ENTRY B0110 20011220 0000B011000000001 SUBENT B0110001 20011220 0000B011000100001 BIB 8 27 B011000100002 TITLE Decay of the Compound Nucleus Po-204. Excitation B011000100003 Function Measurements For the Reactions B011000100004 Dy-164(AR-40,XN)Po-204-X and W-184(NE-20,XN)Po-204-X B011000100005 AUTHOR (B.LAGARDE, Y.LE BEYEC) B011000100006 INSTITUTE (2FR PAR) Institut De Physique Nucleaire, Orsay B011000100007 REFERENCE (J,ZP/A,288,415,1978) B011000100008 (W,LAGARDE,1979) Numerical Values B011000100009 (T,LAGARDE,1979) Experimental Details B011000100010 (J,PR/C,14,1038,1976) Decay Data B011000100011 FACILITY (ISOCY,2FR PAR) Alice Accelerator at Orsay B011000100012 ERR-ANALYS The Errors Shown in the Thesis For One Point of Each B011000100013 Curve Only are 15-30%. They Include Mainly B011000100014 Uncertainties of the Activity Measurement, Beam B011000100015 Measurement (ABOUT 2%), and Target (ABOUT 3%). No B011000100016 Detailed Information is Given. B011000100017 MISC-COL (MISC) Excitation Energy of the Compound Nucleus in theB011000100018 Cm-System Calculated For the Middle of the Target As B011000100019 Given by the Authors. Using these Values the Compiler B011000100020 Of Kachapag has Calculated the Laboratory Energies B011000100021 Given. B011000100022 HISTORY (19791130C)Lapf B011000100023 (19940713A) Some Corrections have Been Included by B011000100024 CAJAD B011000100025 (19950403A). Some Corrections For 'Reaction'. B011000100026 (19981210A). Low Case Transform. Some Remarks For B011000100027 Decay-Data. B011000100028 (20011010U) Last checking has been done. B011000100029 ENDBIB 27 0 B011000100030 NOCOMMON 0 0 B011000100031 ENDSUBENT 30 0 B011000199999 SUBENT B0110002 20011220 0000B011000200001 BIB 6 33 B011000200002 REACTION (74-W-184(10-NE-20,4N)84-PO-200,,SIG,,,EXP) B011000200003 RAD-DET (84-PO-200,A) B011000200004 DECAY-DATA (84-PO-200,11.8MIN,A,5860.,0.14) B011000200005 SAMPLE W-Oxide (ENRICHMENT 94.3% W-184, THICKNESS B011000200006 0.3 MG/CM**2) Evaporated onto 1.2 Mg/Cm**2 Al-Backing. B011000200007 METHOD 1(EXTB,SITA,REC,EDEG,BCINT) B011000200008 For the Direct Determination of Absolute Cross SectionsB011000200009 At 104.5, 111, 116, and 121.5+-3 MeV Different Stacks B011000200010 Containing Al-Foils For Energy Degradation, the Target,B011000200011 And Al-Catcher Foils were Irradiated in a Faraday Cup. B011000200012 The Full Beam Energy was 140+-3 MeV. The Energy at theB011000200013 Middle of the Target was Calculated According to B011000200014 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011000200015 Corrected As Described by R.Bimbot,Et Al., Nucl.Instr. B011000200016 And Meth.153,161,78. After Each Irradiation the RecoilsB011000200017 In the Catcher Foils were Measured in an Alpha B011000200018 Ionization Chamber, and the Different Isotopes B011000200019 Identified by Their Half-Lives. B011000200020 2(EXTB,SITA,HEJET,EDEG,BCINT) B011000200021 Relative Cross Sections were Measured by the Hejet B011000200022 Technique and Normalized to Absolute Values by Means B011000200023 Of the Cross Sections Measured Directly. The Full Beam B011000200024 Energy Used was 140+-3 MeV. The Energy B011000200025 Degradation by Ni-Absorbers was Calculated According toB011000200026 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011000200027 Corrected As Described by R.Bimbot Et Al., Nucl.Instr. B011000200028 And Meth. 153,161,78. The Beam Current During the B011000200029 Irradiation was Measured by a Tungsten-Grid Which was B011000200030 Calibrated by Measurements with a Faraday Cup Before B011000200031 And After Each Irradiation. B011000200032 DETECTOR 1(IOCH).For Absolute Cross Sections Measured in the B011000200033 Al-Catcher Foils. B011000200034 2(SOLST).Mounted Within the Hejet Detection Chamber. B011000200035 ENDBIB 33 0 B011000200036 NOCOMMON 0 0 B011000200037 DATA 3 4 B011000200038 EN DATA MISC B011000200039 MEV MB MEV B011000200040 96. 