|
| /*===================================================================*/
/* NRDF D1502 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
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,1;
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,1;
INC-ENGY-LAB=(45MEV/A);
/* OTHERS=('8'): */
/*@8@*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
DATA1'6' DELTA-DATA1 DATA2'7,12' DELTA-DATA2'12'
(NODIM) (NODIM) (UNIT) (UNIT)
8.386E-03 +6.708E-03-7.975E-03 -1.849E+01 +9.735E-01-1.100E+00
3.272E-02 +6.472E-03-8.709E-03 -1.926E+01 +7.749E-01-7.996E-01
5.391E-02 +8.717E-03-1.073E-02 -1.913E+01 +8.495E-01-9.488E-01
7.535E-02 +1.146E-02-9.465E-03 -1.674E+01 +3.740E-01-6.489E-01
9.388E-02 +9.719E-03-6.973E-03 -1.361E+01 +4.739E-01-6.245E-01
1.128E-01 +7.482E-03-7.710E-03 -1.183E+01 +8.240E-01-5.493E-01
1.334E-01 +1.022E-02-8.723E-03 -9.481E+00 +8.736E-01-5.235E-01
1.563E-01 +9.944E-03-8.249E-03 -7.359E+00 +4.500E-01-7.005E-01
1.768E-01 +5.728E-03-1.049E-02 -5.108E+00 +4.256E-01-6.495E-01
1.957E-01 +6.467E-03-8.966E-03 -3.256E+00 +6.739E-01-6.734E-01
2.125E-01 +9.454E-03-8.731E-03 4.219E-01 +4.739E-01-8.245E-01
2.365E-01 +1.097E-02-9.475E-03 3.193E+00 +4.003E-01-9.000E-01
2.583E-01 +5.489E-03-1.147E-02 4.668E+00 +7.488E-01-3.496E-01
2.794E-01 +6.981E-03-8.232E-03 5.793E+00 +6.497E-01-6.989E-01
2.957E-01 +5.985E-03-8.222E-03 4.702E+00 +6.734E-01-3.987E-01
3.137E-01 +6.459E-03-1.048E-02 5.282E+00 +3.984E-01-7.993E-01
3.309E-01 +9.484E-03-8.712E-03 5.887E+00 +5.480E-01-3.995E-01
3.557E-01 +1.245E-02-8.723E-03 4.637E+00 +7.730E-01-5.746E-01
3.757E-01 +8.953E-03-8.980E-03 3.067E+00 +5.738E-01-9.239E-01
3.940E-01 +4.972E-03-1.072E-02 4.146E+00 +1.399E+00-1.025E+00
\END;
/*===================================================================*/
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