Diffuse Gamma-Rays Produced in Cosmic-Ray Interactions and the TeV-band Spectrum of RX J1713.7-3946
| dc.creator | Huang, C. -Y. | |
| dc.creator | Pohl, M. | |
| dc.creator | Park, S. -E. | |
| dc.creator | Daniels, C. D. | |
| dc.date | 2007-06-04 | |
| dc.date | 2007-06-05 | |
| dc.date.accessioned | 2026-07-07T08:09:28Z | |
| dc.date.available | 2026-07-07T08:09:28Z | |
| dc.description | We employ the Monte Carlo particle collision code DPMJET3.04 to determine the multiplicity spectra of various secondary particles (in addition to $π^0$'s) with $γ$'s as the final decay state, that are produced in cosmic-ray ($p$'s and $α$'s) interactions with the interstellar medium. We derive an easy-to-use $γ$-ray production matrix for cosmic rays with energies up to about 10 PeV. This $γ$-ray production matrix is applied to the GeV excess in diffuse Galactic $γ$-rays observed by EGRET, and we conclude the non-$π^0$ decay components are insufficient to explain the GeV excess, although they have contributed a different spectrum from the $π^0$-decay component. We also test the hypothesis that the TeV-band $γ$-ray emission of the shell-type SNR RX J1713.7-3946 observed with HESS is caused by hadronic cosmic rays which are accelerated by a cosmic-ray modified shock. By the $χ^2$ statistics, we find a continuously softening spectrum is strongly preferred, in contrast to expectations. A hardening spectrum has about 1% probability to explain the HESS data, but then only if a hard cutoff at 50-100 TeV is imposed on the particle spectrum. | |
| dc.description | 4 pages; 5 figures; Contribution to the 30th ICRC, Merida, Mexico, 2007; References included | |
| dc.identifier | https://arxiv.org/abs/0706.0506 | |
| dc.identifier | http://arxiv.org/abs/0706.0506 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/131550 | |
| dc.subject | Astrophysics | |
| dc.title | Diffuse Gamma-Rays Produced in Cosmic-Ray Interactions and the TeV-band Spectrum of RX J1713.7-3946 | |
| dc.type | text |