|
| /*===================================================================*/
/* NRDF D0152 Data No.2 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,2;
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,2;
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,2;
INC-ENGY=51.93MEV;
THTC=5.8[110.3DEG;
EXC-ENGY=1.10MEV;
J-PI=1/2-;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (MB/SR) (MB/SR)
6.0 1.04 0.02
8.0 0.95 0.02
10.6 0.73 0.02
13.1 0.42 0.02
15.7 0.24 0.01
18.3 0.19 0.01
20.8 0.20 0.01
23.4 0.20 0.01
26.0 0.16 0.01
28.5 0.11 0.01
31.1 0.083 0.004
33.7 0.059 0.004
36.2 0.064 0.004
38.8 0.054 0.003
41.3 0.039 0.003
43.9 0.025 0.002
46.4 0.018 0.002
49.0 0.015 0.002
51.5 0.013 0.0014
54.1 0.011 0.0013
56.6 0.013 0.0014
59.1 0.012 0.0014
61.7 0.010 0.0013
64.2 0.0085 0.0012
66.7 0.0087 0.0012
69.3 0.0084 0.0012
71.8 0.0057 0.0010
74.3 0.0062 0.0010
76.8 0.0048 0.0009
79.4 0.0043 0.0008
81.9 0.0048 0.0009
86.9 0.0033 0.0007
91.9 0.0033 0.0007
96.9 0.0024 0.0006
101.9 0.0024 0.0006
106.8 0.0014 0.0005
111.8 0.0016 0.0005
\END;
/*===================================================================*/
|