|
| /*===================================================================*/
/* NRDF D1672 Data No.10 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,10;
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,10;
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,10;
INC-ENGY-LAB=6MEV;
EMT-1=D;
RSD=X;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DATA1'41' DELTA-DATA1
(DEG) (NODIM) (NODIM)
2.182E+01 4.214E-03 +3.613E-04-6.643E-05
2.479E+01 4.962E-03 +1.612E-04-1.336E-04
2.740E+01 5.511E-03 +2.830E-04-1.458E-04
3.006E+01 5.886E-03 +2.807E-04-1.875E-04
3.301E+01 6.112E-03 +2.150E-04-2.146E-04
3.602E+01 6.151E-03 +2.146E-04-1.065E-04
3.956E+01 6.909E-03 +1.081E-04-2.952E-04
4.269E+01 7.670E-03 +3.455E-04-2.292E-04
4.790E+01 7.832E-03 +3.876E-04-3.164E-04
5.053E+01 8.474E-03 +1.989E-04-2.811E-04
5.435E+01 9.004E-03 +1.765E-04-2.123E-04
5.699E+01 9.687E-03 +1.745E-04-2.280E-04
5.996E+01 1.090E-02 +1.478E-04-2.009E-04
6.351E+01 1.127E-02 +1.741E-04-1.333E-04
6.618E+01 1.170E-02 +1.616E-04-2.280E-04
7.063E+01 1.302E-02 +1.482E-04-1.875E-04
7.459E+01 1.431E-02 +1.340E-04-2.390E-04
7.835E+01 1.631E-02 +1.592E-04-1.344E-04
8.370E+01 1.721E-02 +1.608E-04-1.741E-04
8.835E+01 1.965E-02 +1.600E-04-2.009E-04
9.050E+01 2.081E-02 +2.936E-04-5.232E-04
9.209E+01 2.157E-02 +0.000E+00-0.000E+00
9.403E+01 2.284E-02 +4.135E-04-4.658E-04
9.749E+01 2.364E-02 +4.576E-04-5.338E-04
1.011E+02 2.564E-02 +3.349E-04-3.750E-04
1.054E+02 2.553E-02 +3.499E-04-4.544E-04
1.096E+02 2.630E-02 +3.994E-04-3.900E-04
1.140E+02 2.581E-02 +4.277E-04-5.452E-04
1.181E+02 2.484E-02 +3.616E-04-4.269E-04
1.221E+02 2.459E-02 +2.146E-04-1.620E-04
1.259E+02 2.178E-02 +2.669E-04-7.979E-05
1.277E+02 2.063E-02 +1.616E-04-1.470E-04
1.293E+02 1.876E-02 +3.094E-04-5.601E-04
1.312E+02 1.767E-02 +3.605E-04-6.022E-04
1.326E+02 1.646E-02 +4.815E-04-5.452E-04
1.347E+02 1.619E-02 +1.352E-04-8.019E-05
1.368E+02 1.462E-02 +3.337E-04-5.436E-04
1.388E+02 1.450E-02 +4.305E-04-4.171E-04
1.412E+02 1.282E-02 +3.074E-04-2.304E-04
1.436E+02 1.175E-02 +1.745E-04-2.539E-04
1.456E+02 1.075E-02 +2.017E-04-2.009E-04
1.478E+02 1.010E-02 +1.887E-04-3.994E-04
1.500E+02 9.993E-03 +3.078E-04-3.746E-04
1.524E+02 7.747E-03 +2.029E-04-2.819E-04
1.534E+02 7.769E-03 +2.005E-04-3.078E-04
1.553E+02 7.599E-03 +2.005E-04-3.475E-04
1.571E+02 6.253E-03 +4.289E-04-3.754E-04
1.585E+02 6.192E-03 +2.653E-04-2.523E-04
1.604E+02 5.099E-03 +4.135E-04-4.006E-04
1.622E+02 3.298E-03 +3.601E-04-3.070E-04
1.649E+02 4.101E-03 +4.815E-04-3.212E-04
\END;
/*===================================================================*/
|