ENTRY A0865 20110323 A071A086500000001 SUBENT A0865001 20110323 A071A086500100001 BIB 11 24 A086500100002 TITLE Investigation of di-nuclear systems as entrance channelA086500100003 to fusion. A086500100004 AUTHOR (S.Heinz, V.Comas, S.Hofmann, D.Ackermann, J.Heredia, A086500100005 F.P.Hessberger, B.Kindler, B.Lommel, R.Mann) A086500100006 INSTITUTE (2GERGSI) A086500100007 (3CUBHAB) A086500100008 (2GERFRK) A086500100009 REFERENCE (J,EPJ/A,43,181,2010) A086500100010 (J,RMP,72,733,2000) A086500100011 REL-REF (I,C1712001,A.N.Andreyev+,J,PR/C,79,064320,2009) A086500100012 FACILITY (LINAC,2GERGSI) Experiment performed using UNILAC A086500100013 accelerator and velocity filter SHIP at GSI Darmstadt A086500100014 SAMPLE The targets were prepared from isotopically enriched A086500100015 Pb-207. Layers of 380 mug/cm**2 thickness of the A086500100016 chemical compound Pb-207-S have been evaporated on A086500100017 carbon foils of 40 mug/cm**2 and covered by A086500100018 10 mug/cm**2 carbon. A086500100019 DETECTOR (MAGSP) Velocity separator SHIP with crossed A086500100020 magnetic and electric fields was used A086500100021 (SISD) A086500100022 METHOD (OLMS) On-line velocity separation A086500100023 STATUS (TABLE).Data were received from Sophia Heinz A086500100024 (APRVD).By S. Heinz A086500100025 HISTORY (20110323C) S.B. A086500100026 ENDBIB 24 0 A086500100027 NOCOMMON 0 0 A086500100028 ENDSUBENT 27 0 A086500199999 SUBENT A0865002 20110323 A071A086500200001 BIB 2 3 A086500200002 REACTION (82-PB-208(26-FE-58,N)108-HS-265,,SIG) fig.1a A086500200003 STATUS (TABLE).Data were received from Sophia Heinz for A086500200004 J,RMP,72,733,2000 A086500200005 ENDBIB 3 0 A086500200006 NOCOMMON 0 0 A086500200007 DATA 2 7 A086500200008 EN-CM DATA A086500200009 MEV PB A086500200010 215.9 14.7 A086500200011 216.8 44.9 A086500200012 217.9 67. A086500200013 219.0 69. A086500200014 220.6 44.8 A086500200015 222.1 23.1 A086500200016 224.8 2.27 A086500200017 ENDDATA 9 0 A086500200018 ENDSUBENT 17 0 A086500299999 SUBENT A0865003 20110323 A071A086500300001 BIB 2 3 A086500300002 REACTION (82-PB-208(28-NI-64,N)110-DS-271,,SIG) fig.1b A086500300003 STATUS (TABLE).Data were received from Sophia Heinz for A086500300004 J,RMP,72,733,2000 A086500300005 ENDBIB 3 0 A086500300006 NOCOMMON 0 0 A086500300007 DATA 2 3 A086500300008 EN-CM DATA A086500300009 MEV PB A086500300010 236.24 7.4 A086500300011 237.27 15. A086500300012 239.23 3.6 A086500300013 ENDDATA 5 0 A086500300014 ENDSUBENT 13 0 A086500399999 SUBENT A0865004 20110323 A071A086500400001 BIB 3 12 A086500400002 REACTION (82-PB-207(28-NI-64,X)84-PO-211,,DA) fig.1c A086500400003 COMMENT *By author*. The double differential cross-sections areA086500400004 related to the acceptance angle of the separator, A086500400005 which is (0 +-2) degree and to the setting which leads A086500400006 to optimized transmission of the respective transfer A086500400007 product. Corrections for the transmission have not beenA086500400008 done, therefore, the cross-sections could be up to a A086500400009 factor of two larger after correction. This is a rough A086500400010 guess. The cross-sections in the table are given in A086500400011 nb/sr. The beam energy is given in the centre-of-mass. A086500400012 STATUS (TABLE).Data were received from Sophia Heinz for A086500400013 J,EPJ/A,43,181,2010 A086500400014 ENDBIB 12 0 A086500400015 COMMON 2 3 A086500400016 ANG-MIN ANG-MAX A086500400017 ADEG ADEG A086500400018 0. 