|
| /*===================================================================*/
/* NRDF D1672 Data No.16 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,16;
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,16;
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,DATA1'44',THTC);
/*@44@*/
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,16;
INC-ENGY-LAB=6MEV;
EMT-1=D;
RSD=X;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DATA4'44' DELTA-DATA4
(DEG) (NODIM) (NODIM)
2.104E+01 -1.281E-03 +0.000E+00-0.000E+00
2.400E+01 -1.826E-03 +1.348E-04-3.820E-04
2.703E+01 -3.135E-03 +1.571E-04-2.017E-04
2.975E+01 -3.613E-03 +1.574E-04-2.472E-04
3.353E+01 -3.957E-03 +1.348E-04-2.022E-04
3.729E+01 -4.706E-03 +2.021E-04-4.462E-05
4.015E+01 -6.150E-03 +0.000E+00-0.000E+00
4.367E+01 -7.078E-03 +0.000E+00-0.000E+00
4.711E+01 -8.119E-03 +0.000E+00-0.000E+00
5.029E+01 -9.428E-03 +0.000E+00-0.000E+00
5.251E+01 -1.071E-02 +0.000E+00-0.000E+00
5.564E+01 -1.115E-02 +0.000E+00-4.494E-05
5.853E+01 -1.151E-02 +0.000E+00-0.000E+00
6.307E+01 -1.350E-02 +0.000E+00-0.000E+00
6.731E+01 -1.432E-02 +0.000E+00-0.000E+00
7.179E+01 -1.536E-02 +0.000E+00-0.000E+00
7.452E+01 -1.593E-02 +2.016E-04-3.143E-04
7.930E+01 -1.782E-02 +0.000E+00-0.000E+00
8.280E+01 -1.954E-02 +0.000E+00-0.000E+00
8.631E+01 -2.056E-02 +0.000E+00-0.000E+00
8.909E+01 -2.227E-02 +2.919E-04-3.372E-04
9.133E+01 -2.261E-02 +0.000E+00-3.222E-07
9.274E+01 -2.407E-02 +3.593E-04-2.249E-04
9.691E+01 -2.473E-02 +4.937E-04-4.266E-04
1.012E+02 -2.638E-02 +1.794E-04-2.698E-04
1.064E+02 -2.911E-02 +1.573E-04-2.249E-04
1.107E+02 -2.984E-02 +5.845E-04-1.565E-04
1.138E+02 -3.016E-02 +2.252E-04-4.044E-04
1.172E+02 -2.943E-02 +2.700E-04-3.823E-04
1.215E+02 -2.811E-02 +2.021E-04-1.574E-04
1.257E+02 -2.720E-02 +0.000E+00-0.000E+00
1.272E+02 -2.551E-02 +2.695E-04-4.264E-04
1.294E+02 -2.460E-02 +3.590E-04-3.815E-04
1.318E+02 -2.316E-02 +3.364E-04-4.714E-04
1.344E+02 -2.213E-02 +3.375E-04-3.370E-04
1.357E+02 -2.038E-02 +0.000E+00-0.000E+00
1.387E+02 -1.918E-02 +0.000E+00-0.000E+00
1.407E+02 -1.736E-02 +2.465E-04-3.372E-04
1.431E+02 -1.582E-02 +2.017E-04-2.693E-04
1.450E+02 -1.407E-02 +0.000E+00-0.000E+00
1.465E+02 -1.331E-02 +0.000E+00-0.000E+00
1.485E+02 -1.133E-02 +2.918E-04-4.489E-04
1.503E+02 -1.057E-02 +3.142E-04-3.592E-04
1.528E+02 -9.341E-03 +0.000E+00-0.000E+00
1.532E+02 -6.848E-03 +2.472E-04-2.473E-04
1.556E+02 -6.223E-03 +1.566E-04-2.924E-04
1.578E+02 -5.014E-03 +2.467E-04-3.597E-04
1.597E+02 -4.434E-03 +2.008E-04-3.369E-04
1.623E+02 -3.743E-03 +3.602E-04-2.017E-04
1.639E+02 -1.633E-03 +2.468E-04-2.019E-04
1.673E+02 -2.090E-03 +1.793E-04-4.707E-04
\END;
/*===================================================================*/
|