|
| /*===================================================================*/
/* NRDF D1672 Data No.12 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,12;
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,12;
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,12;
INC-ENGY-LAB=6MEV;
EMT-1=D;
RSD=X;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DATA2'42' DELTA-DATA2
(DEG) (NODIM) (NODIM)
2.211E+01 -4.501E-02 +0.000E+00-0.000E+00
2.577E+01 -4.360E-02 +0.000E+00-0.000E+00
2.775E+01 -3.877E-02 +0.000E+00-0.000E+00
2.965E+01 -3.433E-02 +0.000E+00-0.000E+00
3.276E+01 -2.993E-02 +0.000E+00-0.000E+00
3.610E+01 -2.499E-02 +1.785E-04-2.499E-04
3.928E+01 -2.040E-02 +0.000E+00-0.000E+00
4.234E+01 -1.728E-02 +0.000E+00-0.000E+00
4.619E+01 -1.387E-02 +0.000E+00-0.000E+00
4.960E+01 -1.179E-02 +0.000E+00-0.000E+00
5.292E+01 -9.917E-03 +0.000E+00-0.000E+00
5.628E+01 -9.402E-03 +0.000E+00-0.000E+00
5.942E+01 -9.601E-03 +3.209E-04-5.704E-04
6.213E+01 -8.768E-03 +0.000E+00-0.000E+00
6.549E+01 -8.431E-03 +0.000E+00-0.000E+00
6.911E+01 -8.915E-03 +1.778E-04-4.295E-04
7.315E+01 -1.025E-02 +2.506E-04-4.298E-04
7.793E+01 -1.191E-02 +0.000E+00-0.000E+00
8.303E+01 -1.406E-02 +0.000E+00-0.000E+00
8.757E+01 -1.590E-02 +0.000E+00-0.000E+00
8.931E+01 -1.486E-02 +3.584E-04-4.648E-04
9.158E+01 -1.581E-02 +0.000E+00-0.000E+00
9.324E+01 -1.480E-02 +3.930E-04-3.573E-04
9.608E+01 -1.615E-02 +6.072E-04-5.708E-04
1.003E+02 -1.495E-02 +6.068E-04-5.009E-04
1.042E+02 -8.969E-03 +6.782E-04-8.214E-04
1.087E+02 -4.878E-03 +0.000E+00-0.000E+00
1.131E+02 1.175E-03 +1.781E-04-3.562E-04
1.172E+02 6.120E-03 +3.930E-04-3.930E-04
1.210E+02 1.124E-02 +3.908E-04-4.998E-04
1.237E+02 1.447E-02 +0.000E+00-0.000E+00
1.257E+02 1.569E-02 +5.708E-04-6.797E-04
1.272E+02 1.809E-02 +5.355E-04-5.701E-04
1.293E+02 1.960E-02 +3.216E-04-4.287E-04
1.312E+02 1.829E-02 +2.142E-04-4.295E-04
1.330E+02 1.947E-02 +2.491E-04-4.276E-04
1.350E+02 1.791E-02 +0.000E+00-0.000E+00
1.371E+02 1.849E-02 +4.663E-04-1.789E-04
1.399E+02 1.758E-02 +4.317E-04-4.284E-04
1.423E+02 1.655E-02 +4.641E-04-7.496E-04
1.441E+02 1.649E-02 +3.577E-04-3.213E-04
1.466E+02 1.475E-02 +6.433E-04-6.072E-04
1.487E+02 1.458E-02 +3.938E-04-3.216E-04
1.504E+02 1.316E-02 +4.287E-04-4.633E-04
1.531E+02 1.128E-02 +3.573E-04-5.365E-04
1.543E+02 9.788E-03 +3.216E-04-2.491E-04
1.565E+02 8.299E-03 +5.693E-04-5.347E-04
1.580E+02 8.091E-03 +3.562E-04-5.001E-04
1.596E+02 8.171E-03 +4.641E-04-5.362E-04
1.612E+02 4.572E-03 +4.994E-04-7.121E-04
1.633E+02 5.438E-03 +5.355E-04-4.287E-04
\END;
/*===================================================================*/
|