/*===================================================================*/
 /* NRDF D1673 Data No.5                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,5;
 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,5;
 /* 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%;
 ANL=DWBA'17';
 /* '17' Macroscopic distorted-wave calculations based on the Lane
         model using the code DWUCK-4 [P.D.Kuntz, The code DWUCK-4,
         unpublished.] */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,5;
 INC-ENGY-LAB=35MEV;
 TOT-ERR=<15%;
 EXC-ENGY=[1MEV;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (DEG) (MB/SR) (MB/SR)
 6.928E-01 8.797E+00 +-NEGLIGIBLE
 3.899E+00 8.594E+00 +-NEGLIGIBLE
 1.119E+01 6.070E+00 +-NEGLIGIBLE
 1.655E+01 3.969E+00 +-NEGLIGIBLE
 2.166E+01 2.637E+00 +-NEGLIGIBLE
 2.697E+01 2.641E+00 +-NEGLIGIBLE
 3.219E+01 2.677E+00 +-NEGLIGIBLE
 3.733E+01 2.870E+00 +-NEGLIGIBLE
 4.249E+01 2.360E+00 +-NEGLIGIBLE
 4.800E+01 1.941E+00 +-NEGLIGIBLE
 5.285E+01 1.259E+00 +-NEGLIGIBLE
 5.819E+01 1.052E+00 +-NEGLIGIBLE
 6.328E+01 7.639E-01 +-NEGLIGIBLE
 6.824E+01 8.492E-01 +-6.382E-02
 7.334E+01 6.215E-01 +-NEGLIGIBLE
 7.855E+01 6.909E-01 +-NEGLIGIBLE
 8.399E+01 4.723E-01 +-NEGLIGIBLE
 8.864E+01 4.259E-01 +-3.195E-02
 9.384E+01 2.719E-01 +-NEGLIGIBLE
 9.845E+01 2.917E-01 +-3.338E-02
 1.035E+02 2.445E-01 +-NEGLIGIBLE
 1.133E+02 1.569E-01 +-NEGLIGIBLE
 1.234E+02 1.318E-01 +-NEGLIGIBLE
 1.331E+02 1.103E-01 +-NEGLIGIBLE
 1.426E+02 8.973E-02 +-NEGLIGIBLE
 \END;
 /*===================================================================*/