0.5 52. B011000200041 100. 10.5 55.5 B011000200042 104. 22. 59. B011000200043 113. 10. 67. B011000200044 ENDDATA 6 0 B011000200045 ENDSUBENT 44 0 B011000299999 SUBENT B0110003 20011220 0000B011000300001 BIB 6 33 B011000300002 REACTION (74-W-184(10-NE-20,5N)84-PO-199-M,,SIG,,,EXP) B011000300003 RAD-DET (84-PO-199-M,A) B011000300004 DECAY-DATA (84-PO-199-M,4.2MIN,A,6070.,0.275) B011000300005 SAMPLE W-Oxide (ENRICHMENT 94.3% W-184, THICKNESS B011000300006 0.3 MG/CM**2) Evaporated onto 1.2 Mg/Cm**2 Al-Backing. B011000300007 METHOD 1(EXTB,SITA,REC,EDEG,BCINT) B011000300008 For the Direct Determination of Absolute Cross SectionsB011000300009 At 104.5, 111, 116, and 121.5+-3 MeV Different Stacks B011000300010 Containing Al-Foils For Energy Degradation, the Target,B011000300011 And Al-Catcher Foils were Irradiated in a Faraday Cup. B011000300012 The Full Beam Energy was 140+-3 MeV. The Energy at theB011000300013 Middle of the Target was Calculated According to B011000300014 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011000300015 Corrected As Described by R.Bimbot,Et Al., Nucl.Instr. B011000300016 And Meth.153,161,78. After Each Irradiation the RecoilsB011000300017 In the Catcher Foils were Measured in an Alpha B011000300018 Ionization Chamber, and the Different Isotopes B011000300019 Identified by Their Half-Lives. B011000300020 2(EXTB,SITA,HEJET,EDEG,BCINT) B011000300021 Relative Cross Sections were Measured by the Hejet B011000300022 Technique and Normalized to Absolute Values by Means B011000300023 Of the Cross Sections Measured Directly. The Full Beam B011000300024 Energies Used were 180+-4 and 140+-3 MeV. The Energy B011000300025 Degradation by Ni-Absorbers was Calculated According toB011000300026 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011000300027 Corrected As Described by R.Bimbot Et Al., Nucl.Instr. B011000300028 And Meth. 153,161,78. The Beam Current During the B011000300029 Irradiation was Measured by a Tungsten-Grid Which was B011000300030 Calibrated by Measurements with a Faraday Cup Before B011000300031 And After Each Irradiation. B011000300032 DETECTOR 1(IOCH).For Absolute Cross Sections Measured in the B011000300033 Al-Catcher Foils. B011000300034 2(SOLST).Mounted Within the Hejet Detection Chamber. B011000300035 ENDBIB 33 0 B011000300036 NOCOMMON 0 0 B011000300037 DATA 3 12 B011000300038 EN DATA MISC B011000300039 MEV MB MEV B011000300040 96. 0.1 52. B011000300041 100. 2. 55.5 B011000300042 100. 2.35 55.5 B011000300043 100. 3.3 55.5 B011000300044 104. 28.5 59. B011000300045 107. 46. 61.5 B011000300046 108. 66. 63. B011000300047 113. 97. 67. B011000300048 115. 110. 69. B011000300049 122. 28. 75.5 B011000300050 122. 31. 75.5 B011000300051 125. 15.5 77.5 B011000300052 ENDDATA 14 0 B011000300053 ENDSUBENT 52 0 B011000399999 SUBENT B0110004 20011220 0000B011000400001 BIB 6 33 B011000400002 REACTION (74-W-184(10-NE-20,6N)84-PO-198,,SIG,,,EXP) B011000400003 RAD-DET (84-PO-198,A) B011000400004 DECAY-DATA (84-PO-198,1.8MIN,A,6190.,0.70) B011000400005 SAMPLE W-Oxide (ENRICHMENT 94.3% W-184, THICKNESS B011000400006 0.3 MG/CM**2) Evaporated onto 1.2 Mg/Cm**2 Al-Backing. B011000400007 METHOD 1(EXTB,SITA,REC,EDEG,BCINT) B011000400008 For the Direct Determination of Absolute Cross SectionsB011000400009 At 104.5, 111, 116, and 121.5+-3 MeV Different Stacks B011000400010 Containing Al-Foils For Energy Degradation, the Target,B011000400011 And Al-Catcher Foils were Irradiated in a Faraday Cup. B011000400012 The Full Beam Energy was 140+-3 MeV. The Energy at theB011000400013 Middle of the Target was Calculated According to B011000400014 