ENTRY S0069 20210120 S029S006900000001 SUBENT S0069001 20210120 S029S006900100001 BIB 11 52 S006900100002 TITLE Competition between fusion-fission and quasifission S006900100003 processes in the 32S+184W reaction S006900100004 AUTHOR (H.Q.Zhang, C.L.Zhang, C.J.Lin, Z.H.Liu, F.Yang, S006900100005 A.K.Nasirov, G.Mandaglio, M.Manganaro, G.Giardina) S006900100006 INSTITUTE (3CPRAEP,4ZZZDUB,2ITYMES,2ITYCAT) S006900100007 REFERENCE (J,PR/C,81,034611,2010) S006900100008 #doi:10.1103/PhysRevC.81.034611 S006900100009 (J,JP/CS,420,012126,2013) S006900100010 #doi:10.1088/1742-6596/420/1/012126 S006900100011 (J,NP/A,834,201C,2010) S006900100012 #doi:10.1016/j.nuclphysa.2009.12.040 S006900100013 (J,EPJ/CS,17,04002,2011) S006900100014 #doi:10.1051/epjconf/20111704002 S006900100015 Same data in fig (002) and table (008) S006900100016 FACILITY (VDGT,3CPRAEP) Experiment performed at the HI-13 S006900100017 tandem accelerator S006900100018 INC-SOURCE The typical 32S beam current range was 70-90pnA S006900100019 monitored by a shielded suppressed Faraday cup at the S006900100020 periphery of the chamber. The beam energy loss in S006900100021 traveling half the target was calculated and was S006900100022 about 0.5 MeV. S006900100023 SAMPLE 184W target with thickness about 200 ug/cm2 was S006900100024 evaporated on a 20 ug/cm2 thick carbon foil backing. S006900100025 DETECTOR (SI) Array of five Si detectors with a depletion S006900100026 depth ranging from 200 to 300 um covered the angular S006900100027 range of 14-35 degree, 35-55 degree and 55-75 degree S006900100028 was mounted on the movable arm in the vacuum chamber. S006900100029 Five masks were placed in the front of each detector S006900100030 to assure the angular resolution. The detector to the S006900100031 target distance was 27 cm. S006900100032 (SISD) Two groups of Si strip detectors were mounted S006900100033 on opposite sides of the beam. These Si strip S006900100034 detectors were 48 x 50 mm2 in area and each detector S006900100035 consisted of 24 strips. Due to a lack of readout S006900100036 electronics, the strips were tied together in groups S006900100037 of eight. Data from these strip detectors were S006900100038 recorded in the coincidence mode (Si strip and Si S006900100039 detectors) with the requirement that each detector S006900100040 was struck by a fission fragment. S006900100041 (SIBAR) Rutherford scattering was monitored at S006900100042 laboratory forward angle of 15 degree by four Si(Au) S006900100043 surface barrier detectors for the normalization of S006900100044 the cross-section measurements. S006900100045 METHOD (COINC) Coincidence between Si strip and Si detectors S006900100046 was required. S006900100047 ERR-ANALYS (DATA-ERR) No information given S006900100048 HISTORY (20101027C) Compiled by Xi Tao S006900100049 (20161104A) Revised by Xi Tao. Main reference was S006900100050 changed to (J,PR/C,81,034611,2010) . S006900100051 (20161104T) Xi Tao Final numerical data sets in EXFOR S006900100052 C1791 replaced preliminary digitized data sets. S006900100053 (20210120U) The J,EPJ/CS,17,04002,2011 was added. S006900100054 ENDBIB 52 0 S006900100055 NOCOMMON 0 0 S006900100056 ENDSUBENT 55 0 S006900199999 SUBENT S0069002 20210120 S029S006900200001 BIB 3 5 S006900200002 REACTION (74-W-184(16-S-32,F),,DA,FF) S006900200003 STATUS (TABLE) Data presented in Fig.2 of S006900200004 J,PR/C,81,034611,2010 received at CNDC from H.Q.Zhang. S006900200005 HISTORY (20161104A) Xi Tao.002-007 merged to 002, data updated.S006900200006 (20210120U) STAUS: NNDC -> CNDC S006900200007 ENDBIB 5 0 S006900200008 NOCOMMON 0 0 S006900200009 DATA 4 68 S006900200010 EN-CM ANG-CM DATA-CM DATA-ERR S006900200011 MEV ADEG MB/SR MB/SR S006900200012 119.0 20.0 3.39E-02 1.07E-02 S006900200013 119.0 26.6 3.05E-02 7.87E-03 S006900200014 119.0 39.9 3.35E-02 5.58E-03 S006900200015 119.0 46.1 2.89E-02 3.96E-03 S006900200016 119.0 71.6 2.55E-02 7.08E-03 S006900200017 119.0 