|
| /*===================================================================*/
/* NRDF D1672 Data No.3 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,3;
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,3;
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,3;
INC-ENGY-LAB=3MEV;
EMT-1=P;
RSD=X;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (MB/SR) (MB/SR)
2.275E+01 3.116E+02 +0.000E+00-0.000E+00
2.509E+01 2.684E+02 +0.000E+00-0.000E+00
2.921E+01 2.445E+02 +0.000E+00-0.000E+00
3.215E+01 2.288E+02 +0.000E+00-0.000E+00
3.486E+01 2.180E+02 +0.000E+00-0.000E+00
3.760E+01 2.110E+02 +0.000E+00-0.000E+00
3.983E+01 2.024E+02 +0.000E+00-0.000E+00
4.249E+01 1.958E+02 +0.000E+00-0.000E+00
4.505E+01 1.878E+02 +0.000E+00-0.000E+00
4.819E+01 1.792E+02 +0.000E+00-0.000E+00
5.093E+01 1.740E+02 +0.000E+00-0.000E+00
5.447E+01 1.668E+02 +0.000E+00-0.000E+00
5.745E+01 1.596E+02 +0.000E+00-0.000E+00
6.026E+01 1.522E+02 +0.000E+00-0.000E+00
6.324E+01 1.458E+02 +0.000E+00-0.000E+00
6.638E+01 1.401E+02 +0.000E+00-0.000E+00
6.896E+01 1.351E+02 +0.000E+00-0.000E+00
7.113E+01 1.302E+02 +0.000E+00-0.000E+00
7.329E+01 1.224E+02 +0.000E+00-0.000E+00
7.804E+01 1.115E+02 +0.000E+00-0.000E+00
8.150E+01 1.033E+02 +0.000E+00-0.000E+00
8.578E+01 9.645E+01 +0.000E+00-0.000E+00
9.038E+01 9.043E+01 +0.000E+00-0.000E+00
9.452E+01 8.869E+01 +0.000E+00-0.000E+00
9.930E+01 8.592E+01 +0.000E+00-0.000E+00
1.029E+02 8.623E+01 +0.000E+00-0.000E+00
1.065E+02 8.674E+01 +0.000E+00-0.000E+00
1.100E+02 8.807E+01 +0.000E+00-0.000E+00
1.138E+02 9.488E+01 +0.000E+00-0.000E+00
1.178E+02 1.025E+02 +0.000E+00-0.000E+00
1.231E+02 1.133E+02 +0.000E+00-0.000E+00
1.277E+02 1.295E+02 +0.000E+00-0.000E+00
1.313E+02 1.454E+02 +0.000E+00-0.000E+00
1.356E+02 1.628E+02 +0.000E+00-0.000E+00
1.389E+02 1.853E+02 +0.000E+00-0.000E+00
1.424E+02 2.102E+02 +0.000E+00-0.000E+00
1.463E+02 2.314E+02 +0.000E+00-0.000E+00
\END;
/*===================================================================*/
|