Production spectrum of gamma rays in interstellar space through neutral pion decay

1981 ◽  
Vol 76 (1) ◽  
pp. 213-233 ◽  
Author(s):  
S. A. Stephens ◽  
G. D. Badhwar
2005 ◽  
Vol 71 (11) ◽  
Author(s):  
Alexander C. Kalloniatis ◽  
Jonathan D. Carroll ◽  
Byung-Yoon Park

1992 ◽  
Vol 396 ◽  
pp. L111 ◽  
Author(s):  
Natalie Mandzhavidze ◽  
Reuven Ramaty
Keyword(s):  

1991 ◽  
Vol 06 (02) ◽  
pp. 143-149
Author(s):  
M.I. DOBROLIUBOV

We found a strong enhancement of the rate of the decay of π0-meson into scalar and pseudoscalar bosons as compared with its decay into two photons. The branching ratio of this mode can be as large as BR(π0→S+P)≃10−6–10−5, which is very interesting from the experimental point of view.


2009 ◽  
Vol 18 (10) ◽  
pp. 1571-1575
Author(s):  
ANDREW TAYLOR

During their acceleration, both UHECR nuclei and UHECR protons may interact with the radiation field present in the accelerator region leading to photo-disintegration and photo-pion production interactions respectively. This leads to a close connection between the degree of disintegration of UHECR nuclei and the UHE neutrino flux produced by a source. Upon escaping the accelerator, UHECR protons go on to generate a secondary UHE photon flux through photo-pion interactions with the cosmic microwave background (CMB) photons, These secondary UHE photons produced (via neutral pion decay) will themselves also interact with the cosmic radio background (CRB) photons. This leads to a second connection between UHE photons and nearby source of UHECR protons. We hear investigate both these connections to draw conclusions on what we can learn about UHECR sources.


1971 ◽  
Vol 2 (1) ◽  
pp. 77-92 ◽  
Author(s):  
G. Cavallo ◽  
R. J. Gould

1960 ◽  
Vol 117 (3) ◽  
pp. 854-858 ◽  
Author(s):  
Maurice Jacob ◽  
Jon Mathews

1958 ◽  
Vol 9 (3) ◽  
pp. 451-460 ◽  
Author(s):  
M. L. Goldberger ◽  
S. B. Treiman
Keyword(s):  

1987 ◽  
Vol 192 (1-2) ◽  
pp. 135-137 ◽  
Author(s):  
M.I. Dobroliubov ◽  
A.Yu. Ignatiev ◽  
V.A. Matveev
Keyword(s):  

1981 ◽  
Vol 94 ◽  
pp. 333-334
Author(s):  
M. Giler ◽  
J. Wdowczyk ◽  
A. W. Wolfendale

In our recent work we have shown that a good model for the highest energy cosmic rays is one where they are generated in clusters of galaxies with a relatively flat production spectrum and then propagate with an energy dependent diffusion coefficient. There is evidence for a similar flat production spectrum (γ ≃ 2.1) for both protons and electrons in our own Galaxy. Here we assume that the spectrum for clusters (specifically the VIRGO cluster) is independent of energy and an evaluation is made of the likely flux of γ-rays.


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