scholarly journals Pion production in high-energy nucleus-nucleus collisions

1987 ◽  
Vol 58 (5) ◽  
pp. 463-466 ◽  
Author(s):  
J. W. Harris ◽  
G. Odyniec ◽  
H. G. Pugh ◽  
L. S. Schroeder ◽  
M. L. Tincknell ◽  
...  
Keyword(s):  
1958 ◽  
Vol 111 (6) ◽  
pp. 1698-1698 ◽  
Author(s):  
Suraj N. Gupta

1999 ◽  
Vol 11 (4) ◽  
pp. 703-708 ◽  
Author(s):  
A. Ahmedov ◽  
I.V. Akushevich ◽  
E.A. Kuraev ◽  
P.G. Ratcliffe

1980 ◽  
Vol 45 (11) ◽  
pp. 874-877 ◽  
Author(s):  
A. Sandoval ◽  
R. Stock ◽  
H. E. Stelzer ◽  
R. E. Renfordt ◽  
J. W. Harris ◽  
...  

1985 ◽  
Vol 15 ◽  
pp. 353-362 ◽  
Author(s):  
C. Besliu ◽  
V. Boldea ◽  
V. Topor Pop ◽  
R. Topor Pop ◽  
V. Popa ◽  
...  
Keyword(s):  

1966 ◽  
Vol 42 (2) ◽  
pp. 251-268 ◽  
Author(s):  
M. S. Spergel ◽  
M. Lieber ◽  
S. N. Milford

1965 ◽  
Vol 23 ◽  
pp. 253-258
Author(s):  
M. Libber ◽  
S. N. Milford ◽  
M. S. Spergel

Collisions of high energy cosmic rays with intergalactic gas produce various secondaries, including neutral pions that decay into high energy γ rays. The Landau-Milekhin hydrodynamical model for proton-proton collisions is used to calculate the pion production spectrum corresponding to cosmic γ rays of energy above 10 Gev. A source function for these high energy γ rays in space is found by combining the pion production and decay spectra with the primary cosmic ray proton flux. The resulting γ ray spectrum follows a different power law than spectra based upon the usual assumption of a line spectrum for the pions in the center of mass system of the colliding protons. The high energy γ ray intensity in space is calculated for a simple model universe. By comparison with previous estimates for the proton photoproduction process, it is found that proton-proton and proton-photon collisions appear to contribute about the same order of magnitude to the intergalactic γ ray intensity above ∼1016 eV.


1982 ◽  
Vol 379 (3) ◽  
pp. 553-567 ◽  
Author(s):  
J. Cugnon ◽  
D. Kinet ◽  
J. Vandermeulen

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