|
| /*===================================================================*/
/* NRDF D1380 Data No.2 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,2;
D#=D1380;
TITLE=/ON THE MOMENTUM DISTRIBUTIONS OF FRAGMENTS OF 11LI AND 11BE/;
ATH=(I.TANIHATA'1');
INST-ATH=(2JPNIPC'1');
REF=X'12';
/*@12@*/
VLP=X;
RCTS=(11LI(D,9LI)X,11LI(C,9LI)X);
PHQS=(MOM-DSTRN);
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,2;
RCT=11LI(C,9LI)X;
INST-ACC=1USALBL;
INC-ENGY-LAB=(790MEV/A,800MEV/A);
PHQ=(MOM-DSTRN);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,2;
INC-ENGY-LAB=800MEV/A;
/*FIG.2*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
DATA'31' COUNTS DELTA-COUNTS
(MEV/C) (NODIM) (NODIM)
-3.879E+02 -4.044E+00 +0.000E+00-0.000E+00
-3.714E+02 -8.251E+00 +0.000E+00-0.000E+00
-3.498E+02 -2.997E+00 +0.000E+00-0.000E+00
-3.318E+02 -2.874E+00 +0.000E+00-0.000E+00
-3.156E+02 -7.982E-01 +0.000E+00-0.000E+00
-3.008E+02 2.446E+00 +0.000E+00-0.000E+00
-2.804E+02 -5.564E-01 +0.000E+00-0.000E+00
-2.579E+02 8.632E+00 +0.000E+00-0.000E+00
-2.404E+02 1.032E+01 +0.000E+00-0.000E+00
-2.242E+02 7.293E+00 +0.000E+00-0.000E+00
-2.089E+02 1.172E+01 +0.000E+00-0.000E+00
-1.876E+02 3.779E+01 +0.000E+00-0.000E+00
-1.685E+02 4.381E+01 +0.000E+00-0.000E+00
-1.486E+02 6.712E+01 +0.000E+00-0.000E+00
-1.342E+02 8.882E+01 +9.430E+00-8.637E+00
-1.197E+02 1.325E+02 +1.180E+01-1.021E+01
-1.018E+02 1.531E+02 +1.336E+01-1.609E+01
-8.004E+01 2.687E+02 +2.042E+01-1.806E+01
-5.820E+01 3.552E+02 +1.886E+01-2.514E+01
-4.065E+01 5.093E+02 +2.946E+01-2.947E+01
-2.530E+01 7.604E+02 +3.260E+01-3.497E+01
-9.861E+00 8.858E+02 +4.165E+01-4.477E+01
8.586E+00 9.739E+02 +4.989E+01-3.888E+01
2.989E+01 8.048E+02 +3.654E+01-3.535E+01
4.906E+01 5.237E+02 +3.496E+01-2.945E+01
6.631E+01 4.213E+02 +2.513E+01-2.240E+01
7.791E+01 2.517E+02 +1.885E+01-2.161E+01
9.755E+01 1.646E+02 +1.570E+01-1.492E+01
1.202E+02 1.306E+02 +1.060E+01-1.217E+01
1.392E+02 1.096E+02 +7.859E+00-1.335E+01
1.565E+02 6.922E+01 +1.021E+01-1.139E+01
1.724E+02 3.516E+01 +0.000E+00-0.000E+00
1.886E+02 2.309E+01 +0.000E+00-0.000E+00
2.081E+02 6.729E+00 +0.000E+00-0.000E+00
2.295E+02 -9.794E-01 +0.000E+00-0.000E+00
2.501E+02 -8.377E-01 +0.000E+00-0.000E+00
2.641E+02 4.373E-01 +0.000E+00-0.000E+00
2.792E+02 1.479E-01 +0.000E+00-0.000E+00
2.981E+02 -4.042E+00 +0.000E+00-0.000E+00
3.163E+02 -3.525E+00 +0.000E+00-0.000E+00
3.357E+02 -1.820E+00 +0.000E+00-0.000E+00
3.529E+02 2.620E-01 +0.000E+00-0.000E+00
3.660E+02 -4.335E-01 +0.000E+00-0.000E+00
3.840E+02 -4.631E+00 +0.000E+00-0.000E+00
\END;
/*===================================================================*/
|