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| /*===================================================================*/
/* NRDF D1429 Data No.55 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,55;
D#=D1615;
TITLE=/Ground-state transition strengths of the (p,t) reactions for
nuclei with A=23-238/;
PURPOSE=/The systematic measurement of cross sections for
ground-to-ground two-neutron pickup reactions to nuclei over a
wider mass region and to look at the behaviour of the cross
sections with changing neutron number./;
ATH=(K.MIURA'1', Y.HIRATATE'1', T.SHOJI'1', T.SUEHIRO'1',
H.YAMAGUCHI'2', Y.ISHIZAKI'3');
INST-ATH=(2JPNTOI'1', 2JPNTKS'2', 2JPNINS'3');
/* '2' Faculty of General Education */
/* '3' Institute for Nuclear Study */
REF=NP/A;
VLP=436(1985)221;
RCTS=(23NA(P,T)21NA, 24MG(P,T)22MG, 26MG(P,T)24MG, 27AL(P,T)25AL,
28SI(P,T)26SI, 30SI(P,T)28SI, 35CL(P,T)33CL, 37CL(P,T)35CL,
40CA(P,T)38CA, 44CA(P,T)42CA, 46TI(P,T)44TI, 48TI(P,T)46TI,
50TI(P,T)48TI, 51V(P,T)49V, 54FE(P,T)52FE, 56FE(P,T)54FE,
58NI(P,T)56NI, 60NI(P,T)58NI, 62NI(P,T)60NI, 63CU(P,T)61CU,
64ZN(P,T)62ZN, 65CU(P,T)63CU, 66ZN(P,T)64ZN, 68ZN(P,T)66ZN,
76SE(P,T)74SE, 78SE(P,T)76SE, 80SE(P,T)78SE, 82SE(P,T)80SE,
90ZR(P,T)88ZR, 92MO(P,T)90MO, 92ZR(P,T)90ZR, 94ZR(P,T)92ZR,
96MO(P,T)94MO, 96ZR(P,T)94ZR, 98MO(P,T)96MO, 100MO(P,T)98MO,
102RU(P,T)100RU, 104PD(P,T)102PD, 104RU(P,T)102RU,
106PD(P,T)104PD, 108PD(P,T)106PD, 110PD(P,T)108PD,
112CD(P,T)110CD, 114CD(P,T)112CD, 115IN(P,T)113IN,
116CD(P,T)114CD, 118SN(P,T)116SN, 120SN(P,T)118SN,
122TE(P,T)120TE, 122SN(P,T)120SN, 124TE(P,T)122TE,
124SN(P,T)122SN, 126TE(P,T)124TE, 128TE(P,T)126TE,
130TE(P,T)128TE, 136BA(P,T)134BA, 138BA(P,T)136BA,
140CE(P,T)138CE, 142CE(P,T)140CE, 144ND(P,T)142ND,
146ND(P,T)144ND, 148ND(P,T)146ND, 150ND(P,T)148ND,
158GD(P,T)156GD, 160GD(P,T)158GD, 165HO(P,T)163HO,
168ER(P,T)166ER, 170ER(P,T)168ER, 172YB(P,T)170YB,
174YB(P,T)172YB, 176YB(P,T)174YB, 181TA(P,T)179TA,
184W(P,T)182W, 186W(P,T)184W, 188OS(P,T)186OS, 190OS(P,T)188OS,
191IR(P,T)189IR, 192OS(P,T)190OS, 193IR(P,T)191IR,
194PT(P,T)192PT, 196PT(P,T)194PT, 197AU(P,T)195AU,
198PT(P,T)196PT, 202HG(P,T)200HG, 204HG(P,T)202HG,
208PB(P,T)206PB, 209BI(P,T)207BI, 232TH(P,T)230TH,
238U(P,T)236U);
PHQS=ANGL-DSTRN;
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,55;
/* 2003-10-01 : Compiled */
RTY=PKUP;
PHQ=ANGL-DSTRN;
PHYS-FORM=SLD;
BAC=X'4';
/* '4' In the form of self-supporting foils and films evaporated
on mylar or aluminum backings. */
POL-TGT=0%;
ALGN-TGT=0%;
ACC=SYNCYC;
INST-ACC=2JPNINS;
INC-ENGY-LAB=51.9MEV;
POL-PRJ=0%;
DET-PARTCL=T;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(MAG'5',PROP-CNTR'6');
/* '5' Emitted tritons were analysed with a broad-range magnetic
spectrometer [K. Yagi, Nucl. Instr. 31(1964)173]. */
/* '6' Emitted tritons were detected with an array of 200
proportional counters [K. Yagi et al., Nucl. Instr.
52(1967)29]. */
ERS-DET=80[120KEV'7';
/* '7' Depending on the thickness of the targets used in the
experiment */
ANL=DWBA;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,55;
INC-ENGY-LAB=150MEV;
EMT-1=ALPHA;
/* A=38'22' */
/*@22@*/
THTL-1=-70DEG;
THTL-2=8DEG;
/*FIG.4-V*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
ENGY-EMT-LAB DATA1'31' DELTA-DATA1'31'
(MEV) (1/SR/MEV) (1/SR/MEV)
2.837E+00 2.033E-02 +0.000E+00-0.000E+00
4.006E+00 2.666E-02 +0.000E+00-0.000E+00
5.609E+00 2.486E-02 +0.000E+00-0.000E+00
7.091E+00 2.077E-02 +0.000E+00-0.000E+00
8.882E+00 1.634E-02 +0.000E+00-0.000E+00
1.073E+01 2.275E-02 +0.000E+00-0.000E+00
1.277E+01 1.450E-02 +0.000E+00-0.000E+00
1.455E+01 2.233E-02 +0.000E+00-0.000E+00
1.640E+01 1.847E-02 +0.000E+00-0.000E+00
1.844E+01 1.368E-02 +0.000E+00-0.000E+00
2.004E+01 1.672E-02 +0.000E+00-0.000E+00
2.122E+01 9.932E-03 +0.000E+00-0.000E+00
2.300E+01 1.813E-02 +0.000E+00-0.000E+00
2.473E+01 9.084E-03 +2.241E-03-1.725E-03
2.578E+01 1.025E-02 +2.529E-03-1.341E-03
2.732E+01 9.091E-03 +2.473E-03-1.576E-03
2.855E+01 1.254E-02 +3.411E-03-2.070E-03
2.973E+01 8.397E-03 +2.179E-03-1.927E-03
3.189E+01 6.035E-03 +1.797E-03-1.146E-03
\END;
/*===================================================================*/
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