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011000400015 Corrected As Described by R.Bimbot,Et Al., Nucl.Instr. B011000400016 And Meth.153,161,78. After Each Irradiation the RecoilsB011000400017 In the Catcher Foils were Measured in an Alpha B011000400018 Ionization Chamber, and the Different Isotopes B011000400019 Identified by Their Half-Lives. B011000400020 2(EXTB,SITA,HEJET,EDEG,BCINT) B011000400021 Relative Cross Sections were Measured by the Hejet B011000400022 Technique and Normalized to Absolute Values by Means B011000400023 Of the Cross Sections Measured Directly. The Full Beam B011000400024 Energies Used were 180+-4 and 140+-3 MeV. The Energy B011000400025 Degradation by Ni-Absorbers was Calculated According toB011000400026 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011000400027 Corrected As Described by R.Bimbot Et Al., Nucl.Instr. B011000400028 And Meth. 153,161,78. The Beam Current During the B011000400029 Irradiation was Measured by a Tungsten-Grid Which was B011000400030 Calibrated by Measurements with a Faraday Cup Before B011000400031 And After Each Irradiation. B011000400032 DETECTOR 1(IOCH).For Absolute Cross Sections Measured in the B011000400033 Al-Catcher Foils. B011000400034 2(SOLST).Mounted Within the Hejet Detection Chamber. B011000400035 ENDBIB 33 0 B011000400036 NOCOMMON 0 0 B011000400037 DATA 3 21 B011000400038 EN DATA MISC B011000400039 MEV MB MEV B011000400040 100. 0.105 55.5 B011000400041 103. 0.32 58. B011000400042 104. 0.67 59. B011000400043 107. 1.45 61.5 B011000400044 113. 13. 67. B011000400045 116. 24. 70. B011000400046 123. 35. 76.5 B011000400047 123. 37.5 76.5 B011000400048 123. 47.5 76.5 B011000400049 129. 14.5 81.5 B011000400050 129. 15.25 81.5 B011000400051 129. 16.5 81.5 B011000400052 129. 17. 81.5 B011000400053 139. 3.85 90.5 B011000400054 145. 1.3 96. B011000400055 145. 1.9 96. B011000400056 150. 0.68 100. B011000400057 152. 0.49 102. B011000400058 155. 0.275 105. B011000400059 158. 0.21 108. B011000400060 162. 0.15 111. B011000400061 ENDDATA 23 0 B011000400062 ENDSUBENT 61 0 B011000499999 SUBENT B0110005 20011220 0000B011000500001 BIB 7 27 B011000500002 REACTION (74-W-184(10-NE-20,7N)84-PO-197,,SIG,,,EXP) B011000500003 RAD-DET (84-PO-197-M,A) B011000500004 (84-PO-197-G,A) B011000500005 DECAY-DATA (84-PO-197-M,27.SEC,A,6380.,1.00) B011000500006 (84-PO-197-G,52.SEC,A,6280.,1.00) B011000500007 The Abundances Given were Assumed by the Authors B011000500008 COMMENT - By Compiler of CAJAD - According to ENSDF Alpha B011000500009 Abundance For Po-197-M is 84+-9%, But For Po-197-G B011000500010 Is 44+-7%. B011000500011 SAMPLE W-Oxide (ENRICHMENT 94.3% W-184, THICKNESS B011000500012 0.3 MG/CM**2) Evaporated onto 1.2 Mg/Cm**2 Al-Backing. B011000500013 METHOD (EXTB,SITA,HEJET,EDEG,BCINT) B011000500014 Relative Cross Sections were Measured by the Hejet B011000500015 Technique. The Normalization to Absolute Values was B011000500016 Performed on the Basis of the Data For Po-198, B011000500017 Po-199-M, and Po-200 (SEE SUBENTRIES B0110002 TO 4) B011000500018 For Which Both Relative and Absolute Cross Sections B011000500019 Were Measured. B011000500020 The Full Beam Energy Used was 180+-4 MeV. The Energy B011000500021 Degradation by Ni-Absorbers was Calculated According toB011000500022 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011000500023 Corrected As Described by R.Bimbot Et Al., Nucl.Instr. B011000500024 And Meth. 153,161,78. The Beam Current During the B011000500025 Irradiation was Measured by a Tungsten-Grid Which was B011000500026 Calibrated by Measurements with a Faraday Cup Before B011000500027 And After Each Irradiation. B011000500028 DETECTOR (SOLST).Mounted Within the Hejet Detection Chamber. B011000500029 ENDBIB 27 0 B011000500030 NOCOMMON 0 0 B011000500031 DATA 3 16 B011000500032 EN DATA MISC B011000500033 MEV MB MEV B011000500034 113. 