/*===================================================================*/ /* NRDF D1620 Data No.4 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,4; 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,4; /* 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,4; 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=4.55[4.56MEV; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (UB/SR) (UB/SR) 3.153E+00 8.856E+00 +-1.135E+00 5.913E+00 7.895E+00 +-1.089E+00 9.142E+00 8.645E+00 +-1.108E+00 1.235E+01 5.726E+00 +-9.567E-01 1.542E+01 4.659E+00 +-9.516E-01 1.833E+01 4.818E+00 +-9.403E-01 2.125E+01 3.966E+00 +-7.000E-01 2.446E+01 3.226E+00 +-6.296E-01 2.752E+01 2.065E+00 +-4.715E-01 3.150E+01 1.337E+00 +-4.093E-01 3.642E+01 1.717E+00 +-3.968E-01 4.133E+01 1.445E+00 +-3.590E-01 4.653E+01 8.632E-01 +-3.040E-01 \END; /*===================================================================*/ |