|
| /*===================================================================*/
/* NRDF D1672 Data No.9 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,9;
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,9;
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'41';
/*@41@*/
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,9;
INC-ENGY-LAB=5MEV;
EMT-1=D;
RSD=X;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DATA1'41' DELTA-DATA1
(DEG) (NODIM) (NODIM)
2.060E+01 3.466E-03 +2.024E-04-2.818E-04
2.428E+01 4.196E-03 +3.867E-04-3.496E-04
2.780E+01 4.097E-03 +3.081E-04-2.123E-04
3.057E+01 5.596E-03 +1.200E-04-2.279E-04
3.402E+01 6.407E-03 +2.546E-04-4.553E-04
3.666E+01 6.420E-03 +1.851E-04-1.744E-04
3.946E+01 6.860E-03 +3.603E-04-3.349E-04
4.216E+01 6.792E-03 +1.605E-04-1.882E-04
4.468E+01 7.489E-03 +3.193E-04-2.016E-04
4.927E+01 7.786E-03 +1.748E-04-3.090E-04
5.361E+01 8.526E-03 +1.333E-04-2.154E-04
5.744E+01 9.603E-03 +1.610E-04-2.542E-04
6.124E+01 1.009E-02 +1.864E-04-1.458E-04
6.460E+01 1.127E-02 +2.274E-04-1.873E-04
6.803E+01 1.236E-02 +1.869E-04-2.948E-04
7.175E+01 1.325E-02 +3.215E-04-3.581E-04
7.443E+01 1.432E-02 +2.132E-04-2.551E-04
7.863E+01 1.556E-02 +1.338E-04-2.551E-04
8.319E+01 1.698E-02 +1.908E-04-2.818E-04
8.849E+01 1.877E-02 +3.099E-04-2.391E-04
9.381E+01 1.945E-02 +2.145E-04-1.735E-04
9.668E+01 2.067E-02 +9.321E-05-1.088E-04
1.005E+02 2.109E-02 +9.585E-05-1.601E-04
1.040E+02 2.205E-02 +1.200E-04-2.132E-04
1.074E+02 2.184E-02 +1.882E-04-1.472E-04
1.115E+02 2.097E-02 +3.220E-04-3.046E-04
1.148E+02 2.076E-02 +1.757E-04-3.202E-04
1.191E+02 2.001E-02 +2.270E-04-1.869E-04
1.234E+02 1.834E-02 +3.621E-04-3.991E-04
1.282E+02 1.770E-02 +0.000E+00-0.000E+00
1.279E+02 1.734E-02 +3.068E-04-7.091E-04
1.305E+02 1.551E-02 +3.077E-04-3.211E-04
1.321E+02 1.550E-02 +1.351E-04-4.424E-04
1.343E+02 1.428E-02 +4.700E-04-4.562E-04
1.356E+02 1.351E-02 +2.391E-04-2.024E-04
1.374E+02 1.231E-02 +3.327E-04-3.206E-04
1.390E+02 1.226E-02 +1.766E-04-1.739E-04
1.412E+02 1.047E-02 +4.147E-04-4.290E-04
1.429E+02 1.014E-02 +6.047E-04-4.518E-04
1.448E+02 1.010E-02 +1.739E-04-1.744E-04
1.466E+02 8.724E-03 +3.621E-04-3.603E-04
1.490E+02 7.934E-03 +3.759E-04-5.187E-04
1.515E+02 7.774E-03 +2.020E-04-2.671E-04
1.528E+02 7.177E-03 +0.000E+00-0.000E+00
1.528E+02 6.990E-03 +1.338E-05-0.000E+00
1.558E+02 6.639E-03 +2.426E-04-3.991E-04
1.578E+02 5.316E-03 +4.031E-04-3.331E-04
1.596E+02 4.529E-03 +4.428E-04-4.687E-04
1.607E+02 3.948E-03 +2.288E-04-4.415E-04
1.633E+02 4.134E-03 +2.577E-04-2.141E-04
1.651E+02 3.147E-03 +5.218E-04-4.816E-04
1.666E+02 3.340E-03 +3.340E-04-2.274E-04
1.676E+02 3.160E-03 +3.228E-04-3.478E-04
\END;
/*===================================================================*/
|