|
| /*===================================================================*/
/* NRDF D1492 Data No.5 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,5;
D#=D1492;
TITLE=/DISAPPEARANCE OF FLOW AS A FUNCTION OF IMPACT PARAMETER AND
ENERGY IN NUCLEUS-NUCLEUS COLLISIONS/;
PURPOSE=/TO DETERMINE NN-CROSS SECTION IN MEDIUM AND NUCLEAR
COMPRESSIBILITY/;
ATH=(J.P.SULLIVAN'1',J.PETER'1',D.CUSSOL'1',G.BIZARD'1',R.BROU'1',
M.LOUVEL'1',J.P.PATRY'1',R.REGIMBART'1',J.C.STECKMEYER'1',
B.TAMAIN'1',E.CREMA'2',H.DOUBRE'2',K.HAGEL'2',G.M.JIN'2,3',
A.PEGHAIRE'2',F.SAINT-LAURENT'2',Y.CASSAGNOU'4',R.LEGRAIN'4',
C.LEBRUN'5',E.ROSATO'6',R.MACGRATH'7',S.C.JEONG'8',S.M.LEE'8',
Y.NAGASHIMA'8',T.NAKAGAWA'8',M.OGIHARA'8',J.KASAGI'9',
T.MOTOBAYASHI'1,2,10');
INST-ATH=(2FR FR '1',2FR FR '2',2CHPIMP'3',2FR SAC'4',2FR FR '5',
2ITYNAP'6',1USASTB'7',2JPNTSU'8',2JPNINS'9',2JPNRIK'10');
/*@3@*/
/*@4@*/
/*@6@*/
REF=PL/B;
VLP=249(1990)8;
RCTS=(27AL(40AR,X),27AL(36AR,X));
PHQS=(X'8');
/*@8@*/
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,5;
RTY=(INEL-SCATT);
INST-ACC=2FR FR '4';
/*@4@*/
DET-SYS=(TOF,X'9');
/*@9@*/
ANT-COINC=NO;
ANL=(X'10');
/*@10@*/
INC-ENGY-LAB=(65MEV/A);
CHRG-INC-ION=40;
PHQ=(X'8');
/*@8@*/
DET-PARTCL=(D);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,5;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
DATA3'17' DELTA-DATA3'17' DATA4'8' DELTA-DATA4'8'
(FM) (FM) (MEV/C) (MEV/C)
5.717E-01 +1.191E+00-9.447E-01 8.104E+00 +1.938E+00-2.364E+00
2.790E+00 +1.102E+00-1.349E+00 1.234E+01 +1.909E+00-2.144E+00
5.911E+00 +1.506E+00-1.642E+00 1.732E+01 +2.907E+00-2.996E+00
1.008E+01 +2.046E+00-2.136E+00 2.100E+01 +3.069E+00-2.922E+00
1.447E+01 +1.506E+00-2.001E+00 2.701E+01 +3.127E+00-3.084E+00
1.918E+01 +2.766E+00-2.563E+00 3.254E+01 +3.260E+00-2.717E+00
2.491E+01 +2.900E+00-2.585E+00 3.049E+01 +2.937E+00-3.054E+00
3.155E+01 +2.654E+00-2.968E+00 2.632E+01 +3.362E+00-2.908E+00
\END;
/*===================================================================*/
|