ENTRY C2240 20161006 C165C2240 0 1 SUBENT C2240001 20160920 C165C2240 1 1 BIB 6 10 C2240 1 2 TITLE Examining the role of transfer coupling in sub-barrier C2240 1 3 fusion of 46,50Ti+124Sn C2240 1 4 AUTHOR (J.F.Liang,J.M.Allmond,C.J.Gross,P.E.Mueller,D.Shapira,C2240 1 5 R.L.Varner,M.Dasgupta,D.J.Hinde,C.Simenel,E.Williams, C2240 1 6 K.Vo-Phuoc,M.L.Brown,I.P.Carter,M.Evers,D.H.Luong, C2240 1 7 T.Ebadi,A.Wakhle) C2240 1 8 INSTITUTE (1USAORL,3AULCBR) C2240 1 9 REFERENCE (J,PR/C,94,024616,2016) C2240 1 10 ERR-ANALYS (DATA-ERR) Total uncertainty C2240 1 11 HISTORY (20160920C) Compiled by S.H. C2240 1 12 ENDBIB 10 0 C2240 1 13 NOCOMMON 0 0 C2240 1 14 ENDSUBENT 13 0 C2240 199999 SUBENT C2240002 20160920 C165C2240 2 1 BIB 6 14 C2240 2 2 REACTION (22-TI-46(50-SN-124,FUS),,SIG,ER) C2240 2 3 STATUS (CURVE) Data taken from fig. 2a of the reference, C2240 2 4 waiting for data from author C2240 2 5 FACILITY (VDGT,1USAORL) Experiment was performed at the C2240 2 6 Holifield Radioactive Ion Beam Facility at Oak Ridge C2240 2 7 National Laboratory. C2240 2 8 DETECTOR (MCPLT,IOCH) The evaporation residues were identified C2240 2 9 by time-of-flight using microchannel-plate timing C2240 2 10 detectors and energy loss using a multi-anode C2240 2 11 ionization chamber. C2240 2 12 SAMPLE Enriched 46Ti self-supporting metallic foil with C2240 2 13 thickness of 295 mu-g/cm2 (ORNL). C2240 2 14 INC-SOURCE 124Sn beam accelerated by the 25 MV tandem C2240 2 15 accelerator to energies near the Coulomb barrier C2240 2 16 ENDBIB 14 0 C2240 2 17 NOCOMMON 0 0 C2240 2 18 DATA 3 11 C2240 2 19 EN-CM DATA DATA-ERR C2240 2 20 MEV MB MB C2240 2 21 120.89 6.83 1.36 C2240 2 22 123.51 20.19 3.09 C2240 2 23 126.35 42.85 C2240 2 24 128.79 96.10 C2240 2 25 131.50 133.93 C2240 2 26 134.25 190.83 C2240 2 27 138.31 263.02 C2240 2 28 142.36 297.06 C2240 2 29 146.45 387.40 C2240 2 30 150.51 467.57 C2240 2 31 154.57 447.32 C2240 2 32 ENDDATA 13 0 C2240 2 33 ENDSUBENT 32 0 C2240 299999 SUBENT C2240003 20160920 C165C2240 3 1 BIB 6 18 C2240 3 2 REACTION ((50-SN-124(22-TI-46,FUS),,SIG,ER)= C2240 3 3 (22-TI-46(50-SN-124,FUS),,SIG,ER)) C2240 3 4 STATUS (CURVE) Data taken from fig. 2a of the reference, C2240 3 5 waiting for data from author C2240 3 6 FACILITY (VDGT,3AULCBR) A follow-up measurement was carried out C2240 3 7 using 14UD tandem electrostatic accelerator at the C2240 3 8 Australian National University. C2240 3 9 DETECTOR (MAGSP) The evaporation residues were transported in C2240 3 10 the superconducting solenoid SOLITAIRE and detected C2240 3 11 at and behind the focus C2240 3 12 (MWPC) The evaporation residues were detected by two C2240 3 13 multiwire proportional counters at and behind the C2240 3 14 focus. C2240 3 15 SAMPLE Enriched 124Sn targets with thickness of 17 mu-g/cm2 C2240 3 16 evaporated onto 20 mu-g/cm2 carbon backings C2240 3 17 were used C2240 3 18 INC-SOURCE 46Ti beam accelerated by the 14UD tandem electrostatic C2240 3 19 accelerator C2240 3 20 ENDBIB 18 0 C2240 3 21 NOCOMMON 0 0 C2240 3 22 DATA 3 24 C2240 3 23 EN-CM DATA DATA-ERR C2240 3 24 MEV MB MB C2240 3 25 115.68 0.15 0.02 C2240 3 26 116.68 0.35 C2240 3 27 117.64 0.68 C2240 3 28 