/*===================================================================*/ /* 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*/ ANL=DWBA'13'; /* '13' The distorted-wave results calculated by the computer code DWBA-74 [R.Schaeffer and J.Raynal, unpublished.]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; /*===================================================================*/ |