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| /*===================================================================*/
/* NRDF D1100 Data No.33 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,33;
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,33;
RCT=74GE(P,P)74GE;
RTY=(ELA-SCATT,INEL-SCATT);
ENR=94.5%;
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,33;
INC-ENGY-LAB=11.5MEV;
EXC-ENGY=0.596MEV;
J-PI=2+;
/*FIG.8-C*/
/* D1100 FIG.8-(C) */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC ANALPW DELTA-ANALPW
(DEG) (NODIM) (NODIM)
25.792 -2.274E-02 +XXXXXXXXX-XXXXXXXXX
30.698 -4.449E-02 +2.635E-02-2.156E-02
36.434 -5.909E-02 +3.594E-02-2.873E-02
40.476 -1.167E-01 +2.152E-02-2.635E-02
46.567 -1.793E-01 +3.832E-02-3.114E-02
50.611 -2.345E-01 +2.635E-02-2.156E-02
55.937 -2.491E-01 +1.916E-02-1.677E-02
61.394 -1.511E-01 +1.677E-02-2.395E-02
65.391 1.026E-01 +1.673E-02-1.919E-02
71.586 1.287E-01 +2.156E-02-1.915E-02
76.492 1.070E-01 +1.918E-02-1.198E-02
81.392 8.044E-02 +1.915E-02-2.156E-02
85.868 4.193E-02 +2.395E-02-1.198E-02
91.151 -8.580E-03 +2.154E-02-1.198E-02
95.930 -1.381E-01 +2.156E-02-1.677E-02
100.763 -2.221E-01 +2.157E-02-1.677E-02
106.066 -2.559E-01 +3.353E-02-2.394E-02
110.569 -2.704E-01 +2.635E-02-2.395E-02
116.049 -1.533E-01 +2.635E-02-3.353E-02
121.242 6.926E-02 +3.115E-02-2.635E-02
126.249 1.337E-01 +3.593E-02-2.874E-02
131.260 2.006E-01 +2.874E-02-1.677E-02
136.540 1.477E-01 +2.394E-02-2.876E-02
141.370 6.127E-02 +2.635E-02-2.159E-02
145.420 1.081E-02 +2.874E-02-2.157E-02
151.094 -5.648E-02 +3.353E-02-2.156E-02
155.615 -5.666E-02 +2.873E-02-2.157E-02
161.430 -4.200E-03 +3.114E-02-2.395E-02
165.995 3.394E-02 +3.114E-02-2.874E-02
\END;
/*===================================================================*/
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