/*===================================================================*/ /* NRDF D0340 Data No.5 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,5; D#=D340; TITLE=/NUCLEAR FRAGMENT EMISSION IN HIGH-ENERGY P-XE AND P-KR COLLISIONS AND A DESCRIPTION OF THEIR PRODUCTION MECHANISM/; PURPOSE=/TO PRESENT DATA FROM KR AND XE TARGETS AND DISCUSS AN INTERPRETATION IN TERMS OF A SIMPLE MODEL FOR HEAVY-FRAGMENT EMISSION./; /*@3@*/ ATH=(J.A.GAIDOS'1,2',L.J.GUTAY'1,2',A.S.HIRSCH'1',R.MITCHELL'1,2', T.V.RAGLAND'1,2',R.P.SCHARENBERG'1,2',F.TURKOT'1,2', R.B.WILLMANN'1,2',C.L.WILSON'1,2'); INST-ATH=(1USAPUR'1',1USANAL'2'); REF=PRL; VLP=42(1979)82; RCTS=(XE(P, )LI,XE(P, )BE,XE(P, )B,XE(P, )C,XE(P, )N,XE(P, )O,XE(P, )F, XE(P, )NE,XE(P, )NA,XE(P, )MG,XE(P, )AL,XE(P, )SI, KR(P, )LI,KR(P, )BE,KR(P, )B,KR(P, )C,KR(P, )N,KR(P, )O,KR(P, )F, KR(P, )NE,KR(P, )NA,KR(P, )MG,KR(P, )AL,KR(P, )SI); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,5; THK-TGT=100NG/CM**2'1'; /*@4@*/ BAC=SELF; POL-TGT=NO; ACC=(X); INST-ACC=1USANAL; INC-ENGY-LAB-RANGE=(20GEV/C[400GEV/C); POL-PRJ=NO; DET-PARTCL=(X'1'); /*@5@*/ DET-SYS=(MAG+PS-SI); ANL=(X'1'); /*@6@*/ PHQ=(A-DSTRN); RCT=KR(P, )B; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,5; THTL=33DEG[76DEG; /*FIG.2-(1)*/ /* D340 FIG.2-(1) */ /* SER#= 1 */ /* XSCALE=LINEAR YSCALE=LOG */ /* XMAX= 1.20000000E+02 YMAX= 1.00000000E+05 */ /* XMIN= 0.00000000E+00 YMIN= 1.00000000E+00 */ /* FOLLOWING DATA ARE TAKEN FROM GRAPH */ /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; DATA1'1' DATA2'2' DELTA-DATA2 (MEV) (ARB-UNT) (ARB-UNT) 10.072 4.529E+04 XXXXXXXXX 12.374 5.306E+04 XXXXXXXXX 14.388 6.300E+04 XXXXXXXXX 16.403 6.641E+04 XXXXXXXXX 18.705 6.910E+04 XXXXXXXXX 20.144 7.189E+04 XXXXXXXXX 22.158 7.284E+04 XXXXXXXXX 23.597 7.479E+04 XXXXXXXXX 25.899 7.579E+04 XXXXXXXXX 27.914 7.381E+04 XXXXXXXXX 29.928 7.001E+04 XXXXXXXXX 31.942 6.641E+04 XXXXXXXXX 33.957 6.300E+04 XXXXXXXXX 35.971 5.820E+04 XXXXXXXXX 38.273 5.306E+04 XXXXXXXXX 40.288 4.902E+04 XXXXXXXXX 42.014 4.411E+04 XXXXXXXXX 43.741 4.021E+04 XXXXXXXXX 45.755 3.666E+04 XXXXXXXXX 48.057 3.432E+04 XXXXXXXXX 50.360 3.047E+04 XXXXXXXXX 52.086 2.778E+04 XXXXXXXXX 54.388 2.533E+04 XXXXXXXXX 56.403 2.220E+04 XXXXXXXXX 57.842 1.971E+04 XXXXXXXXX 60.144 1.821E+04 XXXXXXXXX 62.158 1.617E+04 XXXXXXXXX 64.460 1.494E+04 XXXXXXXXX 66.475 1.398E+04 XXXXXXXXX 68.489 1.275E+04 XXXXXXXXX 70.791 1.117E+04 XXXXXXXXX 72.518 9.791E+03 XXXXXXXXX 74.532 8.927E+03 XXXXXXXXX 76.547 8.580E+03 XXXXXXXXX 78.273 7.519E+03 XXXXXXXXX 79.712 6.765E+03 XXXXXXXXX 82.302 6.250E+03 XXXXXXXXX 84.604 5.698E+03 XXXXXXXXX 86.619 5.127E+03 XXXXXXXXX 88.345 4.736E+03 XXXXXXXXX 90.647 4.736E+03 XXXXXXXXX 93.237 3.989E+03 XXXXXXXXX 94.676 3.686E+03 2.515E+02 96.403 3.590E+03 3.998E+02 98.705 2.984E+03 3.764E+02 100.719 2.793E+03 2.302E+02 \END; /*===================================================================*/ |