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| /*===================================================================*/
/* NRDF D1677 Data No.13 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,13;
D#=D1677;
TITLE=/A NEW APPROACH TO A 'MODEL-INDEPENDENT' OPTICAL POTENTIAL AND
ITS APPLICATION TO PROTON ELASTIC SCATTERING NEAR THE (P,N)
THRESHOLD ENERGY REGION/;
PURPOSE=/A NEW APPROACH TO A "MODEL INDEPENDENT" OPTICAL POTENTIAL IS
PROPOSED, WHICH FEATURES THE ADAPTIVE IMPROVEMENT OF EXPANSION
BASE AND PRACTICAL ESTIMATION OF THE ERRORS OF TEH DERIVED
POTENTIAL/;
ATH=(Y.AOKI'1',K.HIROTA'1',H.KISHITA'1',K.KOYAMA'1',M.MASAKI'1',
K.MIURA'1',Y.MUKOUHARA'1',S.NAKAGAWA'1',N.OKUMURA'1',
Y.TAGISHI'1');
INST-ATH=(2JPNTSU'1');
REF=NP/A;
VLP=599(1996)417;
RCTS=(28SI(P,P)28SI,40CA(P,P)40)CA;
PHQS=(ANALPW,DSIGMA/DOMEGA-RATIO);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,13;
RCT=28SI(P,P)28SI;
RTY=(ELA-SCATT);
ENR=NAT;
CHM=SI02;
PHYS-FORM=SLD;
THK-TGT=XMG/CM**2;
ACC=(VDGT);
INC-ENGY-LAB=(12.5MEV,14.5MEV,15.5MEV,16.5MEV,17.5MEV,18.5MEV,20.5MEV);
DELTA-INC-ENGY-LAB=800KEV;
CHRG-INC-ION=1;
DET-PARTCL=(P);
COINC=NO;
ANT-COINC=NO;
/*@12@*/
SOLID-ANGL=1.1[1.4MSR;
ERS-DET=80KEV;
ANL=(OPT-MODEL);
PHQ=(ANALPW, DSIGMA/DOMEGA-RATIO);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,13;
INC-ENGY-LAB=14.5MEV;
EMT=P;
RSD=28SI;
STATIST-ERR=<5%;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC ANALPW DELTA-ANALPW
(DEG) (NODIM) (NODIM)
3.030E+01 -8.667E-02 +0.000E+00-0.000E+00
3.592E+01 -4.027E-02 +0.000E+00-0.000E+00
4.082E+01 9.387E-02 +0.000E+00-0.000E+00
4.321E+01 3.864E-01 +6.593E-03-9.860E-03
4.519E+01 6.688E-01 +2.293E-02-3.279E-02
5.006E+01 6.853E-01 +1.319E-02-1.960E-02
5.270E+01 4.355E-01 +1.960E-02-1.319E-02
5.489E+01 2.540E-01 +1.313E-02-1.295E-02
6.089E+01 2.289E-02 +0.000E+00-0.000E+00
6.693E+01 -1.036E-01 +0.000E+00-0.000E+00
7.195E+01 -2.341E-01 +0.000E+00-0.000E+00
7.680E+01 -3.517E-01 +0.000E+00-0.000E+00
8.106E+01 -4.500E-01 +2.952E-02-1.307E-02
8.580E+01 -6.820E-01 +1.960E-02-9.801E-03
9.126E+01 -8.449E-01 +6.534E-03-2.929E-02
9.733E+01 -8.635E-01 +1.972E-02-1.972E-02
1.027E+02 -2.225E-01 +0.000E+00-0.000E+00
1.077E+02 6.568E-01 +1.639E-02-2.952E-02
1.117E+02 9.178E-01 +3.932E-02-3.279E-02
1.165E+02 8.591E-01 +2.281E-02-6.190E-02
1.219E+02 7.125E-01 +1.960E-02-2.305E-02
1.270E+02 5.919E-01 +1.663E-02-6.534E-03
1.327E+02 5.566E-01 +1.628E-02-1.634E-02
1.378E+02 5.112E-01 +6.593E-03-2.287E-02
1.424E+02 5.634E-01 +6.651E-03-1.622E-02
1.464E+02 7.231E-01 +1.639E-02-1.634E-02
1.512E+02 8.473E-01 +2.614E-02-3.932E-02
1.555E+02 6.837E-01 +3.932E-02-2.625E-02
1.617E+02 5.409E-01 +1.639E-02-3.261E-02
1.667E+02 3.843E-01 +1.301E-02-3.267E-03
1.720E+02 2.539E-01 +0.000E+00-0.000E+00
\END;
/*===================================================================*/
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