0.34 67. B011000500035 116. 0.4 70. B011000500036 123. 2.75 76.5 B011000500037 123. 3.35 76.5 B011000500038 125. 5.6 77.5 B011000500039 129. 10.5 81.5 B011000500040 129. 11.5 81.5 B011000500041 129. 13. 81.5 B011000500042 139. 10. 90.5 B011000500043 145. 5. 96. B011000500044 146. 5.15 96.5 B011000500045 150. 2.1 100. B011000500046 152. 1.5 102. B011000500047 155. 1.1 105. B011000500048 158. 0.78 108. B011000500049 162. 0.56 111. B011000500050 ENDDATA 18 0 B011000500051 ENDSUBENT 50 0 B011000599999 SUBENT B0110006 20011220 0000B011000600001 BIB 6 22 B011000600002 REACTION (74-W-184(10-NE-20,8N)84-PO-196,,SIG,,,EXP) B011000600003 RAD-DET (84-PO-196,A) B011000600004 DECAY-DATA (84-PO-196,5.5SEC,A,6520.,1.00) B011000600005 The Abundance Given was Assumed by the Authors. B011000600006 SAMPLE W-Oxide (ENRICHMENT 94.3% W-184, THICKNESS B011000600007 0.3 MG/CM**2) Evaporated onto 1.2 Mg/Cm**2 Al-Backing. B011000600008 METHOD (EXTB,SITA,HEJET,EDEG,BCINT) B011000600009 Relative Cross Sections were Measured by the Hejet B011000600010 Technique. The Normalization to Absolute Values was B011000600011 Performed on the Basis of the Data For Po-198, B011000600012 Po-199-M, and Po-200 (SEE SUBENTRIES B0110002 TO 4) B011000600013 For Which Both Relative and Absolute Cross Sections B011000600014 Were Measured. B011000600015 The Full Beam Energy Used was 180+-4 MeV. The Energy B011000600016 Degradation by Ni-Absorbers was Calculated According toB011000600017 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011000600018 Corrected As Described by R.Bimbot Et Al., Nucl.Instr. B011000600019 And Meth. 153,161,78. The Beam Current During the B011000600020 Irradiation was Measured by a Tungsten-Grid Which was B011000600021 Calibrated by Measurements with a Faraday Cup Before B011000600022 And After Each Irradiation. B011000600023 DETECTOR (SOLST).Mounted Within the Hejet Detection Chamber. B011000600024 ENDBIB 22 0 B011000600025 NOCOMMON 0 0 B011000600026 DATA 3 15 B011000600027 EN DATA MISC B011000600028 MEV MB MEV B011000600029 115. 0.025 69. B011000600030 122. 0.064 75.5 B011000600031 123. 0.12 76. B011000600032 123. 0.135 76.5 B011000600033 128. 0.26 81. B011000600034 128. 0.29 81. B011000600035 128. 0.35 81. B011000600036 139. 2.15 90.5 B011000600037 145. 4.2 96. B011000600038 150. 3.15 100. B011000600039 152. 2.6 102. B011000600040 155. 2.15 105. B011000600041 159. 1.95 109. B011000600042 162. 1.4 111. B011000600043 168. 0.7 117. B011000600044 ENDDATA 17 0 B011000600045 ENDSUBENT 44 0 B011000699999 SUBENT B0110007 20011220 0000B011000700001 BIB 6 26 B011000700002 REACTION M(74-W-184(10-NE-20,9N)84-PO-195-M,,SIG,,,EXP) B011000700003 G(74-W-184(10-NE-20,9N)84-PO-195-G,,SIG,,,EXP) B011000700004 RAD-DET M(84-PO-195-M,A) B011000700005 G(84-PO-195-G,A) B011000700006 DECAY-DATAM(84-PO-195-M,2.0SEC,A,6700.,1.00) B011000700007 The Abundance Given was Assumed by the Authors. B011000700008 G(84-PO-195-G,4.5SEC,A,6610.,1.00) B011000700009 The Abundance Given was Assumed by the Authors. B011000700010 SAMPLE W-Oxide (ENRICHMENT 94.3% W-184, THICKNESS B011000700011 0.3 MG/CM**2) Evaporated onto 1.2 Mg/Cm**2 Al-Backing. B011000700012 METHOD (EXTB,SITA,HEJET,EDEG,BCINT) B011000700013 Relative Cross Sections were Measured by the Hejet B011000700014 Technique. The Normalization to Absolute Values was B011000700015 Performed on the Basis of the Data For Po-198, B011000700016 Po-199-M, and Po-200 (SEE SUBENTRIES B0110002 TO 4) B011000700017 For Which Both Relative and Absolute Cross Sections B011000700018 Were Measured. B011000700019 The Full Beam Energy Used was 180+-4 MeV. The Energy B011000700020 Degradation by Ni-Absorbers was Calculated