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| /*===================================================================*/
/* NRDF D0110 Data No.4 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,4;
D#=D110;
TITLE=/ Effect of inelastic scattering processes on (p,t) reactions
exciting the first 2+ states in Te, Sn and Cd isotopes /;
ATH=(K.YAGI'1', Y.AOKI'1', C.RANGACHARYULU'1', K.MATOBA'2',
M.HYAKUTAKE'2', J.NIDOME'2');
INST-ATH=(2JPNOSA'1', 2JPNKYU'2');
/* '1' Department of Physics, Faculty of Science */
/* '2' Department of Nuclear Engineering */
REF=PL/B;
VLP=44(1973)447;
RCTS=(122TE(P,T)120TE, 124TE(P,T)122TE, 126TE(P,T)124TE,
128TE(P,T)126TE, 130TE(P,T)128TE, 118SN(P,T)116SN,
116SN(P,T)114SN, 116CD(P,T)114CD, 114CD(P,T)112CD);
PHQS=ANGL-DSTRN;
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,4;
/* 2009-08-28 : Compiled+Checked, Nh */
/* Related references
- R.B.Firestone et al., FIRESTONE, (1996).
(Level energies of 1st 2+ states are not given in K.Yagi et al.
J,PL/B,44,447,1973, and taken from this book by compiler.)
PHQ=ANGL-DSTRN;
CHM=ELM;
PHYS-FORM=SLD;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=SYNCYC;
INST-ACC=2JPNINS;
INC-ENGY-LAB-RANGE=52MEV;
POL-PRJ=0%;
DET-PARTCL=T;
COINC=NO;
ANT-COINC=NO;
DET-SYS=MAG;
ERS-DET=80KEV;
ANL=(CCBA,DWBA);
RCT=128TE(P,T)126TE;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,4;
INC-ENGY-LAB=52MEV;
SYS-ERR=15%'3';
/* '3' Uncertainty in absolute cross sections */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA FLAG'7'
(KEV) (DEG) (UB/SR) (UB/SR) (NODIM)
0.0 5.250E+00 3.381E+02 +-NEGLIGIBLE 7.
0.0 6.096E+00 3.298E+02 +-NEGLIGIBLE 7.
0.0 6.948E+00 2.636E+02 +-NEGLIGIBLE 7.
0.0 9.481E+00 2.599E+02 +-2.553E+01 7.
0.0 1.186E+01 2.883E+02 +-2.288E+01 7.
0.0 1.452E+01 3.439E+02 +-NEGLIGIBLE 7.
0.0 1.705E+01 3.070E+02 +-NEGLIGIBLE 7.
0.0 1.945E+01 2.161E+02 +-NEGLIGIBLE 7.
0.0 2.253E+01 9.159E+01 +-5.533E+00 7.
0.0 2.528E+01 2.158E+01 +-2.263E+00 7.
0.0 2.782E+01 1.523E+01 +-1.597E+00 7.
0.0 3.043E+01 4.785E+01 +-3.341E+00 7.
0.0 3.280E+01 7.164E+01 +-7.700E+00 7.
0.0 3.547E+01 6.463E+01 +-5.130E+00 7.
0.0 3.801E+01 3.371E+01 +-3.055E+00 7.
0.0 4.068E+01 1.077E+01 +-1.129E+00 7.
0.0 4.324E+01 7.935E+00 +-8.526E-01 7.
0.0 4.561E+01 1.387E+01 +-1.491E+00 7.
0.0 4.810E+01 2.139E+01 +-1.950E+00 7.
0.0 5.051E+01 2.165E+01 +-1.923E+00 7.
0.0 5.318E+01 1.933E+01 +-1.718E+00 7.
0.0 5.601E+01 8.635E+00 +-8.479E-01 7.
0.0 5.856E+01 3.269E+00 +-4.944E-01 7.
666.338 5.142E+00 1.143E+02 +-8.629E+00 8.
666.338 6.357E+00 1.054E+02 +-7.973E+00 8.
666.338 7.365E+00 1.293E+02 +-1.038E+01 8.
666.338 9.971E+00 1.292E+02 +-9.668E+00 8.
666.338 1.276E+01 9.179E+01 +-5.985E+00 8.
666.338 1.548E+01 6.103E+01 +-5.240E+00 8.
666.338 1.775E+01 5.507E+01 +-4.730E+00 8.
666.338 2.050E+01 4.911E+01 +-4.715E+00 8.
666.338 2.308E+01 4.584E+01 +-3.935E+00 8.
666.338 2.581E+01 3.530E+01 +-2.764E+00 8.
666.338 2.822E+01 2.374E+01 +-2.151E+00 8.
666.338 3.077E+01 1.502E+01 +-1.369E+00 8.
666.338 3.316E+01 7.740E+00 +-9.726E-01 8.
666.338 3.578E+01 1.049E+01 +-1.111E+00 8.
666.338 3.838E+01 1.071E+01 +-1.000E+00 8.
666.338 4.098E+01 1.057E+01 +-1.107E+00 8.
666.338 4.360E+01 1.028E+01 +-1.046E+00 8.
666.338 4.608E+01 3.773E+00 +-8.489E-01 8.
666.338 4.867E+01 3.521E+00 +-5.386E-01 8.
666.338 5.117E+01 4.358E+00 +-4.981E-01 8.
666.338 5.359E+01 4.553E+00 +-4.825E-01 8.
666.338 5.624E+01 5.021E+00 +-5.641E-01 8.
666.338 5.884E+01 4.665E+00 +-5.242E-01 8.
\END;
/*===================================================================*/
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