ENTRY D6319 20190408 D120D631900000001 SUBENT D6319001 20190408 D120D631900100001 BIB 12 32 D631900100002 TITLE Relationship between and effect of inelastic D631900100003 excitations and transfer channels on sub-barrier D631900100004 fusion enhancement D631900100005 AUTHOR (Khushboo, S.Mandal, S.Nath, N.Madhavan, J.Gehlot, D631900100006 A.Jhingan, N.Kumar, T.Banerjee, G.Kaur, K.R.Devi, D631900100007 A.Banerjee, Neelam, T.Varughese, D.Siwal, R.Garg, D631900100008 I.Mukul, M.Saxena, S.Verma, S.Kumar, B.R.Behera, D631900100009 P.Verma) D631900100010 INSTITUTE (3INDDLH,3INDNSD,3INDPUC) D631900100011 REFERENCE (J,PR/C,96,014614,2017) D631900100012 FACILITY (VDGT,3INDNSD) Pelletron accelerator D631900100013 DETECTOR (MAGSP,MWPC) Evaporation residues were detected D631900100014 through a 15.2 X 5.1 cm2 multiwire proportional D631900100015 counter (MWPC) operated at a pressure of 3 mbar of D631900100016 isobutane gas. D631900100017 (SIBAR) Two silicon-surface barrier detectors were D631900100018 mounted symmetrically at angle 15.5 degree with D631900100019 respect to beam direction at a distance of 10 cm from D631900100020 the target. The detectors were used for beam direction D631900100021 monitor and cross section normalization. D631900100022 METHOD (TOF) Delta E-TOF for evaporation residue selection. D631900100023 (ASEP) Fusion cross-sections were measured using the D631900100024 Heavy Ion Reaction Analyzer (HIRA). D631900100025 ANALYSIS (NTRTH) D631900100026 ERR-ANALYS (ERR-T) The experimental errors includes statistical D631900100027 error and HIRA efficiency error D631900100028 (ERR-1) The uncertainty due to HIRA efficiency D631900100029 determination (10%) D631900100030 CORRECTION Energies are corrected for energy loss in the carbon D631900100031 backing and target half thickness. D631900100032 STATUS (TABLE) Table I of Phys. Rev. C, 96 (2017) 014614 D631900100033 HISTORY (20190408C) VT D631900100034 ENDBIB 32 0 D631900100035 COMMON 1 3 D631900100036 ERR-1 D631900100037 PER-CENT D631900100038 10. D631900100039 ENDCOMMON 3 0 D631900100040 ENDSUBENT 39 0 D631900199999 SUBENT D6319002 20190408 D120D631900200001 BIB 3 6 D631900200002 REACTION (40-ZR-96(14-SI-28,FUS),,SIG,ER) D631900200003 SAMPLE (40-ZR-96,ENR=0.864) target having thickness 85 ug/cm2 D631900200004 was prepared on backing of thickness 20 ug/cm2 using D631900200005 electron beam evaporation technique. D631900200006 CORRECTION The fusion cross sections are corrected for isotopic D631900200007 impurity in the target of 96ZrO2. D631900200008 ENDBIB 6 0 D631900200009 NOCOMMON 0 0 D631900200010 DATA 3 15 D631900200011 EN-CM DATA ERR-T D631900200012 MEV MB MB D631900200013 63.0 0.11 0.02 D631900200014 64.5 1.43 0.22 D631900200015 66.1 7.03 1.06 D631900200016 67.7 20.23 3.07 D631900200017 69.2 39.19 5.92 D631900200018 70.8 51.76 7.80 D631900200019 72.4 116.3 17.6 D631900200020 73.9 159.8 24.6 D631900200021 75.4 212.7 32.5 D631900200022 77.7 317.4 48.0 D631900200023 80.1 397.6 60.1 D631900200024 83.2 485.4 74.1 D631900200025 85.5 548.8 83.5 D631900200026 89.4 689.8 104.6 D631900200027 92.5 778.6 121.9 D631900200028 ENDDATA 17 0 D631900200029 ENDSUBENT 28 0 D631900299999 SUBENT D6319003 20190408 D120D631900300001 BIB 2 4 D631900300002 REACTION (40-ZR-92(14-SI-28,FUS),,SIG,ER) D631900300003 SAMPLE (40-ZR-96,ENR=0.9513) target having thickness 265 D631900300004 ug/cm2 was prepared on backing of thickness 50 ug/cm2 D631900300005 using electron beam evaporation technique. D631900300006 ENDBIB 4 0 D631900300007 NOCOMMON 0 0 D631900300008 DATA 3 4 D631900300009 EN-CM DATA ERR-T D631900300010 MEV MB MB D631900300011 67.8 7.03 1.06 D631900300012 70.9 53.68 8.06 D631900300013 76.3 253.02 37.98 D631900300014 84.0 535.69 80.37 D631900300015 ENDDATA 6 0 D631900300016 ENDSUBENT 15 0 D631900399999 ENDENTRY 3 0 D631999999999