According toB011000700021 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011000700022 Corrected As Described by R.Bimbot Et Al., Nucl.Instr. B011000700023 And Meth. 153,161,78. The Beam Current During the B011000700024 Irradiation was Measured by a Tungsten-Grid Which was B011000700025 Calibrated by Measurements with a Faraday Cup Before B011000700026 And After Each Irradiation. B011000700027 DETECTOR (SOLST).Mounted Within the Hejet Detection Chamber. B011000700028 ENDBIB 26 0 B011000700029 NOCOMMON 0 0 B011000700030 DATA 4 8 B011000700031 EN DATA MDATA GMISC B011000700032 MEV MB MB MEV B011000700033 145. 0.06 0.084 96. B011000700034 146. 0.13 0.1 96.5 B011000700035 150. 0.14 0.108 100. B011000700036 152. 0.21 0.125 102. B011000700037 155. 0.31 0.195 105. B011000700038 159. 0.51 0.22 109. B011000700039 162. 0.59 0.25 111. B011000700040 168. 0.46 0.208 117. B011000700041 ENDDATA 10 0 B011000700042 ENDSUBENT 41 0 B011000799999 SUBENT B0110008 20011220 0000B011000800001 BIB 7 24 B011000800002 REACTION (66-DY-164(18-AR-40,4N)84-PO-200,,SIG,,,EXP) B011000800003 RAD-DET (84-PO-200,A) B011000800004 DECAY-DATA (84-PO-200,11.8MIN,A,5860.,0.14) B011000800005 SAMPLE Dy-Fluoride (ENRICHMENT 98.6% DY-164, THICKNESS B011000800006 0.2 MG/CM**2) Evaporated onto 1.3 Mg/Cm**2 Al-Backing. B011000800007 METHOD (EXTB,SITA,REC,EDEG,BCINT) B011000800008 For the Direct Determination of Absolute Cross SectionsB011000800009 At 10 Energies Between 160 and 210 MeV Different StacksB011000800010 Containing Al-Foils For Energy Degradation, the Target,B011000800011 And Al-Catcher Foils were Irradiated in a Faraday Cup. B011000800012 The Full Beam Energy was 210+-5 MeV. The Energy at theB011000800013 Middle of the Target was Calculated According to B011000800014 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011000800015 Corrected As Described by R.Bimbot,Et Al., Nucl.Instr. B011000800016 And Meth.153,161,78. After Each Irradiation the RecoilsB011000800017 In the Catcher Foils were Measured in an Alpha B011000800018 Ionization Chamber, and the Different Isotopes B011000800019 Identified by Their Half-Lives. B011000800020 CORRECTION In Addition the Beam Energy Scale was Refixed at B011000800021 Four Energies at 212, 233, 240, and 245+-1.5 MeV by B011000800022 Means of the Proton Recoil Method As Described by B011000800023 R.Bimbot Et Al., Rev.Phys.Appl.13,393,1978. B011000800024 DETECTOR (IOCH).For Absolute Cross Sections Measured in the B011000800025 Al-Catcher Foils. B011000800026 ENDBIB 24 0 B011000800027 NOCOMMON 0 0 B011000800028 DATA 3 5 B011000800029 EN DATA MISC B011000800030 MEV MB MEV B011000800031 162. 2.3 47. B011000800032 168. 15. 52. B011000800033 172. 20. 55.5 B011000800034 179. 6. 61. B011000800035 187. 2. 67. B011000800036 ENDDATA 7 0 B011000800037 ENDSUBENT 36 0 B011000899999 SUBENT B0110009 20011220 0000B011000900001 BIB 7 37 B011000900002 REACTION (66-DY-164(18-AR-40,5N)84-PO-199-M,,SIG,,,EXP) B011000900003 RAD-DET (84-PO-199-M,A) B011000900004 DECAY-DATA (84-PO-199-M,4.2MIN,A,6070.,0.275) B011000900005 SAMPLE Dy-Fluoride (ENRICHMENT 98.6% DY-164, THICKNESS B011000900006 0.2 MG/CM**2) Evaporated onto 1.3 Mg/Cm**2 Al-Backing. B011000900007 METHOD 1(EXTB,SITA,REC,EDEG,BCINT) B011000900008 For the Direct Determination of Absolute Cross SectionsB011000900009 At 10 Energies Between 160 and 210 MeV Different StacksB011000900010 Containing Al-Foils For Energy Degradation, the Target,B011000900011 And Al-Catcher Foils were Irradiated in a Faraday Cup. B011000900012 The Full Beam Energy was 210+-5 MeV. The Energy at theB011000900013 Middle of the Target was Calculated According to B011000900014 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011000900015 Corrected As Described by R.Bimbot,Et