|
| /*===================================================================*/
/* NRDF D1620 Data No.3 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,3;
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,3;
/* 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,3;
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=4.95[4.96MEV;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (UB/SR) (UB/SR)
5.981E+00 1.874E+01 +-1.629E+00
8.936E+00 2.880E+01 +-2.504E+00
1.200E+01 3.008E+01 +-2.495E+00
1.499E+01 1.780E+01 +-1.729E+00
1.805E+01 1.776E+01 +-1.908E+00
2.094E+01 1.619E+01 +-1.574E+00
2.416E+01 1.652E+01 +-1.368E+00
2.719E+01 1.406E+01 +-9.942E-01
3.020E+01 9.429E+00 +-8.205E-01
3.452E+01 3.497E+00 +-5.145E-01
3.944E+01 4.476E+00 +-5.265E-01
4.461E+01 3.636E+00 +-4.994E-01
4.958E+01 1.939E+00 +-3.767E-01
\END;
/*===================================================================*/
|