77.4 3.54E-02 6.58E-03 S006900200018 119.0 83.4 2.26E-02 4.12E-03 S006900200019 119.0 89.1 2.51E-02 3.88E-03 S006900200020 119.0 94.4 2.87E-02 3.23E-03 S006900200021 123.0 20.1 3.41E-01 3.07E-02 S006900200022 123.0 26.7 2.84E-01 2.17E-02 S006900200023 123.0 33.5 2.32E-01 1.33E-02 S006900200024 123.0 40.0 1.93E-01 1.21E-02 S006900200025 123.0 46.7 2.00E-01 1.58E-02 S006900200026 123.0 53.0 1.51E-01 1.18E-02 S006900200027 123.0 65.7 1.37E-01 7.75E-03 S006900200028 123.0 71.9 1.61E-01 7.89E-03 S006900200029 123.0 77.8 1.44E-01 1.50E-02 S006900200030 123.0 83.7 1.13E-01 1.04E-02 S006900200031 123.0 89.4 1.12E-01 9.24E-03 S006900200032 123.0 94.7 1.36E-01 7.94E-03 S006900200033 127.0 20.2 3.31E+00 2.09E-01 S006900200034 127.0 26.8 2.43E+00 1.06E-01 S006900200035 127.0 33.6 2.21E+00 1.17E-01 S006900200036 127.0 40.2 1.50E+00 7.38E-02 S006900200037 127.0 53.2 1.32E+00 1.13E-01 S006900200038 127.0 59.7 1.18E+00 6.87E-02 S006900200039 127.0 65.9 1.31E+00 7.74E-02 S006900200040 127.0 72.0 1.16E+00 6.10E-02 S006900200041 127.0 78.1 1.32E+00 4.33E-02 S006900200042 127.0 84.1 9.74E-01 3.41E-02 S006900200043 127.0 89.8 8.91E-01 2.49E-02 S006900200044 127.0 95.1 8.85E-01 1.93E-02 S006900200045 132.0 20.3 1.24E+01 7.46E-01 S006900200046 132.0 26.9 9.20E+00 4.99E-01 S006900200047 132.0 33.8 7.40E+00 3.45E-01 S006900200048 132.0 47.1 6.58E+00 2.24E-01 S006900200049 132.0 53.4 5.66E+00 1.64E-01 S006900200050 132.0 60.0 6.42E+00 1.29E-01 S006900200051 132.0 66.2 5.47E+00 1.06E-01 S006900200052 132.0 72.5 5.27E+00 1.37E-01 S006900200053 132.0 78.4 4.50E+00 1.15E-01 S006900200054 132.0 84.4 4.72E+00 9.91E-02 S006900200055 132.0 90.1 3.74E+00 6.84E-02 S006900200056 132.0 95.4 4.37E+00 5.75E-02 S006900200057 136.0 20.4 2.23E+01 2.88E-01 S006900200058 136.0 27.0 1.98E+01 2.11E-01 S006900200059 136.0 33.9 1.62E+01 1.46E-01 S006900200060 136.0 40.6 1.46E+01 1.22E-01 S006900200061 136.0 47.3 1.09E+01 1.54E-01 S006900200062 136.0 53.6 1.26E+01 1.46E-01 S006900200063 136.0 60.2 1.08E+01 1.05E-01 S006900200064 136.0 66.5 1.11E+01 9.44E-02 S006900200065 136.0 72.8 1.06E+01 1.38E-01 S006900200066 136.0 84.7 9.02E+00 3.98E-02 S006900200067 136.0 90.5 7.04E+00 5.00E-02 S006900200068 140.0 20.5 3.68E+01 8.01E-01 S006900200069 140.0 27.2 2.71E+01 7.12E-01 S006900200070 140.0 34.1 2.03E+01 4.04E-01 S006900200071 140.0 47.5 1.68E+01 5.72E-01 S006900200072 140.0 53.9 1.54E+01 4.28E-01 S006900200073 140.0 60.5 1.44E+01 3.22E-01 S006900200074 140.0 66.8 1.33E+01 2.75E-01 S006900200075 140.0 73.0 1.33E+01 3.01E-01 S006900200076 140.0 79.0 1.22E+01 2.07E-01 S006900200077 140.0 85.1 1.11E+01 1.55E-01 S006900200078 140.0 90.8 1.14E+01 1.40E-01 S006900200079 140.0 96.1 1.20E+01 1.12E-01 S006900200080 ENDDATA 70 0 S006900200081 ENDSUBENT 80 0 S006900299999 NOSUBENT S0069003 20161104 S021S006900300001 NOSUBENT S0069004 20161104 S021S006900400001 NOSUBENT S0069005 20161104 S021S006900500001 NOSUBENT S0069006 20161104 S021S006900600001 NOSUBENT S0069007 20161104 S021S006900700001 SUBENT S0069008 20210120 S029S006900800001 BIB 5 8 S006900800002 REACTION (74-W-184(16-S-32,F),,SIG) S006900800003 ANALYSIS (INTAD) S006900800004 STATUS (TABLE) Data presented in Fig.5 of S006900800005 J,PR/C,81,034611,2010 received at CNDC from H.Q.Zhang. S006900800006 (DEP,S0069002) Angular differential cross sections. S006900800007 MISC-COL (MISC) Excitation energy of compound nucleus S006900800008 HISTORY (20161104A) Xi Tao. Data updated. S006900800009 (20210120U) STAUS: NNDC -> CNDC S006900800010 ENDBIB 8 0 S006900800011 NOCOMMON 0 0 S006900800012 DATA 4 7 S006900800013 EN-CM DATA DATA-ERR MISC S006900800014 MEV MB MB MEV S006900800015 118.8 0.04 0.0482 37.2 S006900800016 123.1 2.35 0.71 41.5 S006900800017 127.3 22.97 6.3 45.8 S006900800018 131.5 81.01 18.2 50.0 S006900800019 135.8 132.27 20.5 54.3 S006900800020 141.1 189.33 32.6 58.5 S006900800021 144.4 237.06 53.0 61.8 S006900800022 ENDDATA 9 0 S006900800023 ENDSUBENT 22 0 S006900899999 ENDENTRY 8 0 S006999999999