|
| /*===================================================================*/
/* NRDF D1502 Data No.2 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,2;
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,2;
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,2;
INC-ENGY-LAB=(45MEV/A);
/* OTHERS=('9'): */
/*@9@*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
DATA1'6' DELTA-DATA1 DATA2'7,12' DELTA-DATA2'12'
(NODIM) (NODIM) (UNIT) (UNIT)
8.878E-03 +7.309E-03-5.333E-03 -1.373E+01 +6.803E-01-1.008E+00
2.711E-02 +7.579E-03-8.105E-03 -1.349E+01 +5.795E-01-7.574E-01
4.843E-02 +6.064E-03-8.109E-03 -1.268E+01 +3.768E-01-4.285E-01
7.027E-02 +8.343E-03-7.611E-03 -1.164E+01 +3.018E-01-6.814E-01
9.242E-02 +5.303E-03-1.039E-02 -9.894E+00 +3.779E-01-5.043E-01
1.094E-01 +5.569E-03-8.364E-03 -6.606E+00 +5.545E-01-6.560E-01
1.295E-01 +7.577E-03-9.881E-03 -4.657E+00 +4.283E-01-6.549E-01
1.482E-01 +9.858E-03-1.037E-02 -2.051E+00 +3.272E-01-6.049E-01
1.725E-01 +1.214E-02-9.626E-03 2.981E-01 +3.277E-01-7.566E-01
1.921E-01 +7.862E-03-8.355E-03 1.693E+00 +4.791E-01-6.553E-01
2.100E-01 +4.791E-03-9.118E-03 4.148E+00 +4.037E-01-7.316E-01
2.262E-01 +6.323E-03-8.853E-03 4.941E+00 +4.031E-01-4.793E-01
2.466E-01 +4.287E-03-7.099E-03 6.512E+00 +2.010E-01-3.285E-01
2.707E-01 +5.297E-03-1.141E-02 6.971E+00 +3.524E-01-5.554E-01
2.932E-01 +3.027E-03-7.609E-03 7.456E+00 +3.524E-01-5.784E-01
3.084E-01 +7.324E-03-4.572E-03 7.040E+00 +3.022E-01-6.060E-01
3.279E-01 +8.328E-03-4.825E-03 7.225E+00 +3.777E-01-7.064E-01
3.483E-01 +5.565E-03-5.307E-03 6.855E+00 +4.791E-01-5.047E-01
3.696E-01 +8.079E-03-1.139E-02 4.367E+00 +4.524E-01-8.576E-01
3.907E-01 +7.577E-03-6.343E-03 5.484E+00 +4.776E-01-9.591E-01
\END;
/*===================================================================*/
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