/*===================================================================*/ /* NRDF D1492 Data No.5 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,5; D#=D1492; TITLE=/DISAPPEARANCE OF FLOW AS A FUNCTION OF IMPACT PARAMETER AND ENERGY IN NUCLEUS-NUCLEUS COLLISIONS/; PURPOSE=/TO DETERMINE NN-CROSS SECTION IN MEDIUM AND NUCLEAR COMPRESSIBILITY/; ATH=(J.P.SULLIVAN'1',J.PETER'1',D.CUSSOL'1',G.BIZARD'1',R.BROU'1', M.LOUVEL'1',J.P.PATRY'1',R.REGIMBART'1',J.C.STECKMEYER'1', B.TAMAIN'1',E.CREMA'2',H.DOUBRE'2',K.HAGEL'2',G.M.JIN'2,3', A.PEGHAIRE'2',F.SAINT-LAURENT'2',Y.CASSAGNOU'4',R.LEGRAIN'4', C.LEBRUN'5',E.ROSATO'6',R.MACGRATH'7',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',2CHPIMP'3',2FR SAC'4',2FR FR '5', 2ITYNAP'6',1USASTB'7',2JPNTSU'8',2JPNINS'9',2JPNRIK'10'); /*@3@*/ /*@4@*/ /*@6@*/ REF=PL/B; VLP=249(1990)8; RCTS=(27AL(40AR,X),27AL(36AR,X)); PHQS=(X'8'); /*@8@*/ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,5; RTY=(INEL-SCATT); INST-ACC=2FR FR '4'; /*@4@*/ DET-SYS=(TOF,X'9'); /*@9@*/ ANT-COINC=NO; ANL=(X'10'); /*@10@*/ INC-ENGY-LAB=(65MEV/A); CHRG-INC-ION=40; PHQ=(X'8'); /*@8@*/ DET-PARTCL=(D); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,5; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; DATA3'17' DELTA-DATA3'17' DATA4'8' DELTA-DATA4'8' (FM) (FM) (MEV/C) (MEV/C) 5.717E-01 +1.191E+00-9.447E-01 8.104E+00 +1.938E+00-2.364E+00 2.790E+00 +1.102E+00-1.349E+00 1.234E+01 +1.909E+00-2.144E+00 5.911E+00 +1.506E+00-1.642E+00 1.732E+01 +2.907E+00-2.996E+00 1.008E+01 +2.046E+00-2.136E+00 2.100E+01 +3.069E+00-2.922E+00 1.447E+01 +1.506E+00-2.001E+00 2.701E+01 +3.127E+00-3.084E+00 1.918E+01 +2.766E+00-2.563E+00 3.254E+01 +3.260E+00-2.717E+00 2.491E+01 +2.900E+00-2.585E+00 3.049E+01 +2.937E+00-3.054E+00 3.155E+01 +2.654E+00-2.968E+00 2.632E+01 +3.362E+00-2.908E+00 \END; /*===================================================================*/ |