/*===================================================================*/ /* NRDF D1620 Data No.6 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,6; D#=D1620; TITLE=/ Strength functions of deeply bound hole states in 111, 115, 119, 123Sn /; PURPOSE=/ To investigate the strength functions of deeply bound hole states in 111, 115, 119, 123Sn nuclei with high resolution (p,d) experiments at the bombaring energy of 50 MeV. /; ATH=(M.MATOBA'1', H.IJIRI'1', H.KAMETANI'1', I.KUMABE'2', M.HYAKUTAKE'2', N.KOORI'2', T.SAKAE'2', T.MAKI'3'); INST-ATH=(2JPNKYU'1', 2JPNKYU'2', 2JPNKIT'3'); /* '1' Graduate School of Engineering Sciences */ /* '2' Faculty of Engineering */ /* '3' School of Nursing and Technology */ REF=NP/A; VLP=456(1986)235; RCTS=(112SN(P,D)111SN, 124SN(P,D)123SN, 116SN(P,D)115SN, 120SN(P,D)119SN); PHQS=(ANGL-DSTRN, SPEC-FCTR'4'); /* '4' The spectroscopic factors as a function of the average excitation energies */ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,6; /* 2003-10-02 : Converted, Sr + Am + On. Converted to EXFOR E1620 RTY=PKUP; CHM=ELM; PHYS-FORM=SLD; BAC=SELF; POL-TGT=0%; ALGN-TGT=0%; ACC=CYC; INST-ACC=2JPNRCN; INC-ENGY-LAB=50.4MEV; POL-PRJ=0%; DET-PARTCL=D; COINC=NO; ANT-COINC=NO; DET-SYS=(MAG'5',X'6'); /* '5' Multi-magnet spectrograph RAIDEN [H.Ikegami et al., Nucl. Instr. Meth. 175(1980)33] */ /* '6' Focal plane detector system KYUSHU [M.Matoba et al., Nucl. Instr. Meth. 180(1981)419] */ /* 2006-12-19 : Altered, At. Re-digitized */ RCT=124SN(P,D)123SN; PHQ=ANGL-DSTRN; ENR=96.96%; THK-TGT=0.75MG/CM**2; ANL=DWBA; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,6; INC-ENGY-LAB=50.4MEV; SYS-ERR=<20%'7'; /* '7' The accuracy of the normalization of the absolute cross section is better than 20% */ NORM=/ The absolute (p,d) cross sections were obtained by normalization to proton elastic scattering measured under identical experimental conditions, except for magnetic field adjustment of the spectrograph. /; EXC-ENGY=5.75[5.76MEV; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (UB/SR) (UB/SR) 4.548E+00 8.833E+00 +-1.178E+00 7.470E+00 1.001E+01 +-1.464E+00 1.054E+01 1.058E+01 +-1.412E+00 1.361E+01 9.657E+00 +-1.233E+00 1.669E+01 1.069E+01 +-1.258E+00 1.960E+01 9.868E+00 +-1.161E+00 2.266E+01 7.089E+00 +-8.547E-01 2.588E+01 6.041E+00 +-7.713E-01 2.862E+01 2.981E+00 +-5.550E-01 3.293E+01 3.533E+00 +-5.882E-01 3.769E+01 3.736E+00 +-5.140E-01 4.288E+01 1.626E+00 +-4.157E-01 4.808E+01 8.985E-01 +-3.221E-01 \END; /*===================================================================*/ |