|
| /*===================================================================*/
/* NRDF D1677 Data No.9 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,9;
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,9;
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,9;
INC-ENGY-LAB=18.5MEV;
EMT=P;
RSD=28SI;
STATIST-ERR=<5%;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC ANALPW DELTA-ANALPW
(DEG) (NODIM) (NODIM)
3.599E+01 -4.816E-01 +2.318E-02-2.985E-02
4.035E+01 -8.022E-01 +1.315E-02-2.306E-02
4.503E+01 5.162E-01 +1.321E-02-1.645E-02
5.022E+01 2.094E-01 +0.000E+00-0.000E+00
5.618E+01 4.520E-02 +0.000E+00-0.000E+00
6.229E+01 -8.252E-02 +0.000E+00-0.000E+00
6.716E+01 -2.442E-01 +0.000E+00-0.000E+00
7.178E+01 -4.027E-01 +0.000E+00-0.000E+00
7.646E+01 -5.315E-01 +1.658E-02-1.321E-02
8.095E+01 -5.943E-01 +2.667E-02-1.988E-02
8.616E+01 -4.154E-01 +2.642E-02-1.327E-02
9.207E+01 7.459E-02 +0.000E+00-0.000E+00
9.745E+01 4.188E-01 +1.321E-02-1.645E-02
1.021E+02 6.469E-01 +1.988E-02-1.994E-02
1.067E+02 6.866E-01 +1.988E-02-1.321E-02
1.113E+02 6.271E-01 +9.909E-03-1.976E-02
1.160E+02 4.422E-01 +0.000E+00-0.000E+00
1.224E+02 1.858E-01 +0.000E+00-0.000E+00
1.273E+02 -8.814E-02 +0.000E+00-0.000E+00
1.324E+02 -2.397E-01 +0.000E+00-0.000E+00
1.371E+02 -2.330E-01 +0.000E+00-0.000E+00
1.460E+02 7.087E-02 +0.000E+00-0.000E+00
1.509E+02 3.255E-01 +1.321E-02-9.909E-03
1.562E+02 5.706E-01 +1.976E-02-2.636E-02
1.625E+02 8.461E-01 +2.300E-02-2.312E-02
1.675E+02 9.356E-01 +2.636E-02-1.982E-02
1.717E+02 8.395E-01 +2.318E-02-3.627E-02
\END;
/*===================================================================*/
|