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| /*===================================================================*/
/* NRDF D1100 Data No.34 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,34;
D#=D1100;
TITLE=/EVIDENCE OF A SHAPE TRANSITION IN EVEN-A GE ISOTOPES/;
PURPOSE=/TO INVESTIGATE THE COLLECTIVE PROPERTIES OF THE EVEN-EVEN
ISOTOPES OF GE(70,72,74,76) AS MANIFESTED IN THE ELASTIC AND
INELASTIC SCATTERING TO THE FIRST 2+ STATE OF VECTOR POLARIZED
DEUTERONS AND PROTONS FROM THESE NUCLEI./;
ATH=(S.SEN'1',S.E.DARDEN'1',R.C.LUHN'1',N.O.GAISER'1',G.MURILLO'2',
J.RAMIREZ'2');
INST-ATH=(1USANOT'1',3MEXCNM'2');
REF=PR/C;
VLP=31(1985)787;
RCTS=(70GE(D,D)70GE,72GE(D,D)72GE,74GE(D,D)74GE,76GE(D,D)76GE,
70GE(P,P)70GE,72GE(P,P)72GE,74GE(P,P)74GE,76GE(P,P)76GE);
PHQS=(ANGL-DSTRN,XSECTN-RATIO,ANALPW);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,34;
RCT=76GE(P,P)76GE;
RTY=(ELA-SCATT,INEL-SCATT);
ENR=73.9%;
CHM=ELM;
THK-TGT=300[350UG/CM**2;
BAC=SELF;
ACC=(VDGT);
INST-ACC=1USANOT;
INC-ENGY-LAB=(11.5MEV);
BEAM-INTNSTY=7NA;
POL-PRJ=0.60'23';
/*@23@*/
DET-PARTCL=(P);
DET-SYS=(SSD);
ANL=(CC);
PHQ=(ANGL-DSTRN,XSECTN-RATIO,ANALPW);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,34;
INC-ENGY-LAB=11.5MEV;
EXC-ENGY=0.562MEV;
J-PI=2+;
/*FIG.8-D*/
/* D1100 FIG.8-(D) */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC ANALPW DELTA-ANALPW
(DEG) (NODIM) (NODIM)
26.633 2.413E-02 +1.916E-02-1.677E-02
31.496 -1.449E-02 +2.156E-02-1.193E-02
36.775 -5.073E-02 +1.437E-02-2.156E-02
40.405 -8.928E-02 +2.156E-02-1.198E-02
46.451 -1.567E-01 +2.158E-02-1.916E-02
50.336 -2.839E-01 +2.637E-02-2.156E-02
56.152 -2.483E-01 +2.395E-02-3.114E-02
60.850 -1.480E-01 +1.679E-02-2.156E-02
66.237 1.104E-01 +2.398E-02-1.916E-02
71.185 1.197E-01 +2.395E-02-1.677E-02
76.526 1.194E-01 +2.156E-02-1.437E-02
81.436 1.071E-01 +3.353E-02-2.156E-02
85.826 3.257E-02 +1.916E-02-2.395E-02
91.041 -3.961E-02 +1.916E-02-1.916E-02
96.637 -1.286E-01 +3.114E-02-2.395E-02
101.010 -2.127E-01 +2.635E-02-2.395E-02
105.894 -2.393E-01 +3.353E-02-3.590E-02
111.584 -2.756E-01 +4.077E-02-3.830E-02
116.679 -1.825E-01 +4.072E-02-3.590E-02
121.978 2.561E-02 +3.114E-02-3.111E-02
127.099 1.331E-01 +3.353E-02-3.353E-02
132.207 2.334E-01 +3.356E-02-3.353E-02
137.812 1.492E-01 +3.114E-02-3.111E-02
141.782 6.994E-02 +3.353E-02-3.351E-02
146.548 -2.377E-02 +3.353E-02-3.114E-02
151.768 -9.355E-02 +3.356E-02-3.111E-02
156.559 -1.729E-01 +2.635E-02-3.114E-02
162.477 -7.982E-02 +5.030E-02-4.548E-02
166.717 -5.816E-03 +5.504E-02-4.311E-02
\END;
/*===================================================================*/
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