B011304200009 FLAG (1.) The incident energy of the projectiles was B011304200010 determined by the scattered proton technique, thus B011304200011 lowering the energy error to about 0.5%. B011304200012 STATUS (TABLE) Table X in Phys.Rev.C.18,1298,1978 B011304200013 1(DEP,B0113042) B011304200014 (DEP,B0113038) B011304200015 ENDBIB 13 0 B011304200016 NOCOMMON 0 0 B011304200017 DATA 7 10 B011304200018 EN EN-ERR FLAG DATA 1ERR-T 1DATA 2B011304200019 ERR-T 2 B011304200020 MEV MEV NO-DIM MB MB MB B011304200021 MB B011304200022 289. 4. 1. 0.35 0.07 0.35B011304200023 0.07 B011304200024 295. 3. 1. 1.95 0.4 1.95B011304200025 0.4 B011304200026 301. 13. 5.8 1.2 5.8B011304200027 1.2 B011304200028 309. 2. 1. 9.6 2. 9.6B011304200029 2. B011304200030 309. 12. 7.4 1.5 7.4B011304200031 1.5 B011304200032 321. 10. 22.6 3.6 22.6B011304200033 3.6 B011304200034 321. 16. 19.4 3.2 19.4B011304200035 3.2 B011304200036 355. 11. 35. 12. 52.B011304200037 10. B011304200038 377. 8. 54. 16. 72.B011304200039 14. B011304200040 410. 9. 53. 15. 73.B011304200041 14. B011304200042 ENDDATA 24 0 B011304200043 ENDSUBENT 42 0 B011304299999 SUBENT B0113043 20190123 B029B011304300001 BIB 9 21 B011304300002 REACTION 1(81-TL-205(9-F-19,X)85-AT-211,,SIG) B011304300003 2(81-TL-205(9-F-19,X)86-RN-211,,SIG) B011304300004 COMMENT 2- by authors - alpha- and beta-decaying precursors may B011304300005 contribute, the cross sections are, however, probably B011304300006 small. B011304300007 RAD-DET (84-PO-211-G,A) B011304300008 DECAY-DATA (86-RN-211,14.6HR,A,5850.,0.26) B011304300009 (85-AT-211,7.2HR,A,5868.,0.409) B011304300010 (84-PO-211-G,0.52SEC,A,7448.,1.) In equilibrium with B011304300011 at-211. B011304300012 METHOD (EXTB,BCINT,SITA,REC) B011304300013 ANALYSIS (DECAY) The decay curve of the 7.448 MeV alpha peak wasB011304300014 resolved into two components resulting from the B011304300015 exponential decay of at-211 and the accumulation of B011304300016 at-211 from Rn-211 if present. B011304300017 a direct analysis of the complex alpha peaks of Rn-211 B011304300018 and at-211 was obviously impossible As stated in B011304300019 earlier papers, see under 'comment'. B011304300020 DETECTOR (IOCH) 2-pi ionization chamber B011304300021 STATUS (TABLE) Table XI in Phys.Rev.C.18,1298,1978 B011304300022 HISTORY (20190123A) Corrected SF3: use X for 043.1. B011304300023 ENDBIB 21 0 B011304300024 NOCOMMON 0 0 B011304300025 DATA 6 1 B011304300026 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2B011304300027 MEV MEV MB MB MB MB B011304300028 178. 6. 0.092 0.007 1.47 0.11B011304300029 ENDDATA 3 0 B011304300030 ENDSUBENT 29 0 B011304399999 SUBENT B0113044 20190123 B029B011304400001 BIB 5 7 B011304400002 REACTION (81-TL-205(9-F-19,X)84-PO-210,CUM,SIG) B011304400003 the cumulative cross section includes the formation B011304400004 of Po-210, at-210, and Bi-210. B011304400005 DECAY-DATA (84-PO-210,138.4D,A,5305.,1.) B011304400006 METHOD (EXTB,BCINT,SITA,REC) B011304400007 DETECTOR (IOCH) 2-pi ionization chamber B011304400008 STATUS (TABLE) Table XI in Phys.Rev.C.18,1298,1978 B011304400009 ENDBIB 7 0 B011304400010 NOCOMMON 0 0 B011304400011 DATA 4 1 B011304400012 EN EN-ERR DATA ERR-T B011304400013 MEV MEV MB MB B011304400014 178. 6. 27.5 5.4 B011304400015 ENDDATA 3 0 B011304400016 ENDSUBENT 15 0 B011304499999 SUBENT B0113045 20190123 B029B011304500001 BIB 7 17 B011304500002 REACTION 1(81-TL-205(10-NE-20,X)85-AT-211,,SIG) B011304500003 2(81-TL-205(10-NE-20,X)86-RN-211,,SIG) B011304500004 RAD-DET (84-PO-211-G,A) B011304500005 DECAY-DATA (86-RN-211,14.6HR,A,5850.,0.26) B011304500006 (85-AT-211,7.2HR,A,5868.,0.409) B011304500007 (84-PO-211-G,0.52SEC,A,7448.,1.) In equilibrium with B011304500008 at-211. B011304500009 METHOD (EXTB,BCINT,SITA,REC) B011304500010 ANALYSIS (DECAY) The decay curve of the 7.448 MeV alpha peak wasB011304500011 resolved into two components resulting from the B011304500012 exponential decay of at-211 and the accumulation of B011304500013 at-211 from Rn-211 if present. B011304500014 a direct analysis of the complex alpha peaks of Rn-211 B011304500015 and at-211 was obviously impossible As stated in B011304500016 earlier papers, see under 'comment'. B011304500017 DETECTOR (IOCH) 2-pi ionization chamber B011304500018 STATUS (TABLE) Table XI in Phys.Rev.C.18,1298,1978 B011304500019 ENDBIB 17 0 B011304500020 NOCOMMON 0 0 B011304500021 DATA 6 1 B011304500022 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2B011304500023 MEV MEV MB MB MB MB B011304500024 193.5 5. 