ENTRY D0921 20181220 D119D092100000001 SUBENT D0921001 20181220 D119D092100100001 BIB 14 50 D092100100002 TITLE Fission cross sections as a probe of fusion dynamics D092100100003 at high angular momentum D092100100004 AUTHOR (C.S.Palshetkar, D.J.Hinde, M.Dasgupta, E.Williams, D092100100005 K.Ramachandran, I.P.Carter, K.J.Cook, D.Y.Jeung, D092100100006 D.H.Luong, S.D.McNeil, D.C.Rafferty, A.Wakhle) D092100100007 INSTITUTE (3AULCBR) D092100100008 REFERENCE (J,PR/C,98,044603,2018) D092100100009 #doi:10.1103/PhysRevC.98.044603 D092100100010 REL-REF (M,,D.J.Hinde+,J,PR/C,53,1290,1996) Kinematic D092100100011 coincidence method D092100100012 FACILITY (VDGT,3AULCBR) 14UD electrostatic tandem accelerator D092100100013 at the Heavy Ion Accelerator Facility. D092100100014 INC-SOURCE Pulsed beams of less than 1 ns FWHM D092100100015 SAMPLE The thicknesses of target and 12C backing are D092100100016 Target(ug/cm**2) Backing(ug/cm**2) D092100100017 SM-148 30 40 D092100100018 BA-136 40 12 D092100100019 SN-124 17 12 D092100100020 The target was located 18 cm away from the central D092100100021 cathode foil of each MWPC. D092100100022 DETECTOR (MWPC) The CUBE spectrometer consisting of two large D092100100023 area multiwire proportional counters, each having an D092100100024 active area of 27.9 x 35.7 cm**2 and giving an D092100100025 angular coverage in-plane of 75 degree. D092100100026 MWPC 1: angular coverage of theta1 = 95-170 degree D092100100027 for 40Ca + 124Sn, theta1 = 55-130 degree D092100100028 MWPC 2: angular coverage of theta2 = 5-80 degree D092100100029 (SIBAR) Two silicon surface barrier detectors were D092100100030 placed out of plane, at thetamon = 23 degree and D092100100031 phi1 = 90 degree, phi2 = 270 degree to detect the D092100100032 elastically scattered beam particles that were used D092100100033 for normalization. The solid angle of the detection D092100100034 system was determined by using 28Si+197Au and D092100100035 40Ca+197Au elastic scattering. D092100100036 METHOD (TOF) The emission angle of the detected fission D092100100037 fragments and their velocities. D092100100038 (COINC) Two MWPCs for the detection of binary fission D092100100039 fragments in coincidence. D092100100040 ANALYSIS The cross sections were converted from the lab frame D092100100041 to the CM frame assuming binary fission and by taking D092100100042 the average kinetic energy of the fragments given by D092100100043 the Viola systematics. D092100100044 CORRECTION Fission yields corresponding to 5 degree bins in angle D092100100045 were extracted and were corrected for the detector D092100100046 solid angle to get the differential cross sections for D092100100047 each energy. D092100100048 HISTORY (20181210R) Numerical data of Fig. 3 was received from D092100100049 Dr. C.S.Palshetkar. D092100100050 (20181220C) So NDS D092100100051 STATUS (APRVD) Approved by Dr. Palshetkar on 12. January 2019 D092100100052 ENDBIB 50 0 D092100100053 NOCOMMON 0 0 D092100100054 ENDSUBENT 53 0 D092100199999 SUBENT D0921002 20181220 D119D092100200001 BIB 3 4 D092100200002 REACTION (62-SM-148(8-O-16,F),,DA,FF) D092100200003 ERR-ANALYS (ERR-S) The