2. A086500400019 ENDCOMMON 3 0 A086500400020 DATA 2 5 A086500400021 EN-CM DATA-CM A086500400022 MEV NB/SR A086500400023 234.7 1634. A086500400024 244.4 789. A086500400025 254.2 200. A086500400026 264.0 22. A086500400027 270.3 7.7 A086500400028 ENDDATA 7 0 A086500400029 ENDSUBENT 28 0 A086500499999 SUBENT A0865005 20110323 A071A086500500001 BIB 3 12 A086500500002 REACTION (82-PB-207(28-NI-64,X)85-AT-212,,DA) fig.1c A086500500003 STATUS (TABLE).Data were received from Sophia Heinz for A086500500004 J,EPJ/A,43,181,2010 A086500500005 COMMENT *By author*. The double differential cross-sections areA086500500006 related to the acceptance angle of the separator, A086500500007 which is (0 +-2 ) degree and to the setting which leadsA086500500008 to optimized transmission of the respective transfer A086500500009 product. Corrections for the transmission have not beenA086500500010 done, therefore, the cross-sections could be up to a A086500500011 factor of two larger after correction. This is a rough A086500500012 guess. The cross-sections in the table are given in A086500500013 nb/sr. The beam energy is given in the centre-of-mass. A086500500014 ENDBIB 12 0 A086500500015 COMMON 2 3 A086500500016 ANG-MIN ANG-MAX A086500500017 ADEG ADEG A086500500018 0. 2. A086500500019 ENDCOMMON 3 0 A086500500020 DATA 2 6 A086500500021 EN-CM DATA-CM A086500500022 MEV NB/SR A086500500023 234.7 366. A086500500024 244.4 1087. A086500500025 254.2 330. A086500500026 264.0 60. A086500500027 270.3 44. A086500500028 289.4 3. A086500500029 ENDDATA 8 0 A086500500030 ENDSUBENT 29 0 A086500599999 SUBENT A0865006 20110323 A071A086500600001 BIB 3 12 A086500600002 REACTION (82-PB-207(28-NI-64,X)86-RN-213,,DA) fig.1c A086500600003 STATUS (TABLE).Data were received from Sophia Heinz for A086500600004 J,EPJ/A,43,181,2010 A086500600005 COMMENT *By author*. The double differential cross-sections areA086500600006 related to the acceptance angle of the separator, A086500600007 which is (0+- 2) degree and to the setting which leads A086500600008 to optimized transmission of the respective transfer A086500600009 product. Corrections for the transmission have not beenA086500600010 done, therefore, the cross-sections could be up to a A086500600011 factor of two larger after correction. This is a rough A086500600012 guess. The cross-sections in the table are given in A086500600013 nb/sr. The beam energy is given in the centre-of-mass. A086500600014 ENDBIB 12 0 A086500600015 COMMON 2 3 A086500600016 ANG-MIN ANG-MAX A086500600017 ADEG ADEG A086500600018 0. 2. A086500600019 ENDCOMMON 3 0 A086500600020 DATA 2 6 A086500600021 EN-CM DATA-CM A086500600022 MEV NB/SR A086500600023 234.7 254. A086500600024 244.4 1153. A086500600025 254.2 469. A086500600026 264.0 120. A086500600027 270.3 48. A086500600028 289.4 11. A086500600029 ENDDATA 8 0 A086500600030 ENDSUBENT 29 0 A086500699999 SUBENT A0865007 20110323 A071A086500700001 BIB 3 12 A086500700002 REACTION (82-PB-207(28-NI-64,X)87-FR-213,,DA) fig.1c A086500700003 STATUS (TABLE).Data were received from Sophia Heinz for A086500700004 J,EPJ/A,43,181,2010 A086500700005 COMMENT *By author*. The double differential cross-sections areA086500700006 related to the acceptance angle of the separator, A086500700007 which is (0 +-2) degree and to the setting which leads A086500700008 to optimized transmission of the respective transfer A086500700009 product. Corrections for the transmission have not beenA086500700010 done, therefore, the cross-sections could be up to a A086500700011 factor of two larger after correction. This is a rough A086500700012 guess. The cross-sections in the table are given in A086500700013 nb/sr. The beam energy is given in the centre-of-mass. A086500700014 ENDBIB 12 0 A086500700015 COMMON 2 3 A086500700016 ANG-MIN ANG-MAX A086500700017 ADEG ADEG A086500700018 0. 