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