|
| /*===================================================================*/
/* NRDF D0340 Data No.6 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,6;
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,6;
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, )N;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,6;
THTL=33DEG[76DEG;
/*FIG.2-(2)*/
/* D340 FIG.2-(2) */
/* SER#= 2 */
/* 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)
16.442 3.618E+04 XXXXXXXXX
18.461 4.021E+04 XXXXXXXXX
20.192 4.075E+04 XXXXXXXXX
22.211 4.184E+04 XXXXXXXXX
23.942 4.021E+04 XXXXXXXXX
25.673 3.916E+04 XXXXXXXXX
27.692 3.916E+04 XXXXXXXXX
29.711 3.764E+04 XXXXXXXXX
31.731 3.571E+04 XXXXXXXXX
33.750 3.478E+04 XXXXXXXXX
36.058 3.255E+04 XXXXXXXXX
38.654 3.008E+04 XXXXXXXXX
39.808 2.853E+04 XXXXXXXXX
41.538 2.467E+04 XXXXXXXXX
43.558 2.279E+04 XXXXXXXXX
46.154 2.134E+04 XXXXXXXXX
47.885 1.895E+04 XXXXXXXXX
49.904 1.660E+04 XXXXXXXXX
52.211 1.514E+04 XXXXXXXXX
54.231 1.380E+04 XXXXXXXXX
56.538 1.209E+04 XXXXXXXXX
58.269 1.103E+04 XXXXXXXXX
60.288 9.921E+03 XXXXXXXXX
62.308 8.580E+03 XXXXXXXXX
64.904 7.720E+03 XXXXXXXXX
66.635 7.038E+03 XXXXXXXXX
68.654 6.250E+03 XXXXXXXXX
70.385 5.698E+03 XXXXXXXXX
72.404 4.928E+03 XXXXXXXXX
74.423 4.553E+03 XXXXXXXXX
76.731 4.096E+03 XXXXXXXXX
78.461 3.637E+03 XXXXXXXXX
80.192 3.023E+03 2.927E+02
81.923 2.720E+03 1.856E+02
84.519 2.261E+03 2.189E+02
87.404 2.173E+03 2.104E+02
89.135 2.035E+03 1.677E+02
91.154 1.562E+03 1.740E+02
92.885 1.583E+03 1.305E+02
94.904 1.522E+03 1.254E+02
96.635 1.184E+03 1.146E+02
98.654 1.108E+03 1.234E+02
100.673 8.625E+02 1.217E+02
102.981 9.336E+02 1.040E+02
105.577 8.625E+02 8.351E+01
\END;
/*===================================================================*/
|