|
| /*===================================================================*/
/* NRDF D1672 Data No.15 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,15;
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,15;
RCT=P(D,D)X;
RTY=(POL-RCT);
ENR=NAT;
CHM=ELM;
PHYS-FORM=GAS;
THK-TGT=0.27ATM;
BAC=SELF;
POL-TGT=0.70%;
ACC=(VDGT);
INST-ACC=2JPNKYU;
INC-ENGY-LAB=(2,2.5,3,4,5,6MEV);
DET-PARTCL=(D);
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=(TNSR-ANALPW,DATA1'44',THTC);
/*@44@*/
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,15;
INC-ENGY-LAB=5MEV;
EMT-1=D;
RSD=X;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DATA4'44' DELTA-DATA4
(DEG) (NODIM) (NODIM)
2.013E+01 -8.640E-04 +3.982E-04-4.343E-04
2.236E+01 -1.588E-03 +4.707E-04-6.152E-04
2.547E+01 -1.824E-03 +2.716E-04-3.802E-04
2.834E+01 -3.418E-03 +0.000E+00-0.000E+00
3.169E+01 -3.165E-03 +4.163E-04-2.353E-04
3.519E+01 -4.288E-03 +1.991E-04-3.077E-04
3.838E+01 -4.632E-03 +2.715E-04-1.810E-04
4.212E+01 -5.683E-03 +1.810E-04-3.620E-04
4.571E+01 -7.095E-03 +2.715E-04-5.248E-04
4.842E+01 -7.295E-03 +1.991E-04-4.526E-04
5.200E+01 -9.232E-03 +1.267E-04-2.896E-04
5.511E+01 -9.559E-03 +2.896E-04-2.172E-04
5.838E+01 -1.014E-02 +2.715E-04-2.896E-04
6.133E+01 -1.063E-02 +3.438E-04-3.259E-04
6.531E+01 -1.213E-02 +3.981E-04-3.619E-04
6.937E+01 -1.246E-02 +5.068E-04-3.620E-04
7.415E+01 -1.452E-02 +0.000E+00-0.000E+00
7.798E+01 -1.481E-02 +4.344E-04-1.629E-04
8.204E+01 -1.586E-02 +0.000E+00-0.000E+00
8.594E+01 -1.737E-02 +0.000E+00-0.000E+00
9.040E+01 -1.945E-02 +3.077E-04-2.715E-04
9.279E+01 -2.102E-02 +2.172E-04-1.991E-04
9.581E+01 -2.173E-02 +1.448E-04-4.163E-04
1.004E+02 -2.407E-02 +3.258E-04-2.715E-04
1.054E+02 -2.459E-02 +0.000E+00-0.000E+00
1.098E+02 -2.494E-02 +3.801E-04-2.715E-04
1.137E+02 -2.481E-02 +3.078E-04-3.620E-04
1.176E+02 -2.356E-02 +4.525E-04-2.172E-04
1.217E+02 -2.248E-02 +3.802E-04-2.534E-04
1.240E+02 -2.101E-02 +7.239E-04-6.879E-04
1.264E+02 -2.029E-02 +3.801E-04-2.353E-04
1.281E+02 -1.922E-02 +2.896E-04-2.534E-04
1.305E+02 -1.891E-02 +2.353E-04-3.077E-04
1.319E+02 -1.748E-02 +2.353E-04-3.801E-04
1.347E+02 -1.567E-02 +2.534E-04-3.259E-04
1.365E+02 -1.533E-02 +4.706E-04-3.077E-04
1.392E+02 -1.388E-02 +2.353E-04-3.077E-04
1.418E+02 -1.235E-02 +5.610E-04-4.344E-04
1.440E+02 -1.137E-02 +3.982E-04-3.258E-04
1.459E+02 -1.021E-02 +4.162E-04-3.077E-04
1.482E+02 -8.636E-03 +2.896E-04-4.706E-04
1.502E+02 -7.732E-03 +5.792E-04-3.439E-04
1.518E+02 -6.411E-03 +3.801E-04-5.068E-04
1.539E+02 -4.981E-03 +2.353E-04-5.249E-04
1.561E+02 -4.928E-03 +3.801E-04-3.258E-04
1.571E+02 -3.245E-03 +3.257E-04-1.629E-04
1.598E+02 -3.317E-03 +3.801E-04-3.077E-04
1.616E+02 -1.055E-03 +2.354E-04-5.430E-04
1.636E+02 -2.522E-03 +5.430E-04-6.335E-04
\END;
/*===================================================================*/
|