uncertainties shown on the cross D092100200004 sections are statistical. D092100200005 STATUS (TABLE) Fig. 3 (a) in Phys.Rev.C98,044603(2018) D092100200006 ENDBIB 4 0 D092100200007 NOCOMMON 0 0 D092100200008 DATA 4 46 D092100200009 EN ANG-CM DATA-CM ERR-S D092100200010 MEV ADEG MB/SR MB/SR D092100200011 73.92 112.74 0.00111 0.00078 D092100200012 73.92 117.50 0.00301 0.00123 D092100200013 73.92 122.14 0.00101 0.00072 D092100200014 73.92 126.68 0.00205 0.00103 D092100200015 73.92 131.10 0.00161 0.00093 D092100200016 73.92 135.42 0.00278 0.00124 D092100200017 73.92 139.64 0.00222 0.00111 D092100200018 73.92 143.77 0.00502 0.00167 D092100200019 73.92 147.82 0.00289 0.00129 D092100200020 73.92 151.79 0.00513 0.00182 D092100200021 82.04 113.57 0.02854 0.00344 D092100200022 82.04 118.32 0.03308 0.00353 D092100200023 82.04 122.95 0.03761 0.00379 D092100200024 82.04 127.45 0.03290 0.00357 D092100200025 82.04 131.84 0.02999 0.00349 D092100200026 82.04 136.12 0.03491 0.00384 D092100200027 82.04 140.30 0.03887 0.00406 D092100200028 82.04 144.38 0.03910 0.00408 D092100200029 82.04 148.38 0.03265 0.00380 D092100200030 82.04 152.29 0.04714 0.00482 D092100200031 82.04 156.13 0.05804 0.00591 D092100200032 82.04 159.91 0.06197 0.00699 D092100200033 90.21 114.38 0.25413 0.01943 D092100200034 90.21 119.11 0.22219 0.01734 D092100200035 90.21 123.72 0.26066 0.01892 D092100200036 90.21 128.20 0.26905 0.01943 D092100200037 90.21 132.56 0.30155 0.02109 D092100200038 90.21 136.80 0.29853 0.02140 D092100200039 90.21 140.93 0.28831 0.02111 D092100200040 90.21 144.97 0.35565 0.02356 D092100200041 90.21 148.91 0.33787 0.02342 D092100200042 90.21 152.77 0.44127 0.02830 D092100200043 90.21 156.55 0.49704 0.03320 D092100200044 90.21 160.27 0.52328 0.03903 D092100200045 99.24 115.23 1.70691 0.09162 D092100200046 99.24 119.95 1.60874 0.08506 D092100200047 99.24 124.53 1.70248 0.08829 D092100200048 99.24 128.98 1.93698 0.09547 D092100200049 99.24 133.31 2.03976 0.10058 D092100200050 99.24 137.51 2.02738 0.10241 D092100200051 99.24 141.60 2.37765 0.11169 D092100200052 99.24 145.59 2.71210 0.12020 D092100200053 99.24 149.48 3.02168 0.12979 D092100200054 99.24 153.28 3.14207 0.13987 D092100200055 99.24 157.00 3.60790 0.16588 D092100200056 99.24 160.65 4.25342 0.20677 D092100200057 ENDDATA 48 0 D092100200058 ENDSUBENT 57 0 D092100299999 SUBENT D0921003 20181220 D119D092100300001 BIB 3 4 D092100300002 REACTION (56-BA-136(14-SI-28,F),,DA,FF) D092100300003 ERR-ANALYS (ERR-S) The uncertainties shown on the cross D092100300004 sections are statistical D092100300005 STATUS (TABLE) Fig. 3 (b) in Phys.Rev.C98,044603(2018) D092100300006 ENDBIB 4 0 D092100300007 NOCOMMON 0 0 D092100300008 DATA 4 44 D092100300009 EN ANG-CM DATA-CM ERR-S D092100300010 MEV ADEG MB/SR MB/SR D092100300011 108.22 123.53 0.07135 0.00981 D092100300012 108.22 128.10 0.08125 0.01017 D092100300013 108.22 132.47 0.07456 0.00997 D092100300014 108.22 136.64 0.07598 0.01035 D092100300015 108.22 140.62 0.06108 0.00966 D092100300016 108.22 144.42 0.07710 0.01125 D092100300017 108.22 148.06 0.06980 0.01091 D092100300018 108.22 151.55 0.07770 0.01172 D092100300019 108.22 154.90 0.10562 0.01413 