2. A086500700019 ENDCOMMON 3 0 A086500700020 DATA 2 6 A086500700021 EN-CM DATA-CM A086500700022 MEV NB/SR A086500700023 234.7 11. A086500700024 244.4 182. A086500700025 254.2 244. A086500700026 264.0 157. A086500700027 270.3 92. A086500700028 289.4 30. A086500700029 ENDDATA 8 0 A086500700030 ENDSUBENT 29 0 A086500799999 SUBENT A0865008 20110323 A071A086500800001 BIB 3 12 A086500800002 REACTION (82-PB-207(28-NI-64,X)88-RA-214,,DA) fig.1c A086500800003 STATUS (TABLE).Data were received from Sophia Heinz for A086500800004 J,EPJ/A,43,181,2010 A086500800005 COMMENT *By author*. The double differential cross-sections areA086500800006 related to the acceptance angle of the separator, A086500800007 which is (0+- 2) degree and to the setting which leads A086500800008 to optimized transmission of the respective transfer A086500800009 product. Corrections for the transmission have not beenA086500800010 done, therefore, the cross-sections could be up to a A086500800011 factor of two larger after correction. This is a rough A086500800012 guess. The cross-sections in the table are given in A086500800013 nb/sr. The beam energy is given in the centre-of-mass. A086500800014 ENDBIB 12 0 A086500800015 COMMON 2 3 A086500800016 ANG-MIN ANG-MAX A086500800017 ADEG ADEG A086500800018 0. 2. A086500800019 ENDCOMMON 3 0 A086500800020 DATA 2 6 A086500800021 EN-CM DATA-CM A086500800022 MEV NB/SR A086500800023 234.7 10. A086500800024 244.4 25. A086500800025 254.2 35. A086500800026 264.0 30. A086500800027 270.3 27. A086500800028 289.4 11. A086500800029 ENDDATA 8 0 A086500800030 ENDSUBENT 29 0 A086500899999 SUBENT A0865009 20110323 A071A086500900001 BIB 2 3 A086500900002 REACTION (82-PB-207(28-NI-64,X)84-PO-211,,KE) fig.2 A086500900003 STATUS (TABLE).Data were received from Sophia Heinz for A086500900004 J,EPJ/A,43,181,2010 A086500900005 ENDBIB 3 0 A086500900006 NOCOMMON 0 0 A086500900007 DATA 2 4 A086500900008 EN-CM DATA-CM A086500900009 MEV MEV A086500900010 234.7 150. A086500900011 244.4 163. A086500900012 254.2 162. A086500900013 264.0 148. A086500900014 ENDDATA 6 0 A086500900015 ENDSUBENT 14 0 A086500999999 SUBENT A0865010 20110323 A071A086501000001 BIB 2 3 A086501000002 REACTION (82-PB-207(28-NI-64,X)85-AT-212,,KE) fig.2 A086501000003 STATUS (TABLE).Data were received from Sophia Heinz for A086501000004 J,EPJ/A,43,181,2010 A086501000005 ENDBIB 3 0 A086501000006 NOCOMMON 0 0 A086501000007 DATA 2 5 A086501000008 EN-CM DATA-CM A086501000009 MEV MEV A086501000010 234.7 144. A086501000011 244.4 154. A086501000012 254.2 151. A086501000013 264.0 145. A086501000014 270.3 140. A086501000015 ENDDATA 7 0 A086501000016 ENDSUBENT 15 0 A086501099999 SUBENT A0865011 20110323 A071A086501100001 BIB 2 3 A086501100002 REACTION (82-PB-207(28-NI-64,X)86-RN-213,,KE) fig.2 A086501100003 STATUS (TABLE).Data were received from Sophia Heinz for A086501100004 J,EPJ/A,43,181,2010 A086501100005 ENDBIB 3 0 A086501100006 NOCOMMON 0 0 A086501100007 DATA 2 6 A086501100008 EN-CM DATA-CM A086501100009 MEV MEV A086501100010 234.7 138. A086501100011 244.4 148. A086501100012 254.2 148. A086501100013 264.0 143. A086501100014 270.3 135. A086501100015 289.4 137. A086501100016 ENDDATA 8 0 A086501100017 ENDSUBENT 16 0 A086501199999 SUBENT A0865012 20110323 A071A086501200001 BIB 2 3 A086501200002 REACTION (82-PB-207(28-NI-64,X)87-FR-213,,KE) fig.2 A086501200003 STATUS (TABLE).Data were received from Sophia Heinz for A086501200004 J,EPJ/A,43,181,2010 A086501200005 ENDBIB 3 0 A086501200006 NOCOMMON 0 0 A086501200007 DATA 2 6 A086501200008 EN-CM DATA-CM A086501200009 MEV MEV A086501200010 234.7 135. A086501200011 244.4 134. A086501200012 254.2 135. A086501200013 264.0 136. A086501200014 270.3 127. A086501200015 289.4 132. A086501200016 ENDDATA 8 0 A086501200017 ENDSUBENT 16 0 A086501299999 SUBENT A0865013 20110323 A071A086501300001 BIB 2 3 A086501300002 REACTION (82-PB-207(28-NI-64,X)88-RA-214,,KE) fig.2 A086501300003 STATUS (TABLE).Data were received from Sophia Heinz for A086501300004 J,EPJ/A,43,181,2010 A086501300005 ENDBIB 3 0 A086501300006 NOCOMMON 0 0 A086501300007 DATA 2 6 A086501300008 EN-CM DATA-CM A086501300009 MEV MEV A086501300010 234.7 140. A086501300011 244.4 131. A086501300012 254.2 126. A086501300013 264.0 131. A086501300014 270.3 121. A086501300015 289.4 129. A086501300016 ENDDATA 8 0 A086501300017 ENDSUBENT 16 0 A086501399999 ENDENTRY 13 0 A086599999999