/*===================================================================*/ /* 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; /*===================================================================*/ |