D092100300020 108.22 158.13 0.07967 0.01311 D092100300021 108.22 161.26 0.12347 0.01823 D092100300022 116.38 124.57 2.41445 0.13731 D092100300023 116.38 129.12 2.33033 0.13130 D092100300024 116.38 133.46 2.14002 0.12903 D092100300025 116.38 137.59 2.25468 0.13646 D092100300026 116.38 141.52 2.58230 0.15443 D092100300027 116.38 145.27 3.38301 0.18393 D092100300028 116.38 148.86 3.48322 0.19051 D092100300029 116.38 152.28 3.97651 0.20792 D092100300030 116.38 155.56 4.35175 0.22528 D092100300031 116.38 158.73 4.42137 0.24283 D092100300032 116.38 161.78 4.72689 0.28057 D092100300033 119.07 124.91 4.06028 0.07965 D092100300034 119.07 129.45 4.36834 0.08087 D092100300035 119.07 133.78 4.49924 0.08440 D092100300036 119.07 137.90 4.54018 0.08742 D092100300037 119.07 141.82 4.84091 0.09450 D092100300038 119.07 145.55 5.29519 0.10443 D092100300039 119.07 149.11 5.97147 0.11391 D092100300040 119.07 152.52 6.81984 0.12513 D092100300041 119.07 155.78 7.36244 0.13511 D092100300042 119.07 158.92 7.79497 0.14900 D092100300043 119.07 161.95 8.42399 0.17345 D092100300044 125.42 125.69 12.44580 0.30875 D092100300045 125.42 130.22 12.58450 0.30364 D092100300046 125.42 134.53 13.02050 0.31785 D092100300047 125.42 138.62 13.92690 0.33999 D092100300048 125.42 142.50 15.32190 0.37776 D092100300049 125.42 146.19 15.93700 0.40091 D092100300050 125.42 149.71 17.28200 0.42817 D092100300051 125.42 153.07 18.71690 0.45678 D092100300052 125.42 156.28 19.84430 0.48817 D092100300053 125.42 159.36 21.22200 0.54084 D092100300054 125.42 162.33 23.14470 0.63154 D092100300055 ENDDATA 46 0 D092100300056 ENDSUBENT 55 0 D092100399999 SUBENT D0921004 20181220 D119D092100400001 BIB 3 4 D092100400002 REACTION (50-SN-124(20-CA-40,F),,DA,FF) D092100400003 ERR-ANALYS (ERR-S) The uncertainties shown on the cross D092100400004 sections are statistical D092100400005 STATUS (TABLE) Fig. 3 (c) in Phys.Rev.C98,044603(2018) D092100400006 ENDBIB 4 0 D092100400007 NOCOMMON 0 0 D092100400008 DATA 4 39 D092100400009 EN ANG-CM DATA-CM ERR-S D092100400010 MEV ADEG MB/SR MB/SR D092100400011 126.00 87.78 0.1206 0.0270 D092100400012 126.00 94.52 0.0953 0.0225 D092100400013 126.00 101.02 0.1318 0.0276 D092100400014 126.00 107.26 0.1117 0.0264 D092100400015 126.00 113.21 0.1521 0.0326 D092100400016 126.00 118.85 0.1202 0.0301 D092100400017 126.00 124.17 0.1267 0.0340 D092100400018 126.00 129.17 0.1108 0.0335 D092100400019 126.00 133.85 0.1200 0.0363 D092100400020 126.00 138.21 0.1676 0.0467 D092100400021 130.11 88.32 0.4956 0.0744 D092100400022 130.11 95.10 0.4845 0.0690 D092100400023 130.11 101.64 0.6091 0.0808 D092100400024 130.11 107.90 0.3761 0.0659 D092100400025 130.11 113.87 0.4330 0.0748 D092100400026 130.11 119.53 0.5963 0.0918 D092100400027 130.11 124.86 0.5198 0.0941 D092100400028 130.11 129.86 0.6180 0.1085 D092100400029 130.11 134.53 0.5084 0.1024 D092100400030 130.11 138.87 0.6757 0.1288 D092100400031 139.19 89.50 5.9219 0.3662 D092100400032 139.19 96.37 5.6956 0.3392 D092100400033 139.19 102.98 6.3157 0.3743 D092100400034 139.19 109.31 5.8812 0.3752 D092100400035 139.19 115.34 6.5351 0.4207 D092100400036 139.19 121.03 6.1864 0.4266 D092100400037 139.19 