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| /*===================================================================*/
/* NRDF D0296 Data No.8 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,8;
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,8;
/* 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] */
RCT=116SN(P,D)115SN;
PHQ=SPEC-FCTR'15';
/* '15' The spectroscopic factors as a function of the average
excitation energies */
ENR=95.60%;
THK-TGT=0.7MG/CM**2;
ANL=X'16';
/* '16' Theoretical predictions by Soloviev et al. [V.G.Soloviev
et al.,Nucl.Phys.A342(1980)261;N.D.Thao et al.,
Yadr.Phys.34(1983)43] */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,8;
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. /;
SYS-ERR=([20%'17',X%'18');
/* '17' The errors of the deduced spectroscopic factors are
estimated to be about 20% due mainly to the absolute
normalization procedure. */
/* '18' The errors of the excitation energies and spreading
widths may be small because the error of the absolute cross
section only weakly affects the final results. */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY'19' SPEC-FCTR WDTH'20' L'21'
(MEV) (NODIM) (MEV) (NODIM)
5.31 5.13 1.36 4
5.67 1.97 3.35=170.3DEG;
/*FIG.1-(H)*/
/* D296 FIG 1-(H) */
/* SER#= 8 */
/* XSCALE=LINEAR YSCALE=LINEAR */
/* XMAX= 1.45099993E+01 YMAX= 4.49999988E-01 */
/* XMIN= 1.43699999E+01 YMIN= 2.50000000E-01 */
/* FOLLOWING DATA ARE TAKEN FROM GRAPH */
INC-ENGY-LAB POL DELTA-POL
(MEV) (NODIM) (NODIM)
14.39 3.51E-01 1.90E-02
14.40 3.24E-01 1.90E-02
14.41 3.92E-01 2.14E-02
14.42 3.62E-01 1.78E-02
14.43 3.85E-01 1.78E-02
14.44 3.74E-01 1.78E-02
14.45 4.01E-01 2.02E-02
14.46 3.98E-01 1.42E-02
14.47 4.02E-01 2.26E-02
14.48 3.88E-01 1.90E-02
14.49 3.98E-01 1.54E-02
\END;
/*===================================================================*/
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