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