|
| /*===================================================================*/
/* NRDF D1672 Data No.11 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,11;
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,11;
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'42';
/*@42@*/
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,11;
INC-ENGY-LAB=5MEV;
EMT-1=D;
RSD=X;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DATA2'42' DELTA-DATA2
(DEG) (NODIM) (NODIM)
2.201E+01 -3.984E-02 +7.493E-04-8.577E-04
2.402E+01 -3.959E-02 +2.493E-04-5.705E-04
2.707E+01 -3.819E-02 +3.207E-04-4.280E-04
2.943E+01 -3.418E-02 +0.000E+00-0.000E+00
3.251E+01 -3.007E-02 +7.132E-04-4.991E-04
3.558E+01 -2.503E-02 +5.343E-04-6.425E-04
3.861E+01 -2.267E-02 +6.088E-04-3.209E-04
4.243E+01 -1.927E-02 +5.350E-04-6.782E-04
4.633E+01 -1.619E-02 +8.568E-04-2.859E-04
4.895E+01 -1.347E-02 +3.575E-04-6.057E-04
5.263E+01 -1.107E-02 +0.000E+00-0.000E+00
5.618E+01 -1.131E-02 +4.280E-04-5.352E-04
5.907E+01 -1.058E-02 +0.000E+00-0.000E+00
6.228E+01 -9.684E-03 +5.350E-04-5.352E-04
6.582E+01 -9.388E-03 +3.564E-04-5.000E-04
6.938E+01 -1.091E-02 +3.921E-04-3.207E-04
7.374E+01 -1.094E-02 +5.709E-04-4.286E-04
7.787E+01 -1.249E-02 +4.282E-04-4.995E-04
8.281E+01 -1.416E-02 +2.855E-04-3.211E-04
8.691E+01 -1.372E-02 +2.134E-04-3.925E-04
9.199E+01 -1.424E-02 +3.568E-04-5.352E-04
9.415E+01 -1.309E-02 +3.570E-04-4.282E-04
9.664E+01 -1.219E-02 +3.216E-04-3.570E-04
1.002E+02 -8.436E-03 +1.427E-04-3.925E-04
1.046E+02 -5.498E-03 +0.000E+00-0.000E+00
1.098E+02 -2.344E-03 +6.418E-04-5.359E-04
1.148E+02 2.559E-03 +0.000E+00-0.000E+00
1.175E+02 6.456E-03 +6.073E-04-3.211E-04
1.218E+02 1.136E-02 +7.139E-04-4.282E-04
1.244E+02 1.472E-02 +5.372E-04-8.914E-04
1.263E+02 1.469E-02 +5.718E-04-7.859E-04
1.275E+02 1.598E-02 +4.998E-04-6.432E-04
1.304E+02 1.595E-02 +5.720E-04-1.036E-03
1.321E+02 1.713E-02 +6.429E-04-6.432E-04
1.338E+02 1.674E-02 +4.293E-04-5.720E-04
1.355E+02 1.618E-02 +0.000E+00-0.000E+00
1.378E+02 1.718E-02 +4.295E-04-7.148E-04
1.405E+02 1.555E-02 +4.275E-04-4.639E-04
1.433E+02 1.459E-02 +5.707E-04-7.143E-04
1.449E+02 1.467E-02 +4.639E-04-6.070E-04
1.470E+02 1.460E-02 +4.634E-04-4.282E-04
1.492E+02 1.215E-02 +9.630E-04-7.507E-04
1.505E+02 1.265E-02 +7.852E-04-3.211E-04
1.535E+02 1.037E-02 +1.320E-03-9.300E-04
1.549E+02 1.041E-02 +5.709E-04-1.108E-03
1.569E+02 1.020E-02 +4.995E-04-5.000E-04
1.584E+02 7.105E-03 +6.791E-04-4.286E-04
1.600E+02 8.144E-03 +1.072E-03-8.559E-04
1.615E+02 4.544E-03 +1.285E-03-8.570E-04
1.631E+02 6.404E-03 +1.463E-03-1.284E-03
\END;
/*===================================================================*/
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