|
| /*===================================================================*/
/* NRDF D1664 Data No.11 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,11;
D#=D1664;
TITLE=/GAMOW-TELLER STRENGTH OF 90NB IN THE CONTINUUM STUDIED VIA
MULTIPOLE DECOMPOSITION ANALYSIS OF THE 90ZR(P,N) REACTION AT
295 MEV/;
ATH=(T.WAKASA'1,4',H.SAKAI'1',H.OKAMURA'1',S.FUJITA'1,5',S.ISHIDA'1,6',
N.SAKAMOTO'1,6',T.UESAKA'1',Y.SATOU'1',M.B.GREENFIELD'2',
K.HATANAKA'3');
INST-ATH=(2JPNTOK'1',2JPNICU'2',2JPNRCN'3');
/*@34@*/
/*@35@*/
/*@36@*/
REF=PR/C;
VLP=55(1997)2909;
RCTS=(90ZR(P,N)90NB);
PHQS=(POL-TRNSF,DSIGMA/DOMEGA/DE,ANGL-DSTRN,EXC-ENGY);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,11;
/* 2006-02-27 N.OTUKA 2JPNJPN -> 2JPNICU in BIB,1[11 */
RCT=90ZR(P,N)90NB;
RTY=(POL-RCT);
ENR=X;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=112MG/CM**2;
BAC=SELF;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=(CYC);
INST-ACC=2JPNRCN;
INC-ENGY-LAB=(295MEV);
DELTA-INC-ENGY-LAB=1000KEV;
POL-PRJ=73%;
DET-PARTCL=(N);
COINC=NO;
ANT-COINC=NO;
DET-SYS=(NPOL2'21');/*@31@*/
SOLID-ANGL=XMSR;
ERS-DET=1900KEV;
MONTR-RCT=/1H(P(POL),P)1H/;
ANL=(DWIA,X'22');/*@32@*/
PHQ=(ANGL-DSTRN,DSIGMA/DOMEGA/DE);
PHQ=(EXC-ENGY,DSIGMA/DOMEGA/DE);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,11;
INC-ENGY-LAB=295MEV;
EMT-1=N;
RSD=90NB;
THTL-1=12.3DEG;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
EXC-ENGY DSIGMA/DOMEGA/DE
(MEV) (MB/SR/MEV)
-5.496E+00 2.251E-01
-3.038E+00 1.931E-01
-2.081E+00 1.361E-01
-9.954E-01 2.334E-01
3.870E-01 2.740E-01
1.304E+00 5.722E-01
2.211E+00 6.799E-01
3.523E+00 5.455E-01
5.318E+00 4.624E-01
5.743E+00 5.549E-01
7.012E+00 6.985E-01
8.455E+00 7.545E-01
8.699E+00 8.316E-01
1.081E+01 9.594E-01
1.182E+01 8.354E-01
1.380E+01 8.603E-01
1.243E+01 1.072E+00
1.442E+01 1.220E+00
1.520E+01 1.199E+00
1.605E+01 1.312E+00
1.696E+01 1.554E+00
1.780E+01 1.461E+00
1.966E+01 1.584E+00
2.026E+01 1.589E+00
2.128E+01 1.470E+00
2.279E+01 1.773E+00
2.261E+01 1.644E+00
2.435E+01 1.695E+00
2.605E+01 1.972E+00
2.676E+01 1.848E+00
2.826E+01 1.843E+00
2.934E+01 1.919E+00
3.090E+01 1.944E+00
3.259E+01 2.021E+00
3.469E+01 2.030E+00
3.530E+01 2.184E+00
3.710E+01 2.230E+00
3.825E+01 2.353E+00
3.974E+01 2.208E+00
4.070E+01 2.254E+00
4.149E+01 2.331E+00
4.256E+01 2.238E+00
4.394E+01 2.181E+00
4.610E+01 2.159E+00
4.723E+01 2.102E+00
4.849E+01 2.107E+00
4.963E+01 2.101E+00
5.052E+01 1.905E+00
5.203E+01 2.049E+00
5.347E+01 1.986E+00
5.448E+01 1.919E+00
5.586E+01 1.877E+00
5.652E+01 1.805E+00
5.922E+01 1.840E+00
5.975E+01 1.731E+00
6.071E+01 1.659E+00
6.161E+01 1.725E+00
6.215E+01 1.782E+00
6.275E+01 1.725E+00
6.347E+01 1.699E+00
6.425E+01 1.642E+00
6.466E+01 1.606E+00
6.550E+01 1.543E+00
6.670E+01 1.569E+00
6.736E+01 1.486E+00
6.855E+01 1.434E+00
\END;
/*===================================================================*/
|