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| /*===================================================================*/
/* NRDF D1677 Data No.22 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,22;
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,22;
RCT=40CA(P,P)40CA;
RTY=(ELA-SCATT);
ENR=NAT;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=1.5MG/CM**2;
ACC=(VDGT);
INC-ENGY-LAB=(12.5MEV,14.5MEV,15.4MEV,16.5MEV,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,22;
INC-ENGY-LAB=18.5MEV;
EMT=P;
RSD=40CA;
STATIST-ERR=<5%;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC ANALPW DELTA-ANALPW
(DEG) (NODIM) (NODIM)
2.377E+01 -1.194E-01 +2.272E-02-1.617E-02
2.873E+01 -2.718E-02 +0.000E+00-0.000E+00
3.524E+01 3.901E-01 +2.272E-02-2.587E-02
3.980E+01 4.463E-01 +1.294E-02-1.940E-02
4.463E+01 1.047E-01 +0.000E+00-0.000E+00
4.943E+01 -7.828E-02 +0.000E+00-0.000E+00
5.378E+01 -2.067E-01 +6.306E-03-6.468E-03
5.941E+01 -3.728E-01 +1.949E-02-1.617E-02
6.586E+01 -5.154E-01 +1.949E-02-2.579E-02
7.050E+01 -6.986E-01 +2.595E-02-4.196E-02
7.597E+01 -7.580E-01 +3.549E-02-2.587E-02
7.970E+01 -1.816E-01 +6.387E-03-1.932E-02
8.187E+01 8.589E-02 +0.000E+00-0.000E+00
8.489E+01 2.021E-01 +0.000E+00-0.000E+00
8.969E+01 1.485E-01 +0.000E+00-8.117E-05
9.309E+01 6.119E-02 +0.000E+00-0.000E+00
9.682E+01 -1.609E-02 +0.000E+00-0.000E+00
1.016E+02 -1.150E-01 +0.000E+00-0.000E+00
1.065E+02 -2.170E-01 +1.294E-02-2.571E-02
1.109E+02 -3.066E-01 +2.579E-02-4.519E-02
1.155E+02 -3.701E-01 +9.621E-03-1.617E-02
1.200E+02 -3.690E-01 +2.612E-02-6.468E-03
1.258E+02 -3.665E-01 +2.911E-02-1.617E-02
1.324E+02 -4.281E-01 +4.180E-02-1.302E-02
1.370E+02 -6.243E-01 +4.875E-02-3.234E-02
1.379E+02 -6.040E-01 +2.927E-02-3.566E-02
1.424E+02 -7.485E-01 +5.490E-02-5.837E-02
1.460E+02 -4.570E-01 +4.212E-02-4.520E-02
1.507E+02 3.295E-02 +0.000E+00-0.000E+00
1.566E+02 4.820E-01 +3.242E-02-2.595E-02
1.621E+02 8.692E-01 +3.590E-02-7.463E-02
1.675E+02 9.424E-01 +5.174E-02-6.791E-02
1.724E+02 7.627E-01 +3.574E-02-2.911E-02
\END;
/*===================================================================*/
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