|
| /*===================================================================*/
/* NRDF D1502 Data No.6 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,6;
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,6;
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,6;
INC-ENGY-LAB=(45MEV/A);
/* OTHERS=('9'): */
/*@9@*/
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
DATA1'13' DELTA-DATA1 DATA2'14,12' DELTA-DATA2'12'
(NODIM) (NODIM) (UNIT) (UNIT)
-9.480E-01 +2.917E-02-3.677E-02 1.830E+02 +1.208E+00-1.463E+00
-8.807E-01 +2.537E-02-2.915E-02 1.814E+02 +1.526E+00-1.654E+00
-8.073E-01 +1.397E-02-2.662E-02 1.862E+02 +1.081E+00-1.717E+00
-7.249E-01 +1.774E-02-4.438E-02 1.863E+02 +1.335E+00-1.590E+00
-6.527E-01 +3.045E-02-3.676E-02 1.886E+02 +1.081E+00-1.590E+00
-5.525E-01 +1.903E-02-4.563E-02 1.885E+02 +1.399E+00-1.526E+00
-4.650E-01 +2.155E-02-3.422E-02 1.878E+02 +1.271E+00-1.463E+00
-3.927E-01 +2.283E-02-3.549E-02 1.874E+02 +1.399E+00-1.335E+00
-3.218E-01 +2.157E-02-3.675E-02 1.915E+02 +1.335E+00-1.971E+00
-2.494E-01 +2.918E-02-3.931E-02 1.894E+02 +1.653E+00-1.844E+00
-1.531E-01 +2.790E-02-5.960E-02 1.915E+02 +1.526E+00-2.035E+00
-6.947E-02 +3.552E-02-3.675E-02 1.932E+02 +1.590E+00-1.717E+00
1.550E-02 +2.791E-02-3.295E-02 1.930E+02 +1.780E+00-2.099E+00
8.655E-02 +3.295E-02-2.411E-02 1.923E+02 +1.654E+00-1.399E+00
1.689E-01 +2.031E-02-2.406E-02 1.939E+02 +1.145E+00-1.653E+00
2.399E-01 +2.286E-02-2.025E-02 1.964E+02 +1.145E+00-2.290E+00
3.249E-01 +3.300E-02-3.675E-02 1.941E+02 +8.904E-01-1.399E+00
4.072E-01 +3.934E-02-3.421E-02 1.980E+02 +1.844E+00-2.544E+00
5.240E-01 +1.902E-02-4.817E-02 1.941E+02 +1.781E+00-1.527E+00
5.912E-01 +2.031E-02-2.280E-02 1.955E+02 +1.081E+00-1.908E+00
6.634E-01 +1.904E-02-3.041E-02 1.964E+02 +1.017E+00-1.590E+00
7.193E-01 +2.791E-02-1.774E-02 1.953E+02 +1.145E+00-1.272E+00
8.055E-01 +3.174E-02-3.041E-02 1.964E+02 +1.017E+00-1.653E+00
8.930E-01 +2.665E-02-4.945E-02 1.969E+02 +1.399E+00-1.463E+00
9.856E-01 +3.550E-02-2.663E-02 1.954E+02 +1.526E+00-1.336E+00
\END;
/*===================================================================*/
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