ENTRY D6188 20131124 D091D618800000001 SUBENT D6188001 20131124 D091D618800100001 BIB 12 32 D618800100002 TITLE Systematic study of projectile-structure effect on D618800100003 the fusion-barrier distribution D618800100004 AUTHOR (Pratap Roy, A.Saxena, B.K.Nayak, E.T.Mirgule, B.John, D618800100005 Y.K.Gupta, L.S.Danu, R.P.Vind, Ashok Kumar, D618800100006 R.K.Choudhury) D618800100007 INSTITUTE (3INDTRM) D618800100008 (3INDIND) Shobhit University, Meerut D618800100009 REFERENCE (J,PR/C,84,011602,2011) D618800100010 FACILITY (VDGT,3INDTRM)14 UD BARC-TIFR Pelletron accelerator D618800100011 SAMPLE A self-supporting 232Th target (~2 mg/cm2) D618800100012 DETECTOR (TELES,SIBAR,SIBAR) A dE(50 um)-E(150 um) silicon D618800100013 surface barrier detector telescope mounted at an D618800100014 angle of 160 deg to the beam direction to detect D618800100015 the outgoing particles D618800100016 (SIBAR) Silicon surface barrier detector at 20 deg. D618800100017 with respect to the beam direction to measure D618800100018 Rutherford scattering events for normalization D618800100019 METHOD (EDE) D618800100020 COMMENT By authors: Contribution of evaporation alpha coming D618800100021 from 4He + 232Th is found to be negligible from PACE2 D618800100022 calculation D618800100023 ERR-ANALYS Major source of uncertainty in the data was D618800100024 statistical, specially at higher energies where the D618800100025 quasi elastic cross section is less. D618800100026 At the highest energy the statistical uncertainty was D618800100027 less than 5%. D618800100028 Any other systematic uncertainty was found to be D618800100029 insignificant. D618800100030 STATUS (APRVD) Approved by Pratap Roy D618800100031 HISTORY (20130221C) Compiled by B.Jyrwa,S.Badwar,NEHU,Shillong,D618800100032 Meghalaya, India D618800100033 (20131124U) On. Finalized D618800100034 ENDBIB 32 0 D618800100035 NOCOMMON 0 0 D618800100036 ENDSUBENT 35 0 D618800199999 SUBENT D6188002 20131124 D091D618800200001 BIB 2 5 D618800200002 REACTION (90-TH-232(A,SCT)90-TH-232,,DA,,RTH) D618800200003 Quasi-elastic scattering was defined as the sum of D618800200004 elastic plus inelastic events. D618800200005 STATUS (CURVE) Fig.2 of Phys.Rev.C84(2011)011602 D618800200006 (UNOBT) From author: Tabulated data were lost. D618800200007 ENDBIB 5 0 D618800200008 COMMON 1 3 D618800200009 ANG D618800200010 ADEG D618800200011 160. D618800200012 ENDCOMMON 3 0 D618800200013 DATA 2 15 D618800200014 EN-CM DATA D618800200015 MEV NO-DIM D618800200016 15.72 1.00E+00 D618800200017 16.71 1.00E+00 D618800200018 17.70 1.01E+00 D618800200019 18.68 1.00E+00 D618800200020 19.66 9.52E-01 D618800200021 20.64 8.72E-01 D618800200022 21.63 6.71E-01 D618800200023 22.61 4.70E-01 D618800200024 23.59 2.99E-01 D618800200025 24.57 2.07E-01 D618800200026 25.56 9.52E-02 D618800200027 26.54 6.18E-02 D618800200028 27.53 3.40E-02 D618800200029 28.51 1.78E-02 D618800200030 29.49 1.24E-02 D618800200031 ENDDATA 17 0 D618800200032 ENDSUBENT 31 0 D618800299999 ENDENTRY 2 0 D618899999999