118.67 1.28 C2240 3 29 119.77 2.50 C2240 3 30 120.77 4.44 C2240 3 31 121.76 7.88 C2240 3 32 122.83 12.01 C2240 3 33 123.86 19.32 C2240 3 34 124.89 26.92 C2240 3 35 125.98 39.66 C2240 3 36 126.91 51.72 C2240 3 37 127.98 67.45 C2240 3 38 128.91 83.23 C2240 3 39 130.16 102.70 C2240 3 40 131.00 121.24 C2240 3 41 132.00 141.55 C2240 3 42 133.00 159.87 C2240 3 43 134.06 186.65 C2240 3 44 135.09 199.46 C2240 3 45 136.12 222.80 C2240 3 46 137.15 235.47 C2240 3 47 138.18 260.12 C2240 3 48 140.27 300.36 31.46 C2240 3 49 ENDDATA 26 0 C2240 3 50 ENDSUBENT 49 0 C2240 399999 SUBENT C2240004 20160920 C165C2240 4 1 BIB 6 14 C2240 4 2 REACTION (22-TI-50(50-SN-124,FUS),,SIG,ER) C2240 4 3 STATUS (CURVE) Data taken from fig. 2b of the reference, C2240 4 4 waiting for data from author C2240 4 5 FACILITY (VDGT,1USAORL) Experiment was performed at the C2240 4 6 Holifield Radioactive Ion Beam Facility at Oak Ridge C2240 4 7 National Laboratory. C2240 4 8 DETECTOR (MCPLT,IOCH) The evaporation residues were identified C2240 4 9 by time-of-flight using microchannel-plate timing C2240 4 10 detectors and energy loss using a multi-anode C2240 4 11 ionization chamber. C2240 4 12 SAMPLE Enriched 50Ti self- supporting metallic foil with C2240 4 13 thickness of 270 mu-g/cm2 (ORNL). C2240 4 14 INC-SOURCE 124Sn beam accelerated by the 25 MV tandem C2240 4 15 accelerator to energies near the Coulomb barrier C2240 4 16 ENDBIB 14 0 C2240 4 17 NOCOMMON 0 0 C2240 4 18 DATA 3 11 C2240 4 19 EN-CM DATA DATA-ERR C2240 4 20 MEV MB MB C2240 4 21 123.02 8.55 1.57 C2240 4 22 125.68 33.28 3.38 C2240 4 23 128.48 84.42 C2240 4 24 131.35 138.12 C2240 4 25 134.25 198.73 C2240 4 26 137.15 276.91 C2240 4 27 140.02 308.19 C2240 4 28 142.89 358.00 C2240 4 29 147.23 424.86 C2240 4 30 151.55 462.83 C2240 4 31 155.84 515.11 C2240 4 32 ENDDATA 13 0 C2240 4 33 ENDSUBENT 32 0 C2240 499999 SUBENT C2240005 20160920 C165C2240 5 1 BIB 6 18 C2240 5 2 REACTION ((50-SN-124(22-TI-50,FUS),,SIG,ER)= C2240 5 3 (22-TI-50(50-SN-124,FUS),,SIG,ER)) C2240 5 4 STATUS (CURVE) Data taken from fig. 2b of the reference, C2240 5 5 waiting for data from author C2240 5 6 FACILITY (VDGT,3AULCBR) A follow-up measurement was carried out C2240 5 7 using 14UD tandem electrostatic accelerator at the C2240 5 8 Australian National University. C2240 5 9 DETECTOR (MAGSP) The evaporation residues were transported in C2240 5 10 the superconducting solenoid SOLITAIRE and detected C2240 5 11 at and behind the focus C2240 5 12 (MWPC) The evaporation residues were detected by two C2240 5 13 multiwire proportional counters at and behind the C2240 5 14 focus. C2240 5 15 SAMPLE Enriched 124Sn targets with thickness of 17 mu-g/cm2 C2240 5 16 evaporated onto 20 mu-g/cm2 carbon backings C2240 5 17 were used C2240 5 18 INC-SOURCE 50aTi beam accelerated by the 14UD tandem electrostaticC2240 5 19 accelerator C2240 5 20 ENDBIB 18 0 C2240 5 21 NOCOMMON 0 0 C2240 5 22 DATA 3 4 C2240 5 23 EN-CM DATA DATA-ERR C2240 5 24 MEV MB MB C2240 5 25 118.01 0.04 0.01 C2240 5 26 120.03 0.61 0.00 C2240 5 27 122.02 3.19 0.00 C2240 5 28 124.05 11.29 0.00 C2240 5 29 ENDDATA 6 0 C2240 5 30 ENDSUBENT 29 0 C2240 599999 ENDENTRY 5 0 C224099999999