|
| /*===================================================================*/
/* NRDF D1672 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
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,1;
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,1;
INC-ENGY-LAB=2.5MEV;
EMT-1=P;
RSD=X;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (MB/SR) (MB/SR)
2.193E+01 3.798E+02 +5.002E+00-3.732E+00
2.444E+01 3.111E+02 +2.136E+00-3.554E+00
2.725E+01 2.704E+02 +1.964E+00-3.373E+00
2.929E+01 2.425E+02 +0.000E+00-0.000E+00
3.199E+01 2.292E+02 +0.000E+00-0.000E+00
3.501E+01 2.175E+02 +0.000E+00-0.000E+00
3.833E+01 2.092E+02 +0.000E+00-0.000E+00
4.102E+01 2.009E+02 +0.000E+00-0.000E+00
4.434E+01 1.945E+02 +0.000E+00-0.000E+00
4.742E+01 1.862E+02 +0.000E+00-0.000E+00
4.993E+01 1.806E+02 +0.000E+00-0.000E+00
5.286E+01 1.728E+02 +0.000E+00-0.000E+00
5.521E+01 1.664E+02 +0.000E+00-0.000E+00
5.756E+01 1.608E+02 +0.000E+00-0.000E+00
6.000E+01 1.539E+02 +0.000E+00-0.000E+00
6.235E+01 1.477E+02 +0.000E+00-0.000E+00
6.494E+01 1.431E+02 +0.000E+00-0.000E+00
6.786E+01 1.367E+02 +0.000E+00-0.000E+00
7.077E+01 1.322E+02 +0.000E+00-0.000E+00
7.674E+01 1.252E+02 +0.000E+00-0.000E+00
8.094E+01 1.197E+02 +0.000E+00-0.000E+00
8.458E+01 1.144E+02 +0.000E+00-0.000E+00
8.789E+01 1.102E+02 +0.000E+00-0.000E+00
9.127E+01 1.080E+02 +0.000E+00-0.000E+00
9.482E+01 1.065E+02 +0.000E+00-0.000E+00
9.891E+01 1.076E+02 +0.000E+00-0.000E+00
1.034E+02 1.102E+02 +0.000E+00-0.000E+00
1.084E+02 1.172E+02 +0.000E+00-0.000E+00
1.127E+02 1.244E+02 +0.000E+00-0.000E+00
1.156E+02 1.346E+02 +0.000E+00-0.000E+00
1.183E+02 1.466E+02 +0.000E+00-0.000E+00
1.218E+02 1.629E+02 +0.000E+00-0.000E+00
1.252E+02 1.788E+02 +0.000E+00-0.000E+00
1.298E+02 1.991E+02 +0.000E+00-0.000E+00
1.318E+02 2.204E+02 +0.000E+00-0.000E+00
1.373E+02 2.424E+02 +0.000E+00-0.000E+00
1.415E+02 2.659E+02 +0.000E+00-0.000E+00
\END;
/*===================================================================*/
|