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| /*===================================================================*/
/* NRDF D1845 Data No.7 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,7;
D#=D1845;
TITLE=/Feshbach-Kerman-Koonin model analysis of preequilibrium (p,p')
and (p,n) reactions at 12 to 26 MeV/;
PURPOSE=/To investigate preequilibrium nucleon emission in the low
incident energy region below 30 MeV/;
ATH=(Y.WATANABE'1', A.AOTO'1', H.KASHIMOTO'1', S.CHIBA'2',
T.FUKAHORI'2', K.HASEGAWA'2', M.MIZUMOTO'2', S.MEIGO'2',
M.SUGIMOTO'2', Y.YAMANOUTI'2', N.KOORI'3', M.B.CHADWICK'4',
P.E.HODGSON'5');
INST-ATH=(2JPNKYU'1', 2JPNJAE'2', 2JPNTKS'3', 1USALRL'4', 2UK OXF'5');
/* '1' Department of Energy Conversion Engineering */
/* '3' Faculty of Integrated Arts and Sciences */
/* '4' Nuclear Data Group */
/* '5' Nuclear Physics Laboratory, Physics Department */
REF=PR/C;
VLP=51(1995)1891;
RCTS=(98MO(P,P)X, 106PD(P,P)X);
PHQS=ENGY-SPEC;
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,7;
/* 2003-11-13 : Converted, Data converted from EXFOR O0558 */
CHM=ELM;
PHYS-FORM=SLD'6';
/* '6' metalic foils */
BAC=SELF;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=VDGT;
INST-ACC=2JPNJAE;
BEAM-INTNSTY=XNA'7';
/* '7' Beam current was adjusted in a range from about several
tens of nA to about 300 nA in accordance with the detector
angle. */
POL-PRJ=0%;
DET-PARTCL=P;
COINC=NO;
ANT-COINC=NO;
DET-SYS=SBD'8';
/* '8' as Delta E-E counter to detect all emitted charged
particles separately and suppress background events due to
gamma-rays. */
ANL=X'9';
/* '9' Multistep direct (MSD) and multistep-compound (MSC)
reaction models of Feshbach, Kerman, and Koonin (FKK) using the
FKK-GNASH code [M.B.Chadwick and P.G.Young, Phys. Rev. C47
(1993) 2255] */
/* Experimental Method:
- Particle identification by 'E/Delta E' measurement (To detect
all emitted charged particles separately and suppress background
events due to gamma-rays)
- Beam current integrated (Beam intensity was monitored by means
of a current integrator connected to a Faraday cup and the beam
current was adjusted in a range from about several tens of nA to
about 300 nA in accordance with the detector angle.)
RCT=98MO(P,P)X;
PHQ=ENGY-SPEC;
ENR=97.1%;
THK-TGT=0.45MG/CM**2;
INC-ENGY-LAB=25.6MEV;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,7;
INC-ENGY-LAB=25.6MEV;
SYS-ERR=<8%'38';
/* '38' Absolute uncertainty involved in the normalization */
NORM=/ Elastic cross sections at small angles are normalized to the
optical model prediction /;
EMT=P;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
ENGY-EMT-LAB DELTA-DSIGMA/DE
(MEV) (MB/MEV)
\END;
/*===================================================================*/
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