Al., Nucl.Instr. B011000900016 And Meth.153,161,78. After Each Irradiation the RecoilsB011000900017 In the Catcher Foils were Measured in an Alpha B011000900018 Ionization Chamber, and the Different Isotopes B011000900019 Identified by Their Half-Lives. B011000900020 2(EXTB,SITA,HEJET,EDEG,BCINT) B011000900021 Relative Cross Sections were Measured by the Hejet B011000900022 Technique and Normalized to Absolute Values by Means B011000900023 Of the Cross Sections Measured Directly. The Full Beam B011000900024 Energies Used were 280+-6 and 250+-5 MeV. The Energy B011000900025 Degradation by Ni-Absorbers was Calculated According toB011000900026 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011000900027 Corrected As Described by R.Bimbot Et Al., Nucl.Instr. B011000900028 And Meth. 153,161,78. The Beam Current During the B011000900029 Irradiation was Measured by a Tungsten-Grid Which was B011000900030 Calibrated by Measurements with a Faraday Cup Before B011000900031 And After Each Irradiation. B011000900032 CORRECTION In Addition the Beam Energy Scale was Refixed at B011000900033 Four Energies at 212, 233, 240, and 245+-1.5 MeV by B011000900034 Means of the Proton Recoil Method As Described by B011000900035 R.Bimbot Et Al., Rev.Phys.Appl.13,393,1978. B011000900036 DETECTOR 1(IOCH).For Absolute Cross Sections Measured in the B011000900037 Al-Catcher Foils. B011000900038 2(SOLST).Mounted Within the Hejet Detection Chamber. B011000900039 ENDBIB 37 0 B011000900040 NOCOMMON 0 0 B011000900041 DATA 3 5 B011000900042 EN DATA MISC B011000900043 MEV MB MEV B011000900044 182. 17. 63. B011000900045 184. 23.5 65. B011000900046 189. 25.5 69. B011000900047 195. 14. 73.5 B011000900048 204. 0.88 81. B011000900049 ENDDATA 7 0 B011000900050 ENDSUBENT 49 0 B011000999999 SUBENT B0110010 20011220 0000B011001000001 BIB 7 37 B011001000002 REACTION (66-DY-164(18-AR-40,6N)84-PO-198,,SIG,,,EXP) B011001000003 RAD-DET (84-PO-198,A) B011001000004 DECAY-DATA (84-PO-198,1.8MIN,A,6190.,0.70) B011001000005 SAMPLE Dy-Fluoride (ENRICHMENT 98.6% DY-164, THICKNESS B011001000006 0.2 MG/CM**2) Evaporated onto 1.3 Mg/Cm**2 Al-Backing. B011001000007 METHOD 1(EXTB,SITA,REC,EDEG,BCINT) B011001000008 For the Direct Determination of Absolute Cross SectionsB011001000009 At 10 Energies Between 160 and 210 MeV Different StacksB011001000010 Containing Al-Foils For Energy Degradation, the Target,B011001000011 And Al-Catcher Foils were Irradiated in a Faraday Cup. B011001000012 The Full Beam Energy was 210+-5 MeV. The Energy at theB011001000013 Middle of the Target was Calculated According to B011001000014 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011001000015 Corrected As Described by R.Bimbot,Et Al., Nucl.Instr. B011001000016 And Meth.153,161,78. After Each Irradiation the RecoilsB011001000017 In the Catcher Foils were Measured in an Alpha B011001000018 Ionization Chamber, and the Different Isotopes B011001000019 Identified by Their Half-Lives. B011001000020 2(EXTB,SITA,HEJET,EDEG,BCINT) B011001000021 Relative Cross Sections were Measured by the Hejet B011001000022 Technique and Normalized to Absolute Values by Means B011001000023 Of the Cross Sections Measured Directly. The Full Beam B011001000024 Energies Used were 280+-6 and 250+-5 MeV. The Energy B011001000025 Degradation by Ni-Absorbers was Calculated According toB011001000026 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011001000027 Corrected As Described by R.Bimbot Et Al., Nucl.Instr. B011001000028 And Meth. 153,161,78. The Beam Current During the B011001000029 Irradiation was Measured by a Tungsten-Grid Which was B011001000030 Calibrated by Measurements with a Faraday Cup Before B011001000031 And After Each Irradiation. B011001000032 CORRECTION In Addition the Beam Energy Scale was Refixed at B011001000033 Four Energies at 212, 233, 240, and 245+-1.5 MeV by B011001000034 Means of the Proton Recoil Method As Described by B011001000035 R.Bimbot Et Al., Rev.Phys.Appl.13,393,1978. B011001000036 DETECTOR 1(IOCH).For Absolute Cross Sections Measured in the B011001000037 Al-Catcher Foils. B011001000038 2(SOLST).Mounted Within the Hejet Detection Chamber. B011001000039 ENDBIB 37 0 B011001000040 NOCOMMON 0 0 B011001000041 DATA 3 9 B011001000042 EN DATA MISC B011001000043 MEV MB MEV B011001000044 184. 