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/* NRDF D1842 Data No.210 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,210;
D#=D1842;
TITLE=/Preequilibrium (p,p') spectra for nuclei around neutron number
50/;
PURPOSE=/To see how the shell and odd-even effects will appear in the
continuum proton spectra, and to interpret the experimental
results in terms of realistic partial state density within the
framework of the preequilibrium model/;
ATH=(Y.WATANABE'1', I.KUMABE'1', M.HYAKUTAKE'1', N.KOORI'1',
K.OGAWA'1', K.ORITO'1', K.AKAGI'1', N.ODA'1');
INST-ATH=(2JPNKYU'1');
/* '1' Department of Nuclear Engineering */
REF=PR/C;
VLP=36(1987)1325;
RCTS=(90ZR(P,P)X, 92MO(P,P)X, 94MO(P,P)X, 96MO(P,P)X, 98MO(P,P)X,
100MO(P,P)X, 93NB(P,P)X, 106PD(P,P)X, AG(P,P)X);
PHQS=(ENGY-SPEC, ANGL-DSTRN, ENGY-SPEC'2');
/* '2' angular-integrated energy spectrum */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,210;
/* 2003-07-16 : Converted, Data converted to EXFOR E1320 and EXFOR
O0504. Numerical data are exchanged with author's one and data
which are obtained in the same work but not shown in the original
reference are added. */
ENR=NAT;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=0.5[1MG/CM**2'3';
/* '3' Detailed information on the target is listed in Table I of
[I.Kumabe et al., Phys. Rev. C35 (1987) 467]. */
BAC=SELF;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=VDGT;
INST-ACC=2JPNKYU;
INC-ENGY-LAB=18MEV;
POL-PRJ=0%;
DET-PARTCL=P;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(SBD'4',SI(LI)'5');
/* '4' Used as Delta E counter, 75 micro-meter */
/* '5' Used as E counter, 2500 micro-meter */
/* Experimental Method:
- Beam current integrated (Beam intensity was determined with a
current integrator connected to a Faraday cup and was also
monitored by a detector located at a fixed backward angle to the
beam.)
- Particle identification by 'E/Delta E' measurement (Signals of
protons were separated from those of other charged particles with
a particle identification circuit.)
RCT=94MO(P,P)X;
PHQ=ENGY-SPEC'432';
/* '432' angular-integrated energy spectrum */
ANL=(STATIST-MODEL'433',EXCITON-MODEL'434');
/* '433' Hauser-Feshbach Model [W.Hauser and H.Feshbach., Phys.
Rev. 87(1952)366]. */
/* '434' See [A.Iwamoto and K.Harada, Phys. Rev. C26(1982)1821]
for detail. */
/* Analysis:
- Integration of angular distribution (Experimental angular
distribution for each 0.2 MeV energy bin were fitted with a
series of Legendre polynomials up to l=4, and then the
polynomials were integrated.)
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,210;
INC-ENGY-LAB=18MEV;
SYS-ERR=X%'435';
/* '435' Uncertainties associated with the normalization was
estimated to be within 10% for each target. However, the
relative uncertainties of the cross sections for different
targets is believed to be less than 4%. */
NORM=/ Absolute cross sections were determined by normalizing the
experimental elastic cross sections to the optical model
predictions at forward angles. The normalization factors for
two sets of global optical model parameters were compared in
order to estimate the uncertainties involved in this method.
Optical model parameter [F.D. Becchetti, Jr. and G.W.
Greenlees, Phys. Rev. 182(1969)1190] were adopted. /;
EMT=P;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
ENGY-EMT-CM-MIN ENGY-EMT-CM-MAX DSIGMA/DE'436'
DELTA-DSIGMA/DE'436,437'
(MEV) (MEV) (MB/MEV) (MB/MEV)
3.0 3.2 37.862 +-0.272
3.2 3.4 44.041 +-0.287
3.4 3.6 48.750 +-0.297
3.6 3.8 52.264 +-0.304
3.8 4.0 56.644 +-0.312
4.0 4.2 57.508 +-0.313
4.2 4.4 60.825 +-0.319
4.4 4.6 63.085 +-0.323
4.6 4.8 64.138 +-0.325
4.8 5.0 64.980 +-0.327
5.0 5.2 66.050 +-0.329
5.2 5.4 64.188 +-0.325
5.4 5.6 63.702 +-0.324
5.6 5.8 62.595 +-0.322
5.8 6.0 61.682 +-0.320
6.0 6.2 60.158 +-0.316
6.2 6.4 58.402 +-0.313
6.4 6.6 55.279 +-0.306
6.6 6.8 52.351 +-0.300
6.8 7.0 49.897 +-0.295
7.0 7.2 47.833 +-0.291
7.2 7.4 45.121 +-0.285
7.4 7.6 41.731 +-0.278
7.6 7.8 39.443 +-0.275
7.8 8.0 36.813 +-0.271
8.0 8.2 33.868 +-0.265
8.2 8.4 32.009 +-0.260
8.4 8.6 29.636 +-0.254
8.6 8.8 28.334 +-0.251
8.8 9.0 25.850 +-0.244
9.0 9.2 24.757 +-0.241
9.2 9.4 22.816 +-0.234
9.4 9.6 20.718 +-0.226
9.6 9.8 19.783 +-0.222
9.8 10.0 18.826 +-0.216
10.0 10.2 17.554 +-0.209
10.2 10.4 16.782 +-0.202
10.4 10.6 16.601 +-0.199
10.6 10.8 15.299 +-0.191
10.8 11.0 14.942 +-0.187
11.0 11.2 14.665 +-0.184
11.2 11.4 14.150 +-0.180
11.4 11.6 13.556 +-0.176
11.6 11.8 12.777 +-0.171
11.8 12.0 12.634 +-0.181
12.0 12.2 12.319 +-0.178
12.2 12.4 11.308 +-0.172
12.4 12.6 11.218 +-0.169
12.6 12.8 10.598 +-0.164
12.8 13.0 10.516 +-0.174
13.0 13.2 11.130 +-0.213
13.2 13.4 9.674 +-0.335
13.4 13.6 10.711 +-0.785
13.6 13.8 10.417 +-0.666
13.8 14.0 11.496 +-1.784
\END;
/*===================================================================*/
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