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| /*===================================================================*/
/* NRDF D1100 Data No.31 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,31;
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,31;
RCT=70GE(P,P)70GE;
RTY=(ELA-SCATT,INEL-SCATT);
ENR=84.6%;
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,31;
INC-ENGY-LAB=11.5MEV;
EXC-ENGY=1.040MEV;
J-PI=2+;
/*FIG.8-A*/
/* D1100 FIG.8-(A) */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC ANALPW DELTA-ANALPW
(DEG) (NODIM) (NODIM)
26.027 -2.716E-02 +1.975E-02-1.481E-02
30.548 -5.926E-02 +1.728E-02-1.728E-02
36.712 -9.136E-02 +1.728E-02-1.728E-02
40.411 -1.506E-01 +2.222E-02-2.222E-02
51.096 -2.420E-01 +1.975E-02-1.728E-02
56.849 -2.593E-01 +2.222E-02-1.975E-02
60.959 -2.272E-01 +1.975E-02-1.728E-02
65.890 -1.556E-01 +2.222E-02-2.222E-02
70.822 -3.210E-02 +2.469E-02-2.469E-02
79.863 8.642E-02 +2.963E-02-1.975E-02
95.890 -1.136E-01 +2.963E-02-2.222E-02
99.589 -2.074E-01 +2.716E-02-2.716E-02
105.342 -2.123E-01 +2.963E-02-2.469E-02
110.274 -2.568E-01 +3.210E-02-2.963E-02
115.616 -2.543E-01 +2.963E-02-2.469E-02
120.137 -1.852E-01 +2.469E-02-1.975E-02
125.479 -5.926E-02 +2.469E-02-2.222E-02
130.000 3.210E-02 +3.951E-02-3.210E-02
140.274 6.667E-02 +3.951E-02-4.198E-02
145.205 1.457E-01 +5.185E-02-4.938E-02
150.959 1.877E-01 +3.951E-02-4.938E-02
154.658 2.765E-01 +5.185E-02-5.432E-02
160.411 3.654E-01 +3.704E-02-3.457E-02
164.932 3.506E-01 +4.444E-02-4.444E-02
\END;
/*===================================================================*/
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