|
| /*===================================================================*/
/* NRDF D1502 Data No.7 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,7;
D#=D1502;
TITLE=/COMPONENTS OF COLLECTIVE FLOW AND AZIMUTHAL DISTRIBUTIONS IN
40AR+27AL AND 40AR+58NI COLLISIONS BELOW 85 MEV/U/;
PURPOSE=/TO COMPLETELY UNDERSTAND THE DYNAMICS OF THE HEAVY-ION
REACTIONS AND STUDY THE NUCLEAR MATTER,IMCOMPRESSIBILITY
MODULUS/;
ATH=(W.Q.SHEN'1',J.PETER'1',G.BIZARD'1',R.BROU'1',D.CUSSOL'1',
J.P.PATRY'1',R.REGIMBART'1',J.C.STECKMEYER'1',J.P.SULLIVAN'1',
B.TAMAIN'1',E.CREMA'2',H.DOUBRE'2',K.HAGEL'2',G.M.JIM'2,7',
A.PEGHAIRE'2',F.SAINT-LAURENT'2',Y.CASSAGNOU'3',R.LEGRAIN'3',
C.LEBRUN'4',E.ROSATO'5',R.MACGRATH'6',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', 2FR SAC'3',2FR FR '4',2ITYNAP'5',
1USASTB'6',3CHPIMP'7', 2JPNTSU'8',2JPNTOK'9',2JPNYOK'10');
/*@1@*/
/*@2@*/
/*@4@*/
REF=NP/A;
VLP=551(1993)333;
RCTS=(27AL(40AR,X)X,58NI(40AR,X)X);
PHQS=(HEAVY-ION-RCT);
INST-ACC=2FR FR '4';
/*@4@*/
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,7;
RTY=(INEL-SCATT);
POL-TGT=(0%);
ALGN-TGT=(0%);
DET-SYS=(X'17',TOF);
/*@17@*/
ANT-COINC=NO;
ANL=(X'18');
/*@18@*/
POL-TGT=(0%);
ALGN-TGT=(0%);
POL-PRJ=(0%);
BAC=SELF;
RCT=(27AL(40AR,X)X);
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,7;
INC-ENGY-LAB=(45MEV/A);
/* OTHERS=('10'): */
/*@10@*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
DATA1'13' DELTA-DATA1 DATA2'14,12' DELTA-DATA2'12'
(NODIM) (NODIM) (UNIT) (UNIT)
-9.740E-01 +2.433E-02-1.787E-02 1.671E+02 +1.641E+00-1.324E+00
-8.986E-01 +1.539E-02-2.299E-02 1.680E+02 +2.019E+00-1.640E+00
-8.270E-01 +2.562E-02-2.300E-02 1.684E+02 +1.325E+00-1.703E+00
-7.375E-01 +2.689E-02-3.839E-02 1.705E+02 +1.262E+00-1.766E+00
-6.376E-01 +2.047E-02-3.067E-02 1.695E+02 +1.639E+00-1.767E+00
-5.635E-01 +3.712E-02-2.173E-02 1.708E+02 +1.325E+00-1.766E+00
-4.893E-01 +1.925E-02-3.064E-02 1.715E+02 +1.261E+00-2.208E+00
-4.190E-01 +2.050E-02-3.072E-02 1.724E+02 +1.704E+00-1.956E+00
-3.459E-01 +2.304E-02-3.711E-02 1.707E+02 +1.514E+00-1.451E+00
-2.629E-01 +4.608E-02-3.323E-02 1.725E+02 +8.200E-01-1.451E+00
-1.618E-01 +1.792E-02-3.835E-02 1.730E+02 +1.577E+00-2.082E+00
-7.362E-02 +2.306E-02-5.499E-02 1.751E+02 +1.072E+00-1.830E+00
-7.225E-04 +2.813E-02-2.557E-02 1.758E+02 +1.136E+00-2.082E+00
7.613E-02 +2.685E-02-2.689E-02 1.742E+02 +1.514E+00-1.704E+00
1.515E-01 +2.434E-02-3.579E-02 1.759E+02 +1.451E+00-2.209E+00
2.231E-01 +3.072E-02-2.814E-02 1.787E+02 +1.326E+00-1.325E+00
3.038E-01 +5.500E-02-3.325E-02 1.764E+02 +2.271E+00-8.820E-01
4.100E-01 +2.687E-02-3.454E-02 1.769E+02 +8.210E-01-1.703E+00
4.920E-01 +3.199E-02-2.812E-02 1.750E+02 +1.262E+00-1.767E+00
5.647E-01 +2.304E-02-1.277E-02 1.791E+02 +1.263E+00-1.767E+00
6.262E-01 +2.559E-02-1.535E-02 1.772E+02 +1.451E+00-1.325E+00
7.094E-01 +3.330E-02-1.915E-02 1.769E+02 +1.451E+00-2.019E+00
7.784E-01 +2.305E-02-1.918E-02 1.785E+02 +1.514E+00-1.199E+00
8.756E-01 +3.841E-02-3.069E-02 1.788E+02 +1.073E+00-1.577E+00
9.614E-01 +2.559E-02-2.559E-02 1.782E+02 +9.462E-01-1.388E+00
\END;
/*===================================================================*/
|