|
| /*===================================================================*/
/* NRDF D1495 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
D#=D1495;
TITLE=/ Large-angle scattering of 3He particles by 58Ni /;
PURPOSE=/ To obtain better optical model parameters and to estimate
the strength of the spin-orbit interaction for 3He particles
ATH=(H.KAMITSUBO'1', T.WADA'1', T.FUJISAWA'1', M.IGARASHI'1');
INST-ATH=(2JPNIPC'1');
REF=PL/B;
VLP=28(1969)408;
RCTS=58NI(3HE,3HE)58NI;
PHQS=(ANGL-DSTRN, OPT-POTL-PARA);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,1;
/* 2005-11-24 : Converted, C.Kurokawa + N.Otuka. Converted to
EXFOR E1495 */
RTY=ELA-SCATT;
ENR=99.9%;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=0.65MG/CM**2;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=CYC;
INST-ACC=2JPNIPC;
INC-ENGY-LAB-RANGE=34.14MEV;
POL-PRJ=0%;
DET-PARTCL=3HE;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(CNTR-TLSCP'2',SBD'2');
/* '2' To detect scattered particles */
ANL=OPT-MODEL'3';
/* '3' DWBA */
/* 2005-12-22 : Altered, At. Re-digitized */
RCT=58NI(3HE,3HE)58NI;
PHQ=ANGL-DSTRN;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,1;
INC-ENGY-LAB=34.14MEV;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC RUTH-RATIO DELTA-RUTH-RATIO'4'
(DEG) (NODIM) (NODIM)
1.238E+01 6.736E-01 +-NEGLIGIBLE
1.499E+01 5.605E-01 +-NEGLIGIBLE
1.761E+01 4.898E-01 +-NEGLIGIBLE
1.992E+01 3.946E-01 +-NEGLIGIBLE
2.284E+01 3.504E-01 +-NEGLIGIBLE
2.567E+01 2.279E-01 +-NEGLIGIBLE
2.826E+01 1.747E-01 +-NEGLIGIBLE
3.122E+01 1.740E-01 +-NEGLIGIBLE
3.244E+01 1.949E-01 +-NEGLIGIBLE
3.508E+01 1.789E-01 +-NEGLIGIBLE
3.764E+01 1.263E-01 +-NEGLIGIBLE
4.046E+01 7.951E-02 +-NEGLIGIBLE
4.277E+01 6.510E-02 +-NEGLIGIBLE
4.549E+01 7.898E-02 +-NEGLIGIBLE
4.818E+01 8.543E-02 +-NEGLIGIBLE
5.079E+01 7.108E-02 +-NEGLIGIBLE
5.273E+01 4.553E-02 +-NEGLIGIBLE
5.586E+01 2.960E-02 +-NEGLIGIBLE
5.821E+01 2.718E-02 +-NEGLIGIBLE
6.149E+01 2.938E-02 +-NEGLIGIBLE
6.381E+01 2.527E-02 +-NEGLIGIBLE
6.637E+01 1.784E-02 +-NEGLIGIBLE
6.867E+01 1.414E-02 +-NEGLIGIBLE
7.162E+01 1.363E-02 +-NEGLIGIBLE
7.459E+01 1.380E-02 +-NEGLIGIBLE
7.632E+01 1.208E-02 +-NEGLIGIBLE
7.915E+01 7.726E-03 +-NEGLIGIBLE
8.250E+01 3.862E-03 +-NEGLIGIBLE
8.476E+01 2.728E-03 +-NEGLIGIBLE
8.697E+01 4.307E-03 +-NEGLIGIBLE
8.976E+01 6.573E-03 +-NEGLIGIBLE
9.274E+01 6.992E-03 +-NEGLIGIBLE
9.444E+01 5.454E-03 +-NEGLIGIBLE
9.730E+01 3.850E-03 +-NEGLIGIBLE
1.001E+02 1.602E-03 +-NEGLIGIBLE
1.027E+02 5.574E-04 +-8.664E-05
1.048E+02 7.271E-04 +-9.348E-05
1.071E+02 1.847E-03 +-NEGLIGIBLE
1.102E+02 2.203E-03 +-NEGLIGIBLE
1.128E+02 1.863E-03 +-NEGLIGIBLE
1.148E+02 1.501E-03 +-1.896E-04
1.165E+02 1.251E-03 +-NEGLIGIBLE
1.179E+02 9.922E-04 +-1.316E-04
1.204E+02 5.605E-04 +-7.786E-05
1.229E+02 3.325E-04 +-9.260E-05
1.282E+02 4.803E-04 +-8.291E-05
1.326E+02 5.059E-04 +-1.045E-04
1.376E+02 4.479E-04 +-8.475E-05
1.423E+02 4.715E-04 +-9.757E-05
1.470E+02 5.413E-04 +-1.404E-04
1.520E+02 3.724E-04 +-9.336E-05
1.568E+02 2.050E-04 +-5.490E-05
1.616E+02 7.739E-05 +-3.293E-05
1.666E+02 2.126E-04 +-5.163E-05
1.713E+02 5.124E-04 +-1.203E-04
\END;
/*===================================================================*/
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