126.38 6.0574 0.4632 D092100400038 139.19 131.38 7.4293 0.5487 D092100400039 139.19 136.03 8.0931 0.6009 D092100400040 144.07 90.12 9.9517 0.7265 D092100400041 144.07 97.04 9.6750 0.6777 D092100400042 144.07 103.70 8.9591 0.6762 D092100400043 144.07 110.06 9.3459 0.7219 D092100400044 144.07 116.11 10.0265 0.7938 D092100400045 144.07 121.83 10.3455 0.8446 D092100400046 144.07 127.19 10.1596 0.9188 D092100400047 144.07 132.19 11.4793 1.0408 D092100400048 144.07 136.83 11.3120 1.0798 D092100400049 144.07 141.11 13.4815 1.2965 D092100400050 ENDDATA 41 0 D092100400051 ENDSUBENT 50 0 D092100499999 SUBENT D0921005 20181220 D119D092100500001 BIB 5 8 D092100500002 REACTION (62-SM-148(8-O-16,F),,SIG) D092100500003 REL-REF (M,,B.B.Back+,J,PR/C,32,195,1985) D092100500004 ANALYSIS (INTAD) The differential cross sections were fitted D092100500005 with transition state model by Back et al. D092100500006 ERR-ANALYS (DATA-ERR) Uncertainty due to parametrization of D092100500007 the angular distribution for extrapolation to 90 D092100500008 and 180 degree. D092100500009 STATUS (TABLE) Table II in Phys.Rev.C98,044603(2018) D092100500010 ENDBIB 8 0 D092100500011 NOCOMMON 0 0 D092100500012 DATA 3 4 D092100500013 EN-CM DATA DATA-ERR D092100500014 MEV MB MB D092100500015 73.92 0.013 0.008 D092100500016 82.04 0.21 0.01 D092100500017 90.21 1.74 0.04 D092100500018 99.24 12.7 0.2 D092100500019 ENDDATA 6 0 D092100500020 ENDSUBENT 19 0 D092100599999 SUBENT D0921006 20181220 D119D092100600001 BIB 5 8 D092100600002 REACTION (56-BA-136(14-SI-28,F),,SIG) D092100600003 REL-REF (M,,B.B.Back+,J,PR/C,32,195,1985) D092100600004 ANALYSIS (INTAD) The differential cross sections were fitted D092100600005 with transition state model by Back et al. D092100600006 ERR-ANALYS (DATA-ERR) Uncertainty due to parametrization of D092100600007 the angular distribution for extrapolation to 90 D092100600008 and 180 degree. D092100600009 STATUS (TABLE) Table II in Phys.Rev.C98,044603(2018) D092100600010 ENDBIB 8 0 D092100600011 NOCOMMON 0 0 D092100600012 DATA 3 4 D092100600013 EN-CM DATA DATA-ERR D092100600014 MEV MB MB D092100600015 108.22 0.38 0.06 D092100600016 116.38 14.9 0.3 D092100600017 119.07 26.8 0.2 D092100600018 125.42 78.5 0.6 D092100600019 ENDDATA 6 0 D092100600020 ENDSUBENT 19 0 D092100699999 SUBENT D0921007 20181220 D119D092100700001 BIB 5 8 D092100700002 REACTION (50-SN-124(20-CA-40,F),,SIG) D092100700003 REL-REF (M,,B.B.Back+,J,PR/C,32,195,1985) D092100700004 ANALYSIS (INTAD) The differential cross sections were fitted D092100700005 with transition state model by Back et al. D092100700006 ERR-ANALYS (DATA-ERR) Uncertainty due to parametrization of D092100700007 the angular distribution for extrapolation to 90 D092100700008 and 180 degree. D092100700009 STATUS (TABLE) Table II in Phys.Rev.C98,044603(2018) D092100700010 ENDBIB 8 0 D092100700011 NOCOMMON 0 0 D092100700012 DATA 3 4 D092100700013 EN-CM DATA DATA-ERR D092100700014 MEV MB MB D092100700015 126.00 0.96 0.29 D092100700016 130.11 4.0 0.7 D092100700017 139.19 50.2 3.5 D092100700018 144.07 77.2 6.4 D092100700019 ENDDATA 6 0 D092100700020 ENDSUBENT 19 0 D092100799999 ENDENTRY 7 0 D092199999999