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Entry No. D0340

J.A.Gaidos1,2,L.J.Gutay1,2,A.S.Hirsch1,R.Mitchell1,2, T.V.Ragland1,2,R.P.Scharenberg1,2,F.Turkot1,2, R.B.Willmann1,2,C.L.Wilson1,2
Purdue University, West Lafayette, IN1
Fermi National Laboratory, Batavia, IL2
Physical Review Letters42(1979)82

NUCLEAR FRAGMENT EMISSION IN HIGH-ENERGY P-XE AND P-KR COLLISIONS AND A DESCRIPTION OF THEIR PRODUCTION MECHANISM

Click on the data number to see the plot. Or select the box to plot multiple data.
DataFilePhysical quantitiesReaction(s)Energies
1 *DATA11) DATA22)
XE(P, )B; between 20/C and 400/C) GEV
2 *DATA11) DATA22)
XE(P, )N; between 20/C and 400/C) GEV
3 *DATA11) DATA22)
XE(P, )NA; between 20/C and 400/C) GEV
4 *DATA11) DATA22)
XE(P, )X'1'; between 20/C and 400/C) GEV
5 *DATA11) DATA22)
KR(P, )B; between 20/C and 400/C) GEV
6 *DATA11) DATA22)
KR(P, )N; between 20/C and 400/C) GEV
7 *DATA11) DATA22)
KR(P, )SI; between 20/C and 400/C) GEV
8 *DATA11) DATA22)
KR(P, )X'1'; between 20/C and 400/C) GEV

1) DATA1=FRAGMENT NUCLEON NUMBER
2) DATA2=THE INVERSE LOGARITHMIC SLOPE T, WHICH APPEARS IN THE DIFFERENTIAL CROSS SECTION;DSIGMA/DE/DOMEGA=N(E/E1*(E1-B))**(1/2)*EXP(-((E1-B)/T)), WHERE N,B,E ARE A NORMALIZATION CONSTANT, THE COULOMB BARRIER EVERGY,THE MEASURED LABORATORY ENERGY OF THE FRAGMENT,RESPECTIVELY. E1=E+E0-2*(E*E0)**(1/2)*COS(THETA). THETA IS THE LABORATORY ANGLE AND E0=1/2*M*V**2,WHERE M,V ARE THE FRAGMENT MASS AND VELOCITY,RESPECTIVELY.
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Last update of this script: April 12, 2006. Contact address: darpe-admin@jcprg.org