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/* NRDF D1100 Data No.29 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,29;
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,29;
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,29;
INC-ENGY-LAB=11.5MEV;
EXC-ENGY=0.596MEV;
J-PI=2+;
/*FIG.7-C*/
/* D1100 FIG.7-(C) */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (MB/SR) (MB/SR)
34.526 6.224E+00 +4.501E-01-4.197E-01
39.952 5.275E+00 +2.836E-01-2.252E-01
55.255 3.128E+00 +XXXXXXXXX-XXXXXXXXX
70.517 2.228E+00 +XXXXXXXXX-XXXXXXXXX
75.399 2.390E+00 +XXXXXXXXX-XXXXXXXXX
80.279 2.586E+00 +XXXXXXXXX-XXXXXXXXX
84.675 2.726E+00 +XXXXXXXXX-XXXXXXXXX
91.060 2.522E+00 +XXXXXXXXX-XXXXXXXXX
95.982 2.272E+00 +XXXXXXXXX-XXXXXXXXX
100.896 2.119E+00 +XXXXXXXXX-XXXXXXXXX
106.359 1.522E+00 +XXXXXXXXX-XXXXXXXXX
110.793 1.359E+00 +XXXXXXXXX-XXXXXXXXX
115.249 1.102E+00 +XXXXXXXXX-XXXXXXXXX
120.191 9.102E-01 +4.893E-02-3.886E-02
125.089 9.105E-01 +XXXXXXXXX-XXXXXXXXX
129.509 8.643E-01 +4.647E-02-5.119E-02
134.399 8.953E-01 +4.000E-02-3.820E-02
139.733 1.134E+00 +5.057E-02-3.889E-02
145.114 1.164E+00 +XXXXXXXXX-XXXXXXXXX
150.500 1.175E+00 +XXXXXXXXX-XXXXXXXXX
154.914 1.145E+00 +XXXXXXXXX-XXXXXXXXX
159.332 1.096E+00 +4.890E-02-6.494E-02
164.764 9.052E-01 +5.702E-02-6.838E-02
\END;
/*===================================================================*/
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