0.15 0.04 0.65 0.15B011304500025 ENDDATA 3 0 B011304500026 ENDSUBENT 25 0 B011304599999 SUBENT B0113046 20190123 B029B011304600001 BIB 7 17 B011304600002 REACTION 1(81-TL-205(18-AR-40,X)85-AT-211,,SIG) B011304600003 2(81-TL-205(18-AR-40,X)86-RN-211,,SIG) B011304600004 RAD-DET (84-PO-211-G,A) B011304600005 DECAY-DATA (86-RN-211,14.6HR,A,5850.,0.26) B011304600006 (85-AT-211,7.2HR,A,5868.,0.409) B011304600007 (84-PO-211-G,0.52SEC,A,7448.,1.) In equilibrium with B011304600008 at-211. B011304600009 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011304600010 ANALYSIS (DECAY) The decay curve of the 7.448 MeV alpha peak wasB011304600011 resolved into two components resulting from the B011304600012 exponential decay of at-211 and the accumulation of B011304600013 at-211 from Rn-211 if present. B011304600014 a direct analysis of the complex alpha peaks of Rn-211 B011304600015 and at-211 was obviously impossible As stated in B011304600016 earlier papers, see under 'comment'. B011304600017 DETECTOR (IOCH) 2-pi ionization chamber B011304600018 STATUS (TABLE) Table XI in Phys.Rev.C.18,1298,1978 B011304600019 ENDBIB 17 0 B011304600020 NOCOMMON 0 0 B011304600021 DATA 6 5 B011304600022 EN EN-ERR DATA 1ERR-T 1DATA 2ERR-T 2B011304600023 MEV MEV MB MB MB MB B011304600024 197. 15. 0.8 0.07 B011304600025 218. 15. 1.06 0.11 B011304600026 239. 13. 1.46 0.24 0.6 0.14B011304600027 262. 7. 1.48 0.14 1. 0.1B011304600028 284. 7. 0.95 0.18 1.48 0.37B011304600029 ENDDATA 7 0 B011304600030 ENDSUBENT 29 0 B011304699999 SUBENT B0113047 20190123 B029B011304700001 BIB 6 15 B011304700002 REACTION (83-BI-209(20-CA-40,X)84-PO-210,CUM,SIG) B011304700003 DECAY-DATA (84-PO-210,138.4D,A,5305.,1.) B011304700004 METHOD (EXTB,BCINT,STTA,SITA,EDEG,REC) B011304700005 DETECTOR (IOCH) 2-pi ionization chamber B011304700006 FLAG (2.) The purity of the Ca-40 beam was tested in a B011304700007 subsequent experiment by irradiating a thick Al-foil. B011304700008 In case of a contamination with Ar-40 ions an activity B011304700009 of Ar-41 could Be measured. The cross section for the B011304700010 production of this NUCLIDE being very small with Ca-40 B011304700011 projectiles, and much larger with Ar-40 ions. The B011304700012 method is sensitive to a 1% Ar-40 contamination. B011304700013 (4.) The incident energy of the projectiles was B011304700014 determined by the scattered proton technique, thus B011304700015 lowering the energy error to about 0.5%. B011304700016 STATUS (TABLE) Table XIII in Phys.Rev.C.18,1298,1978 B011304700017 ENDBIB 15 0 B011304700018 NOCOMMON 0 0 B011304700019 DATA 7 12 B011304700020 EN EN-ERR DATA DATA-MAX DATA-APRX ERR-T B011304700021 FLAG B011304700022 MEV MEV MB MB MB MB B011304700023 NO-DIM B011304700024 180. 9. 1. B011304700025 2. B011304700026 187. 7. 2.14 0.2B011304700027 2. B011304700028 195. 8. 10.8 02.B011304700029 B011304700030 196. 0.3 10.5 02.B011304700031 4. B011304700032 196. 0.3 9.5 1.B011304700033 4. B011304700034 205. 7. 45.6 5.B011304700035 B011304700036 214. 4. 51. 5.B011304700037 B011304700038 218. 13. 69. 7.B011304700039 2. B011304700040 225. 4. 69. 7.B011304700041 B011304700042 226. 4. 79. 8.B011304700043 B011304700044 249. 5. 83. 8.B011304700045 B011304700046 275. 5. 92. 010.B011304700047 B011304700048 ENDDATA 28 0 B011304700049 ENDSUBENT 48 0 B011304799999 ENDENTRY 47 0 B011399999999