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/* NRDF D0990 Data No.2 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,2;
D#=D990;
TITLE=/MEASUREMENT OF THE P-P ELASTIC-SCATTERING SPIN PARAMETER CLL AT
11.75 GEV/C FOR THETA-C.M.=48-90 DEGREES/;
PURPOSE=/TO DETERMINE IF CLL HAS THE RAPID ANGULAR DEPENDENCE THAT HAS
BEEN OBSERVED FOR LARGE-ANGLE CNN AT 11.75GEV/C, AND TO TEST
THE MODELS THAT HAVE BEEN PROPOSED DESCRIBING LARGE-ANGLE
ELASTIC SCATTERING VIA THE HARD SCATTERING OF TWO QUARKS./;
ATH=(I.P.AUER'1',E.COLTON'1',W.R.DITZLER'1',D.HILL'1',H.SPINKA'1',
N.TAMURA'1',J.-J.TAVERNIER'1',G.THEODOSIOU'1',K.TOSHIOKA'1',
D.UNDERWOOD'1',R.WAGNER'1',A.YOKOSAWA'1');
INST-ATH=(1USAANL'1');
REF=PRL;
VLP=52(1984)808;
RCTS=(P(P,P)P);
PHQ=(ANGL-DSTRN,SPIN-CORRL-PARA);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,2;
RCT=P(P,P)P;
RTY=(ELA-SCATT);
CHM=X'23';
/*@23@*/
PHYS-FORM=LIQD;
POL-TGT=X%;
ACC=(SYN);
INST-ACC=1USAANL;
INC-ENGY-LAB=(11.75GEV/C);
BEAM-INTNSTY=1.5[2.0*10**7'22';
/*@22@*/
CHRG-INC-ION=1;
POL-PRJ=61%;
DET-PARTCL=(P);
DET-SYS=(MAG+PS-PC'24'+PLST-SCT);
/*@24@*/
ANL=(X'25');
/*@25@*/
PHQ=(ANGL-DSTRN,SPIN-CORRL-PARA);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,2;
INC-ENGY-LAB=11.75GEV/C'21';
EXC-ENGY=0MEV;
/*FIG.2-(B)*/
/* D990 FIG.2-(B) */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC SPIN-CORRL-PARA'32' DELTA-SPIN-CORRL-PARA
(DEG) (NODIM) (NODIM)
51.039 +2.597E+00-2.597E+00 -1.405E-01 +7.301E-02-7.633E-02
55.714 +1.818E+00-1.039E+00 -8.075E-02 +8.628E-02-8.628E-02
61.429 +4.156E+00-2.597E+00 -1.670E-01 +8.296E-02-8.960E-02
68.182 +2.857E+00-2.338E+00 -1.173E-01 +9.292E-02-8.296E-02
75.195 +3.117E+00-2.338E+00 -1.139E-01 +1.128E-01-1.029E-01
85.844 +3.377E+00-3.117E+00 -1.504E-01 +1.692E-01-1.692E-01
\END;
/*===================================================================*/
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