3.9 65. B011001000045 189. 8.7 69. B011001000046 195. 17. 73.5 B011001000047 204. 18. 81. B011001000048 206. 11. 82.5 B011001000049 211. 6.5 86.5 B011001000050 218. 2.25 92. B011001000051 218. 2.4 92. B011001000052 218. 2.85 92. B011001000053 ENDDATA 11 0 B011001000054 ENDSUBENT 53 0 B011001099999 SUBENT B0110011 20011220 0000B011001100001 BIB 8 31 B011001100002 REACTION (66-DY-164(18-AR-40,7N)84-PO-197,,SIG,,,EXP) B011001100003 RAD-DET (84-PO-197-M,A) B011001100004 (84-PO-197-G,A) B011001100005 DECAY-DATA (84-PO-197-M,27.SEC,A,6380.,1.00) B011001100006 The Abundance Given was Assumed by the Authors. B011001100007 (84-PO-197-G,52.SEC,A,6280.,1.00) B011001100008 The Abundance Given was Assumed by the Authors. B011001100009 COMMENT - By Compiler of CAJAD - According to ENSDF Alpha B011001100010 Abundance For Po-197-M is 84+-9%, But For Po-197-G B011001100011 Is 44+-7%. B011001100012 SAMPLE Dy-Fluoride (ENRICHMENT 98.6% DY-164, THICKNESS B011001100013 0.2 MG/CM**2) Evaporated onto 1.3 Mg/Cm**2 Al-Backing. B011001100014 METHOD (EXTB,SITA,HEJET,EDEG,BCINT) B011001100015 Relative Cross Sections were Measured by the Hejet B011001100016 Technique and Normalized to Absolute Values by Means B011001100017 Of the Factors Obtained from the Comparison of B011001100018 Absolute and Relative Cross Sections of Po-199-M and B011001100019 Po-198 (SEE SUBENTRIES B0110009 AND 10). The Full Beam B011001100020 Energies Used were 280+-6 and 250+-5 MeV. The Energy B011001100021 Degradation by Ni-Absorbers was Calculated According toB011001100022 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011001100023 Corrected As Described by R.Bimbot Et Al., Nucl.Instr. B011001100024 And Meth. 153,161,78. The Beam Current During the B011001100025 Irradiation was Measured by a Tungsten-Grid Which was B011001100026 Calibrated by Measurements with a Faraday Cup Before B011001100027 And After Each Irradiation. B011001100028 CORRECTION In Addition the Beam Energy Scale was Refixed at B011001100029 Four Energies at 212, 233, 240, and 245+-1.5 MeV by B011001100030 Means of the Proton Recoil Method As Described by B011001100031 R.Bimbot Et Al., Rev.Phys.Appl.13,393,1978. B011001100032 DETECTOR (SOLST).Mounted Within the Hejet Detection Chamber. B011001100033 ENDBIB 31 0 B011001100034 NOCOMMON 0 0 B011001100035 DATA 3 12 B011001100036 EN DATA MISC B011001100037 MEV MB MEV B011001100038 195. 0.46 73.5 B011001100039 195. 0.57 73.5 B011001100040 202. 3. 79. B011001100041 204. 6.1 81. B011001100042 206. 6. 82.5 B011001100043 211. 13.5 86.5 B011001100044 214. 14. 89. B011001100045 218. 10. 92. B011001100046 218. 12.5 92. B011001100047 220. 6.5 94. B011001100048 227. 1.55 99. B011001100049 233. 