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| /*===================================================================*/
/* NRDF D0152 Data No.3 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,3;
D#=D152;
TITLE=/(P,D) REACTIONS AT 52 MEV.I.58NI(P,D)57NI (EXPERIMENTAL)/;
PURPOSE=/TO TEST THE VALIDITY OF CURRENT REACTION THEORIES,(P,D)ANGULAR
DISTRIBUTION HAVE BEEN TAKEN AT THE INCIDENT ENERGY OF 52MEV,
THE HIGHEST ENERGY SO FAR STUDIED,OVER A WIDE RANGE OF ANGLES
AND IN SMALL STEPS'D'/;
ATH=(H.OHNUMA'C',T.SUEHIRO'A,C',M.SEKIGUCHI'C',S.YAMADA'B,C');
INST-ATH=(2JPNINS'C');
/* 'A' PRESENT ADRESS:TOHOKU INSTITUTE OF TECHNOLOGY */
/* 'B' PRESENT ADRESS: TOKYO INSTITUTE OF TECHNOLOGY */
REF=JPJ;
VLP=36(1974)1236;
RCTS=(58NI(P,D)57NI);
/* 'D'THE 58NI(P,D)REACTION,WHICH WE BELIEVE REQUIRE ANALYSIS FROM
VARIOUS ASPECTS. BRIET DESCRIPTION OF ANALYSIS AND SPECTIOSCOPIC
INFORMATION OBTAINED ARE ALSO GIVEN. DETAILS OF THE ANALYSIS WE HAVE
DONE SO FAR WILL BE GIVEN IN A SUBSEQUENT PAPER: H.OHNUMA ET AL.,
J .PHYS.SOC.JAPAN 36(1974)1245 */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,3;
RCT=58NI(P,D)57NI;
CHM=ELM;
THK-TGT=2.7MG/CM**2;
BAC=SELF;
ACC=(SYNCYC);
INST-ACC=2JPNINS;
INC-ENGY-RANGE=(51.93MEV);
DET-PARTCL=(D);
DET-SYS=(D);
DET-SYS=(MAG+PROP-CNTR);
ERS-DET=70KEV;
ANL=(OPT-MODEL,DWBA);
PHQ=(ANGL-DSTRN);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,3;
INC-ENGY=51.93MEV;
THTC=5.8[110.3DEG;
EXC-ENGY=0.76MEV;
J-PI=5/2-;
TRANSF-L=[3;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (MB/SR) (MB/SR)
6.0 1.06 0.02
8.0 1.00 0.02
10.6 0.92 0.02
13.1 0.90 0.03
15.7 0.79 0.02
18.3 0.66 0.02
20.8 0.49 0.01
23.4 0.36 0.01
26.0 0.26 0.01
28.5 0.21 0.01
31.1 0.21 0.01
33.7 0.21 0.01
36.2 0.195 0.006
38.8 0.143 0.005
41.3 0.116 0.004
43.9 0.088 0.004
46.4 0.079 0.003
49.0 0.089 0.004
51.5 0.090 0.004
54.1 0.097 0.004
56.6 0.086 0.003
59.1 0.075 0.003
61.7 0.055 0.003
64.2 0.044 0.003
66.7 0.034 0.002
69.3 0.034 0.002
71.8 0.030 0.002
74.3 0.028 0.002
76.8 0.024 0.002
79.4 0.025 0.002
81.9 0.023 0.002
86.9 0.015 0.0015
91.9 0.012 0.0013
96.9 0.0082 0.0012
101.9 0.0066 0.0010
106.8 0.0042 0.0008
111.8 0.0035 0.0008
\END;
/*===================================================================*/
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