|
| /*===================================================================*/
/* NRDF D1672 Data No.2 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,2;
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,2;
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,2;
INC-ENGY-LAB=2MEV;
EMT-1=P;
RSD=X;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (MB/SR) (MB/SR)
2.567E+01 3.939E+02 +3.469E+00-2.439E+00
2.913E+01 3.181E+02 +0.000E+00-0.000E+00
3.229E+01 2.793E+02 +0.000E+00-0.000E+00
3.491E+01 2.520E+02 +0.000E+00-0.000E+00
3.689E+01 2.324E+02 +0.000E+00-0.000E+00
4.012E+01 2.205E+02 +0.000E+00-0.000E+00
4.262E+01 2.091E+02 +0.000E+00-0.000E+00
4.512E+01 1.995E+02 +0.000E+00-0.000E+00
4.764E+01 1.933E+02 +0.000E+00-0.000E+00
5.096E+01 1.847E+02 +0.000E+00-0.000E+00
5.452E+01 1.771E+02 +0.000E+00-0.000E+00
5.711E+01 1.687E+02 +0.000E+00-0.000E+00
6.027E+01 1.617E+02 +0.000E+00-0.000E+00
6.303E+01 1.568E+02 +0.000E+00-0.000E+00
6.628E+01 1.509E+02 +0.000E+00-0.000E+00
6.921E+01 1.482E+02 +0.000E+00-0.000E+00
7.123E+01 1.430E+02 +0.000E+00-0.000E+00
7.318E+01 1.385E+02 +0.000E+00-0.000E+00
7.765E+01 1.327E+02 +0.000E+00-0.000E+00
8.187E+01 1.270E+02 +0.000E+00-0.000E+00
8.619E+01 1.234E+02 +0.000E+00-0.000E+00
9.075E+01 1.229E+02 +0.000E+00-0.000E+00
9.605E+01 1.224E+02 +0.000E+00-0.000E+00
9.948E+01 1.242E+02 +0.000E+00-0.000E+00
1.025E+02 1.297E+02 +0.000E+00-0.000E+00
1.061E+02 1.341E+02 +0.000E+00-0.000E+00
1.100E+02 1.420E+02 +0.000E+00-0.000E+00
1.145E+02 1.506E+02 +0.000E+00-0.000E+00
1.188E+02 1.634E+02 +0.000E+00-0.000E+00
1.236E+02 1.794E+02 +0.000E+00-0.000E+00
1.280E+02 1.954E+02 +0.000E+00-0.000E+00
1.322E+02 2.147E+02 +0.000E+00-0.000E+00
1.359E+02 2.344E+02 +0.000E+00-0.000E+00
1.388E+02 2.561E+02 +0.000E+00-0.000E+00
1.421E+02 2.799E+02 +0.000E+00-0.000E+00
1.460E+02 3.008E+02 +0.000E+00-0.000E+00
\END;
/*===================================================================*/
|