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| /*===================================================================*/
/* NRDF D1673 Data No.8 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,8;
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,8;
/* 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code DWBA-74 [R.Schaeffer and J.Raynal, unpublished.]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,8;
INC-ENGY-LAB=35MEV;
TOT-ERR=<15%;
EXC-ENGY=2.100MEV;
J-PTY=2-;
ISOSPIN=0;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (MB/SR) (MB/SR)
1.536E-01 2.022E-01 +-4.179E-02
3.378E+00 1.594E-01 +-3.829E-02
1.084E+01 1.179E-01 +-2.051E-02
1.595E+01 2.026E-01 +-3.093E-02
2.144E+01 1.937E-01 +-2.485E-02
3.174E+01 1.957E-01 +-NEGLIGIBLE
3.744E+01 2.674E-01 +-2.972E-02
4.262E+01 1.748E-01 +-NEGLIGIBLE
4.731E+01 1.988E-01 +-2.311E-02
5.273E+01 1.143E-01 +-8.702E-03
6.316E+01 9.274E-02 +-1.173E-02
7.352E+01 4.737E-02 +-6.727E-03
8.332E+01 1.996E-02 +-3.687E-03
9.330E+01 1.491E-02 +-2.831E-03
1.036E+02 1.295E-02 +-1.908E-03
1.133E+02 7.836E-03 +-1.576E-03
1.231E+02 7.530E-03 +-1.391E-03
1.326E+02 9.744E-03 +-1.486E-03
1.420E+02 5.762E-03 +-1.730E-03
\END;
/*===================================================================*/
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