/*===================================================================*/ /* NRDF D1620 Data No.2 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,2; 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,2; /* 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=112SN(P,D)111SN; PHQ=ANGL-DSTRN; ENR=80.04%; THK-TGT=0.9MG/CM**2; ANL=DWBA; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,2; 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=4.35[4.36MEV; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (UB/SR) (UB/SR) 5.861E+00 7.657E+00 +-1.709E+00 8.366E+00 1.267E+01 +-1.374E+00 1.138E+01 8.756E+00 +-1.635E+00 1.460E+01 9.688E+00 +-9.511E-01 1.748E+01 7.686E+00 +-1.141E+00 2.069E+01 7.758E+00 +-1.151E+00 2.375E+01 8.294E+00 +-9.029E-01 2.676E+01 5.538E+00 +-7.679E-01 2.992E+01 3.655E+00 +-5.065E-01 3.388E+01 3.140E+00 +-4.968E-01 3.896E+01 4.219E+00 +-5.430E-01 4.406E+01 1.861E+00 +-3.756E-01 4.921E+01 1.199E+00 +-3.195E-01 \END; /*===================================================================*/ |