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| /*===================================================================*/
/* NRDF D1233 Data No.19 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,19;
D#=D1233;
TITLE=/SYSTEMATIC BEHAVIOR OF OCTUPOLE STRENGTHS IN 46,48,50TI/;
PURPOSE=/TO ESTABLISH THE 48TI LEVEL STRUCTURE OVER THE RANGE OF [1HW
EXCITATION ENERGY, AND TO DISCUSS THE SYSTEMATIC BEHAVIOR OF
THE OCTUPOLE EXCITATION STRENGTHS IN THE TI ISOTOPES/;
ATH=(A.HIGASHI'1',K.KATORI'1',M.FUJIWARA'2',H.IKEGAMI'2',I.KATAYAMA'2',
S.MORINOBU'2',M.TOSAKI'2',S.I.HAYAKAWA'3',N.IKEDA'4',
H.MIYATAKE'1');
INST-ATH=(2JPNOSA'1',2JPNRCN'2',2JPNAIT'3',2JPNINS'4');
REF=PR/C;
VLP=39(1989)1286;
RCTS=(48TI(P,P)48TI);
PHQS=(ANGL-DSTRN,ANALPW,DEFM-PARA,EWSR);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,19;
RCT=48TI(P,P)48TI;
RTY=(INEL-SATT,POL-RCT);
ENR=99.25%;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=0.495MG/CM**2;
BAC=SELF;
ACC=(CYC);
INST-ACC=2JPNRCN;
INC-ENGY-LAB=(65MEV);
BEAM-INTNSTY=[20NA;
POL-PRJ=[80%;
DET-PARTCL=(P);
DET-SYS=(MAG+PLST-SCT+X'21'+EDE,PROP-CNTR);
/*@21@*/
SOLID-ANGL=3.2MSR;
ERS-DET=30KEV;
ANL=(DWBA);
PHQ=(ANGL-DSTRN,ANALPW,DEFM-PARA,EWSR);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,19;
INC-ENGY-LAB=65MEV;
EXC-ENGY=4.472MEV;
TRNSF-L=3;
/*FIG.3-C*/
/* D1233 FIG.3-(C) */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (MB/SR) (MB/SR)
8.432 2.016E-02 +1.632E-02-1.308E-02
11.718 6.384E-03 +2.055E-03-1.720E-03
14.834 1.952E-02 +XXXXXXXXX-XXXXXXXXX
19.860 2.026E-02 +XXXXXXXXX-XXXXXXXXX
22.595 2.253E-02 +XXXXXXXXX-XXXXXXXXX
25.779 2.781E-02 +XXXXXXXXX-XXXXXXXXX
30.372 2.108E-02 +XXXXXXXXX-XXXXXXXXX
33.585 1.773E-02 +XXXXXXXXX-XXXXXXXXX
35.909 1.052E-02 +XXXXXXXXX-XXXXXXXXX
38.697 5.818E-03 +XXXXXXXXX-XXXXXXXXX
40.974 6.466E-03 +XXXXXXXXX-XXXXXXXXX
46.032 4.415E-03 +XXXXXXXXX-XXXXXXXXX
49.717 3.012E-03 +XXXXXXXXX-XXXXXXXXX
53.839 2.718E-03 +6.329E-04-2.701E-04
\END;
/*===================================================================*/
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