|
| /*===================================================================*/
/* NRDF D1194 Data No.5 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,5;
D#=D1194;
TITLE=/ Optical model and folding model potentials for elastic
scattering of 56 MeV polarized deuterons /;
ATH=(N.MATSUOKA'1', H.SAKAI'1', T.SAITO'1', K.HOSONO'1', M.KONDO'1',
H.ITO'1', K.HATANAKA'2', T.ICHIHARA'2', A.OKIHANA'3', K.IMAI'4',
K.NISIMURA'5');
INST-ATH=(2JPNRCN'1', 2JPNIPC'2', 2JPNKUE'3', 2JPNKTO'4',
2JPNINS'5');
/* '3' Department of Physics */
/* '4' Department of Physics */
REF=NP/A;
VLP=455(1986)413;
RCTS=(12C(D,D)12C, 16O(D,D)16O, 40CA(D,D)40CA, 58NI(D,D)58NI,
90ZR(D,D)90ZR, 118SN(D,D)118SN, 144SM(D,D)144SM,
208PB(D,D)208PB);
PHQS=(ANGL-DSTRN, VCTR-ANALPW, TNSR-ANALPW, OPT-POTL-PARA);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,5;
/* 2007-01-31 : Converted, N.Otuka. Converted to EXFOR E1194 */
RTY=ELA-SCATT;
ENR=X%'6';
/* '6' Natural for 12C and 40Ca and enriched (96.7-99.8%) for
58Ni, 90Zr, 118Sn, 144Sm and 208Pb */
CHM=ELM;
THK-TGT=1.88[16.4MG/CM**2'7';
/* '7' 1140 Torr for 16O */
BAC=SELF;
ACC=CYC'8';
/* '8' Isochronous cyclotron, AVF cyclotron */
INST-ACC=2JPNRCN;
INC-ENGY-LAB-RANGE=56MEV;
BEAM-INTNSTY=10[200NA;
POL-PRJ=80[85%;
ION-SOURCE=/ Atomic beam source /;
DET-PARTCL=D;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(CNTR-TLSCP'9',SI'9',NAI'9',EDE'10');
/* '9' To detect scattered particle */
/* '10' E and DE signal by Si and NaI detector */
ERS-DET=600KEV;
ANL=OPT-MODEL;
/* 2007-02-20 : Altered, At. Re-digitized */
RCT=90ZR(D,D)90ZR;
PHQ=ANGL-DSTRN;
PHYS-FORM=SLD;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,5;
INC-ENGY-LAB=56MEV;
SYS-ERR=8%'15';
/* '15' Uncertainty in absolute normalization, mainly due to
target thickness */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC RUTH-RATIO
(DEG) (NODIM)
1.215E+01 2.350E-01
1.450E+01 2.144E-01
1.617E+01 4.529E-01
1.858E+01 6.215E-01
2.052E+01 4.950E-01
2.197E+01 1.783E-01
2.264E+01 6.426E-02
2.448E+01 2.066E-02
2.498E+01 5.235E-02
2.588E+01 1.387E-01
2.835E+01 3.065E-01
3.072E+01 3.353E-01
3.262E+01 2.035E-01
3.449E+01 7.845E-02
3.720E+01 5.330E-02
3.924E+01 9.387E-02
4.124E+01 1.150E-01
4.237E+01 7.644E-02
4.391E+01 5.562E-02
4.585E+01 4.636E-02
4.666E+01 5.432E-02
4.710E+01 7.985E-02
4.916E+01 1.686E-01
5.117E+01 2.367E-01
5.354E+01 2.532E-01
5.588E+01 1.971E-01
5.744E+01 1.720E-01
6.020E+01 1.679E-01
6.180E+01 2.153E-01
6.420E+01 2.760E-01
6.696E+01 2.696E-01
6.930E+01 2.298E-01
7.164E+01 1.915E-01
7.439E+01 1.708E-01
7.677E+01 1.826E-01
7.952E+01 1.824E-01
8.228E+01 1.702E-01
8.422E+01 1.419E-01
8.657E+01 1.237E-01
8.971E+01 1.129E-01
9.247E+01 1.078E-01
\END;
/*===================================================================*/
|