|
| /*===================================================================*/
/* NRDF D1672 Data No.13 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,13;
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,13;
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'43';
/*@43@*/
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,13;
INC-ENGY-LAB=5MEV;
EMT-1=D;
RSD=X;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DATA3'43' DELTA-DATA3
(DEG) (NODIM) (NODIM)
1.885E+01 1.114E-02 +9.161E-04-8.808E-04
2.104E+01 1.233E-02 +3.235E-04-3.594E-04
2.478E+01 1.233E-02 +4.851E-04-6.108E-04
2.891E+01 1.362E-02 +7.008E-04-5.930E-04
3.209E+01 1.318E-02 +7.905E-04-4.675E-04
3.510E+01 1.260E-02 +5.391E-04-5.032E-04
3.812E+01 1.163E-02 +4.492E-04-3.414E-04
4.137E+01 1.192E-02 +4.311E-04-3.416E-04
4.365E+01 1.072E-02 +5.931E-04-5.571E-04
4.675E+01 9.444E-03 +3.775E-04-3.773E-04
5.026E+01 8.403E-03 +2.875E-04-5.389E-04
5.409E+01 7.452E-03 +5.210E-04-5.390E-04
5.824E+01 6.735E-03 +5.031E-04-3.234E-04
6.214E+01 6.449E-03 +4.313E-04-5.031E-04
6.597E+01 5.498E-03 +5.391E-04-2.874E-04
6.963E+01 4.889E-03 +4.851E-04-7.009E-04
7.313E+01 4.782E-03 +3.953E-04-3.234E-04
7.711E+01 5.000E-03 +3.414E-04-4.672E-04
8.100E+01 6.870E-03 +4.131E-04-4.313E-04
8.555E+01 7.699E-03 +4.673E-04-4.674E-04
9.122E+01 1.040E-02 +4.493E-04-3.415E-04
9.404E+01 1.347E-02 +4.672E-04-3.775E-04
9.711E+01 1.493E-02 +4.313E-04-2.875E-04
1.008E+02 1.647E-02 +5.031E-04-5.391E-04
1.039E+02 1.885E-02 +4.490E-04-5.392E-04
1.081E+02 1.863E-02 +3.953E-04-4.491E-04
1.119E+02 1.925E-02 +6.287E-04-9.525E-04
1.153E+02 1.700E-02 +5.211E-04-6.290E-04
1.204E+02 1.459E-02 +5.567E-04-5.750E-04
1.250E+02 1.134E-02 +5.751E-04-7.368E-04
1.277E+02 1.149E-02 +0.000E+00-0.000E+00
1.296E+02 1.023E-02 +7.904E-04-6.830E-04
1.322E+02 8.616E-03 +7.725E-04-8.987E-04
1.339E+02 6.244E-03 +7.548E-04-3.235E-04
1.359E+02 3.604E-03 +6.828E-04-8.091E-04
1.379E+02 3.586E-03 +7.549E-04-7.189E-04
1.390E+02 1.215E-03 +8.090E-04-7.369E-04
1.410E+02 2.812E-04 +5.392E-04-5.929E-04
1.428E+02 7.671E-04 +7.366E-04-3.953E-04
1.449E+02 -4.720E-04 +5.212E-04-5.931E-04
1.470E+02 -1.837E-03 +5.211E-04-5.032E-04
1.495E+02 -2.968E-03 +5.931E-04-7.733E-04
1.508E+02 -3.560E-03 +6.290E-04-3.773E-04
1.535E+02 -2.733E-03 +8.265E-04-3.597E-04
1.575E+02 -3.216E-03 +4.135E-04-5.570E-04
1.622E+02 -2.406E-03 +6.108E-04-6.113E-04
1.646E+02 -2.441E-03 +5.391E-04-6.652E-04
1.664E+02 -3.231E-03 +1.078E-03-1.186E-03
\END;
/*===================================================================*/
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