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| /*===================================================================*/
/* NRDF D1673 Data No.7 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,7;
D#=D1673;
TITLE=/ The 17,18O(p,n)17,18F reaction at Ep=35 MeV /;
PURPOSE=/ To report a high-resolution study of the 17,18O(p,n)17,18F
reactions at Ep=35 MeV and the results of distorted-wave
analysis based on shell-model wave functions. /;
ATH=(M.OURA'1', H.ORIHARA'1', M.HOSAKA'1', G.C.JON'1', A.TERAKAWA'1',
K.ISHII'1', A.NARITA'2', K.HOSOMI'2', T.NAKAGAWA'2', K.MIURA'3',
H.OHNUMA'4', T.NIIZEKI'4', D.DEHNHARD'5');
INST-ATH=(2JPNTOH'1', 2JPNTOH'2', 2JPNTOI'3', 2JPNTIT'4',
1USAMIN'5');
/* '1' Cyclotron and Radioisotope Center */
/* '2' Department of Physics */
/* '4' Department of Physics */
/* '5' Department of Physics and Astronomy */
REF=NP/A;
VLP=586(1995)20;
RCTS=(17O(P,N)17F, 18O(P,N)18F);
PHQS=ANGL-DSTRN;
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,7;
/* 2003-09-02 : Converted, Sr + Am + On. Data converted to EXFOR
E1673 */
RTY=RRG-RCT'6';
/* '6' charge exchange reaction */
PHQ=ANGL-DSTRN;
CHM=ELM;
PHYS-FORM=GAS;
THK-TGT=[1MG/CM**2'7';
/* '7' The effective target thicknesses were of the order of 1
mg/cm2. */
BAC=X'8';
/* '8' The window material was metallic calcium foil for the
drum-shaped cell, while it was Havar foil for the cylndrical
cell, their thicknesses being about 10 mg/cm2. */
THK-BAC=[10MG/CM**2;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=CYC'9';
/* '9' Isochronous cyclotron, AVF cyclotron */
INST-ACC=2JPNTOH'10';
/* '10' Cyclotron and Radioisotope Center */
INC-ENGY-LAB=35MEV;
POL-PRJ=0%;
DET-PARTCL=N;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(SCT'11',TOF);
/* '11' NE213 scintillator. The detector efficiencies were
obtained from Monte Carlo calculations for monoenergetic
neutrons with En=<34MeV. Absolute detector efficiencies were
also measured by counting neutrons from the 7Li(p,n)7Be
reaction and comparing its yield with the absolute neutron
fluence determined by activation. */
ERS-DET=174KEV'12';
/* '12' for the most energetic neutrons */
ANL=DWBA'13';
/* '13' The distorted-wave results calculated by the computer
code DWBA-74 [R.Schaeffer and J.Raynal, unpublished.] */
/* 2006-10-31 : Altered, Mh. Re-digitized */
RCT=18O(P,N)18F;
ENR=98.7%;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,7;
INC-ENGY-LAB=35MEV;
TOT-ERR=<15%;
EXC-ENGY=4.652MEV;
J-PTY=4+;
ISOSPIN=1;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (MB/SR) (MB/SR)
8.999E-01 1.954E-01 +-2.301E-02
4.028E+00 2.101E-01 +-1.971E-02
1.190E+01 2.092E-01 +-2.564E-02
1.686E+01 1.598E-01 +-3.148E-02
2.247E+01 1.763E-01 +-3.204E-02
2.765E+01 1.682E-01 +-1.504E-02
3.336E+01 1.448E-01 +-NEGLIGIBLE
3.833E+01 1.778E-01 +-1.925E-02
4.329E+01 1.584E-01 +-NEGLIGIBLE
4.836E+01 2.410E-01 +-2.267E-02
5.407E+01 1.598E-01 +-NEGLIGIBLE
5.914E+01 2.319E-01 +-1.965E-02
6.432E+01 1.442E-01 +-NEGLIGIBLE
6.928E+01 1.667E-01 +-2.124E-02
7.424E+01 1.149E-01 +-NEGLIGIBLE
7.899E+01 1.194E-01 +-1.123E-02
8.470E+01 7.455E-02 +-5.629E-03
8.923E+01 3.262E-02 +-1.452E-02
9.409E+01 3.207E-02 +-2.718E-03
1.043E+02 4.536E-02 +-3.425E-03
1.145E+02 5.791E-02 +-NEGLIGIBLE
1.240E+02 5.136E-02 +-3.401E-03
1.335E+02 4.058E-02 +-3.065E-03
1.432E+02 2.845E-02 +-2.888E-03
\END;
/*===================================================================*/
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