2010
DOI: 10.1016/j.astropartphys.2010.08.004
|View full text |Cite
|
Sign up to set email alerts
|

Limitations on the photo-disintegration process as a source of VHE photons

Abstract: We consider whether photo-disintegration is ever able to provide an effective mechanism for the production of VHE γ-ray emission from astrophysical sources. We find that the efficiency of this process is always smaller by a factor A/Z 2 (∼ 4/A) than that of nuclei cooling through Bethe-Heitler pair-production. Furthermore, for sources optically thin to TeV emission, we find that the efficiency of this process can be no more than 3 × 10 −5 (Rsource/RLarmor), where Rsource is the source size and RLarmor is the C… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
8
0

Year Published

2011
2011
2024
2024

Publication Types

Select...
4
4
2

Relationship

0
10

Authors

Journals

citations
Cited by 16 publications
(8 citation statements)
references
References 19 publications
(29 reference statements)
0
8
0
Order By: Relevance
“…On the other hand, nuclei interact with lowenergy photons in the source via the photodisintegration process, leading to subsequent (almost prompt) ∼ 0.2 TeV γ A,5 gamma rays from daughter excited nuclei. This signal is useful as a unique probe of nuclei acceleration as well as syn-chrotron and inverse-Compton gamma rays from pairs generated via the Bethe-Heitler process (Murase & Beacom 2010a;Aharonian & Taylor 2010). There are a multitude of potential signatures to be explored.…”
Section: Discussionmentioning
confidence: 99%
“…On the other hand, nuclei interact with lowenergy photons in the source via the photodisintegration process, leading to subsequent (almost prompt) ∼ 0.2 TeV γ A,5 gamma rays from daughter excited nuclei. This signal is useful as a unique probe of nuclei acceleration as well as syn-chrotron and inverse-Compton gamma rays from pairs generated via the Bethe-Heitler process (Murase & Beacom 2010a;Aharonian & Taylor 2010). There are a multitude of potential signatures to be explored.…”
Section: Discussionmentioning
confidence: 99%
“…The Doppler-boosted gamma-ray emission due to the deexcitation of these nuclei with Lorentz factor Γ ≥ 10 5 may lead, in principle, to a rather narrow lines at energy E = Γ E * ∼ 100 GeV (typically the prompt de-excitation gamma-ray lines are produced with energy in the frame of the nucleus E * ∼ 1 MeV). However, the efficiency of this mechanism in typical astrophysical environments is very low (Aharonian & Taylor 2010). Also, the disintegration of the primary nuclei would lead to emission of a large number of lines from secondary nuclei, and eventually to a rather broad distribution.…”
Section: Astrophysical Vhe Gamma-ray Lines?mentioning
confidence: 99%
“…Nevertheless, as internal γγ attenuation is then mitigated [137], GeV-TeV signals from nuclear deexcitation, photopair creation or nuclear synchrotron emission may be observable and provide a unique signature of UHECR nuclei acceleration [172,173]. For example, Lorentz-boosted de-excitation gamma rays at energies ∼ TeV(E A /3 × 10 16 eV), where E A is the energy of CR nuclei, may be detectable from nearby, low-luminosity GRBs (see however [174]). …”
Section: Ultra-high-energy Cosmic Rays and Neutrinosmentioning
confidence: 99%