0.53 104. B011001100050 ENDDATA 14 0 B011001100051 ENDSUBENT 50 0 B011001199999 SUBENT B0110012 20011220 0000B011001200001 BIB 7 25 B011001200002 REACTION (66-DY-164(18-AR-40,8N)84-PO-196,,SIG,,,EXP) B011001200003 RAD-DET (84-PO-196,A) B011001200004 DECAY-DATA (84-PO-196,5.5SEC,A,6520.,1.00) B011001200005 The Abundance Given was Assumed by the Authors. B011001200006 SAMPLE Dy-Fluoride (ENRICHMENT 98.6% DY-164, THICKNESS B011001200007 0.2 MG/CM**2) Evaporated onto 1.3 Mg/Cm**2 Al-Backing. B011001200008 METHOD (EXTB,SITA,HEJET,EDEG,BCINT) B011001200009 Relative Cross Sections were Measured by the Hejet B011001200010 Technique and Normalized to Absolute Values by Means B011001200011 Of the Factors Obtained from the Comparison of B011001200012 Absolute and Relative Cross Sections of Po-199-M and B011001200013 Po-198 (SEE SUBENTRIES B0110009 AND 10). The Full Beam B011001200014 Energies Used were 280+-6 and 250+-5 MeV. The Energy B011001200015 Degradation by Ni-Absorbers was Calculated According toB011001200016 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011001200017 Corrected As Described by R.Bimbot Et Al., Nucl.Instr. B011001200018 And Meth. 153,161,78. The Beam Current During the B011001200019 Irradiation was Measured by a Tungsten-Grid Which was B011001200020 Calibrated by Measurements with a Faraday Cup Before B011001200021 And After Each Irradiation. B011001200022 CORRECTION In Addition the Beam Energy Scale was Refixed at B011001200023 Four Energies at 212, 233, 240, and 245+-1.5 MeV by B011001200024 Means of the Proton Recoil Method As Described by B011001200025 R.Bimbot Et Al., Rev.Phys.Appl.13,393,1978. B011001200026 DETECTOR (SOLST).Mounted Within the Hejet Detection Chamber. B011001200027 ENDBIB 25 0 B011001200028 NOCOMMON 0 0 B011001200029 DATA 3 8 B011001200030 EN DATA MISC B011001200031 MEV MB MEV B011001200032 206. 0.135 82.5 B011001200033 211. 0.64 86.5 B011001200034 218. 2.1 92. B011001200035 220. 3.4 94. B011001200036 227. 4. 99. B011001200037 233. 3. 104. B011001200038 239. 1.5 109. B011001200039 245. 0.54 114. B011001200040 ENDDATA 10 0 B011001200041 ENDSUBENT 40 0 B011001299999 SUBENT B0110013 20011220 0000B011001300001 BIB 7 28 B011001300002 REACTION (66-DY-164(18-AR-40,9N)84-PO-195-M,,SIG,,,EXP) B011001300003 RAD-DET (84-PO-195-M,A) B011001300004 (84-PO-195-G,A) B011001300005 DECAY-DATA (84-PO-195-M,2.0SEC,A,6700.,1.00) B011001300006 The Abundance Given was Assumed by the Authors. B011001300007 (84-PO-195-G,4.5SEC,A,6610.,1.00) B011001300008 The Abundance Given was Assumed by the Authors. B011001300009 SAMPLE Dy-Fluoride (ENRICHMENT 98.6% DY-164, THICKNESS B011001300010 0.2 MG/CM**2) Evaporated onto 1.3 Mg/Cm**2 Al-Backing. B011001300011 METHOD (EXTB,SITA,HEJET,EDEG,BCINT) B011001300012 Relative Cross Sections were Measured by the Hejet B011001300013 Technique and Normalized to Absolute Values by Means B011001300014 Of the Factors Obtained from the Comparison of B011001300015 Absolute and Relative Cross Sections of Po-199-M and B011001300016 Po-198 (SEE SUBENTRIES B0110009 AND 10). The Full Beam B011001300017 Energies Used were 280+-6 and 250+-5 MeV. The Energy B011001300018 Degradation by Ni-Absorbers was Calculated According toB011001300019 Northcliffe and Schilling, Nucl.Data Tables A7,233,70, B011001300020 Corrected As Described by R.Bimbot Et Al., Nucl.Instr. B011001300021 And Meth. 153,161,78. The Beam Current During the B011001300022 Irradiation was Measured by a Tungsten-Grid Which was B011001300023 Calibrated by Measurements with a Faraday Cup Before B011001300024 And After Each Irradiation. B011001300025 CORRECTION In Addition the Beam Energy Scale was Refixed at B011001300026 Four Energies at 212, 233, 240, and 245+-1.5 MeV by B011001300027 Means of the Proton Recoil Method As Described by B011001300028 R.Bimbot Et Al., Rev.Phys.Appl.13,393,1978. B011001300029 DETECTOR (SOLST).Mounted Within the Hejet Detection Chamber. B011001300030 ENDBIB 28 0 B011001300031 NOCOMMON 0 0 B011001300032 DATA 3 6 B011001300033 EN DATA MISC B011001300034 MEV MB MEV B011001300035 227. 0.25 99. B011001300036 233. 0.56 104. B011001300037 239. 0.8 109. B011001300038 245. 0.8 114. B011001300039 251. 0.45 119. B011001300040 258. 0.13 124. B011001300041 ENDDATA 8 0 B011001300042 ENDSUBENT 41 0 B011001399999 ENDENTRY 13 0 B011099999999