|
| /*===================================================================*/
/* NRDF D1672 Data No.14 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,14;
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,14;
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,14;
INC-ENGY-LAB=6MEV;
EMT-1=D;
RSD=X;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DATA3'43' DELTA-DATA3
(DEG) (NODIM) (NODIM)
2.032E+01 1.223E-02 +5.377E-04-3.222E-04
2.310E+01 1.317E-02 +4.303E-04-4.659E-04
2.685E+01 1.432E-02 +6.450E-04-4.838E-04
3.059E+01 1.444E-02 +3.401E-04-2.329E-04
3.385E+01 1.455E-02 +4.840E-04-4.300E-04
3.734E+01 1.451E-02 +4.299E-04-3.763E-04
3.992E+01 1.264E-02 +4.123E-04-5.197E-04
4.276E+01 1.260E-02 +2.866E-04-3.045E-04
4.542E+01 1.097E-02 +2.151E-04-2.329E-04
4.825E+01 9.859E-03 +2.150E-04-1.076E-04
5.165E+01 8.297E-03 +2.147E-04-3.225E-04
5.464E+01 7.489E-03 +1.612E-04-2.870E-04
5.876E+01 5.801E-03 +0.000E+00-0.000E+00
6.314E+01 4.813E-03 +2.150E-04-2.331E-04
6.720E+01 4.182E-03 +1.254E-04-2.511E-04
7.060E+01 3.481E-03 +1.792E-04-2.689E-04
7.450E+01 3.120E-03 +2.689E-04-1.971E-04
7.791E+01 2.992E-03 +3.047E-04-2.867E-04
8.142E+01 3.725E-03 +1.971E-04-3.047E-04
8.730E+01 6.104E-03 +1.613E-04-3.767E-04
9.007E+01 5.941E-03 +3.944E-04-7.889E-04
9.262E+01 7.946E-03 +1.613E-04-2.689E-04
9.498E+01 8.715E-03 +4.838E-04-6.093E-04
9.846E+01 1.269E-02 +5.018E-04-6.453E-04
1.028E+02 1.557E-02 +6.807E-04-6.453E-04
1.064E+02 1.681E-02 +4.122E-04-5.016E-04
1.106E+02 1.964E-02 +4.299E-04-6.090E-04
1.139E+02 1.974E-02 +4.841E-04-4.662E-04
1.172E+02 2.094E-02 +4.299E-04-5.379E-04
1.216E+02 1.823E-02 +4.297E-04-6.100E-04
1.252E+02 1.665E-02 +5.018E-04-4.296E-04
1.274E+02 1.407E-02 +3.944E-04-2.866E-04
1.290E+02 1.358E-02 +5.016E-04-8.241E-04
1.314E+02 1.235E-02 +5.020E-04-5.196E-04
1.336E+02 8.473E-03 +6.987E-04-6.812E-04
1.354E+02 6.554E-03 +5.375E-04-8.422E-04
1.371E+02 5.173E-03 +6.094E-04-5.021E-04
1.386E+02 3.452E-03 +6.809E-04-5.377E-04
1.402E+02 1.049E-03 +6.807E-04-6.094E-04
1.421E+02 1.729E-03 +4.122E-04-3.942E-04
1.440E+02 -4.409E-04 +5.734E-04-4.839E-04
1.463E+02 -1.159E-03 +5.555E-04-6.271E-04
1.478E+02 -3.365E-03 +1.434E-04-3.229E-04
1.499E+02 -3.492E-03 +1.972E-04-1.074E-04
1.516E+02 -3.690E-03 +1.614E-04-2.510E-04
1.520E+02 -4.192E-03 +1.254E-04-2.329E-04
1.532E+02 -4.462E-03 +1.792E-04-1.433E-04
1.540E+02 -4.892E-03 +1.613E-04-2.151E-04
1.561E+02 -5.593E-03 +2.865E-04-2.870E-04
1.589E+02 -6.276E-03 +3.046E-04-5.198E-04
1.615E+02 -5.310E-03 +1.971E-04-2.866E-04
1.633E+02 -5.203E-03 +5.199E-04-5.736E-04
1.647E+02 -5.402E-03 +0.000E+00-0.000E+00
1.672E+02 -5.224E-03 +6.990E-04-3.944E-04
\END;
/*===================================================================*/
|