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