|
| /*===================================================================*/
/* NRDF D1502 Data No.8 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,8;
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,8;
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,8;
INC-ENGY-LAB=(45MEV/A);
/* OTHERS=('11'): */
/*@11@*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
DATA1'13' DELTA-DATA1 DATA2'14,12' DELTA-DATA2'12'
(NODIM) (NODIM) (UNIT) (UNIT)
-9.683E-01 +1.524E-02-2.026E-02 1.590E+02 +1.254E+00-1.753E+00
-8.910E-01 +2.543E-02-3.413E-02 1.597E+02 +1.378E+00-1.251E+00
-8.237E-01 +1.405E-02-2.913E-02 1.593E+02 +1.253E+00-1.817E+00
-7.399E-01 +3.690E-02-3.419E-02 1.588E+02 +1.253E+00-1.691E+00
-6.526E-01 +3.172E-02-3.675E-02 1.608E+02 +1.629E+00-1.629E+00
-5.564E-01 +2.668E-02-4.304E-02 1.625E+02 +2.320E+00-2.315E+00
-4.810E-01 +2.916E-02-2.540E-02 1.588E+02 +1.566E+00-1.816E+00
-4.142E-01 +2.664E-02-1.649E-02 1.616E+02 +2.444E+00-1.878E+00
-3.304E-01 +2.036E-02-3.165E-02 1.615E+02 +1.815E+00-2.194E+00
-2.581E-01 +2.790E-02-4.569E-02 1.619E+02 +1.878E+00-1.757E+00
-1.798E-01 +3.175E-02-4.565E-02 1.643E+02 +1.693E+00-2.194E+00
-7.900E-02 +3.050E-02-3.294E-02 1.607E+02 +1.567E+00-2.318E+00
-7.214E-04 +3.291E-02-2.402E-02 1.633E+02 +2.005E+00-2.694E+00
7.794E-02 +2.159E-02-2.400E-02 1.634E+02 +1.943E+00-2.066E+00
1.411E-01 +3.298E-02-2.789E-02 1.655E+02 +1.629E+00-1.691E+00
2.124E-01 +3.427E-02-2.786E-02 1.640E+02 +1.881E+00-2.004E+00
3.102E-01 +2.920E-02-3.675E-02 1.635E+02 +1.442E+00-1.880E+00
3.898E-01 +4.191E-02-4.173E-02 1.653E+02 +1.254E+00-1.753E+00
4.837E-01 +3.804E-02-3.674E-02 1.655E+02 +1.442E+00-1.941E+00
5.572E-01 +4.442E-02-3.037E-02 1.660E+02 +1.129E+00-2.315E+00
6.249E-01 +2.546E-02-2.523E-02 1.634E+02 +1.442E+00-1.817E+00
6.941E-01 +4.454E-02-3.790E-02 1.672E+02 +1.690E+00-2.257E+00
7.820E-01 +3.431E-02-4.440E-02 1.652E+02 +1.940E+00-1.754E+00
8.682E-01 +2.916E-02-2.026E-02 1.658E+02 +1.064E+00-1.003E+00
9.634E-01 +2.292E-02-2.019E-02 1.656E+02 +1.064E+00-1.565E+00
\END;
/*===================================================================*/
|