|
| /*===================================================================*/
/* NRDF D1672 Data No.4 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,4;
D#=D1672;
TITLE=/ANALYSING POWERS OF P+D SCATTERING BELOW THE DEUTERON BREAKUP
THRESHOLD/;
ATH=(S.SHIMIZU'1',K.SAGARA'1',H.NAKAMURA'1',K.MAEDA'1',T.MIWA'1',
N.NISHIMORI'1',S.UENO'1',T.NAKASHIMA'1',S.MORINOBU'1');
INST-ATH=(2JPNKYU'1');
REF=PR/C;
VLP=52(1995)1193;
RCTS=(D(P,P)X,P(D,D)X);
PHQS=(ANALPW,TNSR-ANALPW,ANGL-DSTRN,
DATA1'41',DATA2'42',DATA3'43',DATA4'44');
/*@41@*/
/*@42@*/
/*@43@*/
/*@44@*/
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,4;
RCT=D(P,P)X;
RTY=(POL-RCT);
ENR=NAT;
CHM=ELM;
PHYS-FORM=GAS;
THK-TGT=0.27ATM;
BAC=SELF;
POL-TGT=X%'22';
/*@22@*/
ACC=(VDGT);
INST-ACC=2JPNKYU;
INC-ENGY-LAB=(2,2.5,3,4,5,6MEV);
DET-PARTCL=(P);
COINC=NO;
ANT-COINC=NO;
DET-SYS=(SSD);
SOLID-ANGL=XMSR;
ERS-DET=XKEV;
MONTR-RCT=/@THE POLARIZATION OF THE BEAM WAS MEASURED THROUGHOUT THE
EXPERIMENT BY A P+4HE POLAEIMETER PLACED AT THE DOWNSTREAM
WND OF THE SCATTERING CHAMBER.@/;
ANL=X'45';
/*@45@*/
PHQ=(ANGL-DSTRN,THTC);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,4;
INC-ENGY-LAB=4MEV;
EMT-1=P;
RSD=X;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (MB/SR) (MB/SR)
2.292E+01 2.517E+02 +0.000E+00-0.000E+00
2.588E+01 2.306E+02 +0.000E+00-0.000E+00
2.926E+01 2.181E+02 +0.000E+00-0.000E+00
3.241E+01 2.097E+02 +0.000E+00-0.000E+00
3.507E+01 2.048E+02 +0.000E+00-0.000E+00
3.774E+01 1.976E+02 +0.000E+00-0.000E+00
3.976E+01 1.927E+02 +0.000E+00-0.000E+00
4.234E+01 1.853E+02 +0.000E+00-0.000E+00
4.581E+01 1.790E+02 +0.000E+00-0.000E+00
4.872E+01 1.711E+02 +0.000E+00-0.000E+00
5.187E+01 1.667E+02 +0.000E+00-0.000E+00
5.592E+01 1.616E+02 +0.000E+00-0.000E+00
5.801E+01 1.552E+02 +0.000E+00-0.000E+00
6.189E+01 1.485E+02 +0.000E+00-0.000E+00
6.439E+01 1.419E+02 +0.000E+00-0.000E+00
6.657E+01 1.380E+02 +0.000E+00-0.000E+00
6.891E+01 1.300E+02 +0.000E+00-0.000E+00
7.093E+01 1.253E+02 +0.000E+00-0.000E+00
7.351E+01 1.160E+02 +0.000E+00-0.000E+00
7.803E+01 1.064E+02 +0.000E+00-0.000E+00
8.239E+01 9.808E+01 +0.000E+00-0.000E+00
8.773E+01 9.079E+01 +0.000E+00-0.000E+00
9.121E+01 8.392E+01 +0.000E+00-0.000E+00
9.615E+01 8.025E+01 +0.000E+00-0.000E+00
9.971E+01 7.660E+01 +0.000E+00-0.000E+00
1.031E+02 7.335E+01 +0.000E+00-0.000E+00
1.065E+02 7.230E+01 +0.000E+00-0.000E+00
1.111E+02 7.245E+01 +0.000E+00-0.000E+00
1.152E+02 7.663E+01 +0.000E+00-0.000E+00
1.202E+02 7.938E+01 +0.000E+00-0.000E+00
1.240E+02 8.817E+01 +0.000E+00-0.000E+00
1.280E+02 9.978E+01 +0.000E+00-0.000E+00
1.319E+02 1.132E+02 +0.000E+00-0.000E+00
1.352E+02 1.292E+02 +0.000E+00-0.000E+00
1.390E+02 1.515E+02 +0.000E+00-0.000E+00
1.431E+02 1.705E+02 +0.000E+00-0.000E+00
1.468E+02 1.933E+02 +0.000E+00-0.000E+00
\END;
/*===================================================================*/
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