ENTRY O2289 20160717 O060O228900000001 SUBENT O2289001 20160717 O060O228900100001 BIB 10 25 O228900100002 TITLE Sub-barrier radioactive ion beam investigations using aO228900100003 new methodology and analysis for the stacked target O228900100004 technique. O228900100005 AUTHOR (M.Fisichella,A.C.Shotter,A.Di Pietro,P.Figuera, O228900100006 M.Lattuada,C.Marchetta,V.Privitera,L.Romano,C.Ruiz, O228900100007 M.Zadro) O228900100008 INSTITUTE (2ITYLNS,2UK EDG,2ITYCAT,1CANTMF,3CRORBZ) O228900100009 REFERENCE (J,PR/C,92,064611,2015) O228900100010 FACILITY (VDGT,2ITYLNS) O228900100011 METHOD (STTA,ACTIV) O228900100012 SAMPLE Two stacks made of four 120Sn targets with an average O228900100013 thickness of 0.5mg/cm**2, evaporated on 93Nb catcher O228900100014 foils of 1.5mg/cm2,were irradiated by 6Li beams, O228900100015 delivered by the Tandem Van de Graaff, at E(lab)=25 MeVO228900100016 and at E(lab)= 21 MeV,respectively. O228900100017 From this data mean cross-section were deduced. O228900100018 The targets were characterized by determining their O228900100019 surface morphology-from this information functions for O228900100020 each target in the stack could be determined and the O228900100021 corresponding values of E-mean beam energy and O228900100022 E-effective could be calculated. O228900100023 DETECTOR (SILI) O228900100024 ERR-ANALYS (DATA-ERR).The uncertainty associated with the O228900100025 experimental procedure.Any information is absent. O228900100026 HISTORY (20160717C) SB O228900100027 ENDBIB 25 0 O228900100028 NOCOMMON 0 0 O228900100029 ENDSUBENT 28 0 O228900199999 SUBENT O2289002 20160717 O060O228900200001 BIB 3 10 O228900200002 REACTION (50-SN-120(3-LI-9,FUS),,SIG,ER) O228900200003 uniform targets O228900200004 STATUS (CURVE).Fig 14 of J,PR/C,92,064611,2015 O228900200005 (COREL,O2289003) Data from nonuniform target O228900200006 COMMENT The fusion cross-section plotted versus E-mean beam O228900200007 energy and E-eff. In the case of uniform targets it is O228900200008 expected that the E-eff energy is always shifted towardO228900200009 higher values with respect to E-mean energy because O228900200010 of the weighted average with the exponential increasingO228900200011 cross-section. O228900200012 ENDBIB 10 0 O228900200013 NOCOMMON 0 0 O228900200014 DATA 3 8 O228900200015 EN DATA DATA-ERR O228900200016 MEV MB MB O228900200017 17.41 1.644E+00 2.760E-01 O228900200018 18.59 9.073E+00 1.441E+00 O228900200019 19.67 3.429E+01 4.496E+00 O228900200020 20.81 8.975E+01 1.261E+01 O228900200021 21.24 1.056E+02 1.482E+01 O228900200022 22.47 1.892E+02 3.006E+01 O228900200023 23.68 2.948E+02 3.865E+01 O228900200024 24.85 3.990E+02 8.103E+01 O228900200025 ENDDATA 10 0 O228900200026 ENDSUBENT 25 0 O228900299999 SUBENT O2289003 20160717 O060O228900300001 BIB 3 10 O228900300002 REACTION (50-SN-120(3-LI-9,FUS),,SIG,ER) O228900300003 nonuniform targets O228900300004 STATUS (CURVE).Fig 14 of J,PR/C,92,064611,2015 O228900300005 (COREL,O2289002) Data from uniform target O228900300006 COMMENT The fusion cross-section plotted versus E-mean beam O228900300007 energy and E-eff.For a nonuniform target with a cross- O228900300008 section independent of beam energy, Eeff < E-mean, O228900300009 since the incoming beam particles can locally explore O228900300010 a target thickness larger than the average one, O228900300011 thus reducing the average interaction energy. O228900300012 ENDBIB 10 0 O228900300013 NOCOMMON 0 0 O228900300014 DATA 3 8 O228900300015 EN DATA DATA-ERR O228900300016 MEV MB MB O228900300017 17.30 1.644E+00 3.197E-01 O228900300018 18.41 8.783E+00 1.152E+00 O228900300019 19.55 3.356E+01 4.400E+00 O228900300020 20.65 8.689E+01 1.057E+01 O228900300021 21.07 1.033E+02 1.354E+01 O228900300022 22.35 1.892E+02 2.481E+01 O228900300023 23.56 2.885E+02 3.509E+01 O228900300024 24.74 3.904E+02 5.844E+01 O228900300025 ENDDATA 10 0 O228900300026 ENDSUBENT 25 0 O228900399999 ENDENTRY 3 0 O228999999999