/*===================================================================*/
 /* NRDF D1673 Data No.3                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,3;
 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,3;
 /* 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,3;
 INC-ENGY-LAB=35MEV;
 TOT-ERR=<15%;
 EXC-ENGY=0.0MEV;
 J-PTY=1+;
 ISOSPIN=0;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (DEG) (MB/SR) (MB/SR)
 6.261E-01 4.896E+00 +-NEGLIGIBLE
 3.958E+00 4.378E+00 +-NEGLIGIBLE
 1.124E+01 2.919E+00 +-NEGLIGIBLE
 1.634E+01 2.495E+00 +-NEGLIGIBLE
 2.219E+01 2.754E+00 +-NEGLIGIBLE
 2.730E+01 3.116E+00 +-NEGLIGIBLE
 3.220E+01 2.977E+00 +-NEGLIGIBLE
 3.772E+01 2.629E+00 +-NEGLIGIBLE
 4.302E+01 1.850E+00 +-NEGLIGIBLE
 4.801E+01 1.249E+00 +-NEGLIGIBLE
 5.310E+01 7.062E-01 +-NEGLIGIBLE
 5.861E+01 5.243E-01 +-NEGLIGIBLE
 6.382E+01 3.909E-01 +-NEGLIGIBLE
 6.892E+01 3.876E-01 +-3.221E-02
 7.392E+01 2.890E-01 +-NEGLIGIBLE
 7.892E+01 2.830E-01 +-NEGLIGIBLE
 8.412E+01 1.688E-01 +-NEGLIGIBLE
 8.858E+01 1.054E-01 +-1.195E-02
 9.368E+01 6.999E-02 +-5.093E-03
 9.888E+01 5.394E-02 +-1.404E-02
 1.040E+02 6.180E-02 +-NEGLIGIBLE
 1.136E+02 3.747E-02 +-2.686E-03
 1.237E+02 2.126E-02 +-1.928E-03
 1.330E+02 1.625E-02 +-1.412E-03
 1.425E+02 2.710E-02 +-2.761E-03
 \END;
 /*===================================================================*/