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| /*===================================================================*/
/* NRDF D0404 Data No.4 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,4;
D#=D404;
TITLE=/USE OF 30SI(P,ALPHA)27AL ANALYZING POWER/;
PURPOSE=/THE PURPOSE OF THE PRESENT REPORT IS TO SHOW HOW THE ANALYZING
POWER , I*T11,OF THE (P,ALPHA) REACTION COULD HELP IN FINDING
A UNIQUE SET OF OPTICAL MODEL PARAMETERS AND THE SPIN AND
PARITY OF A STAE/;
ATH=(M.A.M.SHAHABUDDIN'1',L.BUJA-BIJUNAS'1',W.R.STOTT'1',
J.C.WADDINGTON'1');
INST-ATH=(1CANMCM'1');
REF=CJP;
VLP=57(1979)505;
RCTS=(30SI(P,ALPHA)27AL);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,4;
ENR=X%;
CHM=ELM;
THK-TGT=100UG/CM**2;
BAC=SELF;
POL-TGT=NO;
ALGN-TGT=NO;
ACC=(VDG);
INST-ACC=1CANMCM;
INC-ENGY-LAB-RANGE=(17.0MEV);
DELTA-INC-ENGY-LAB=XKEV;
ERS-PRJ=XKEV;
BEAM-INTNSTY=[30NA;
POL-PRJ=YES;
DET-PARTCL=(ALPHA);
DET-SYS=(CNTR-TLSCP);
SOLID-ANGL=XMSR;
ERS-DET=XKEV;
ANL=(OPT-MODEL,DWBA);
PHQ=(XSECTN,ANGL-DSTRN,DSIGMA/DOMEGA,ANALPW,OPT-POTL-PARA);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,4;
EXC-ENGY=0.0MEV;
DELTA-EXC-ENGY=X MEV;
J-PI=5/2+;
/*FIG.1-(D)*/
/* D404 FIG.1-(D) */
/* SER#= 4 */
/* XSCALE=LINEAR YSCALE=LINEAR */
/* XMAX= 1.00000000E+02 YMAX= 5.99999964E-01 */
/* XMIN= 0.00000000E+00 YMIN= 0.00000000E+00 */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DATA1'1' DELTA-DATA1
(DEG) (NODIM) (NODIM)
16.201 -2.065E-01 3.348E-02
21.508 -2.344E-01 2.511E-02
26.816 -2.372E-01 3.069E-02
32.402 -2.009E-01 3.906E-02
37.709 -1.060E-01 2.511E-02
43.017 -7.535E-02 3.069E-02
48.603 -1.256E-01 2.790E-02
53.073 -1.507E-01 2.511E-02
58.938 -1.647E-01 2.511E-02
63.966 -1.702E-01 3.069E-02
\END;
/*===================================================================*/
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