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Article: High-energy afterglow emission from giant flares of soft gamma-ray repeaters: The case of the 2004 December 27 event from SGR 1806-20

TitleHigh-energy afterglow emission from giant flares of soft gamma-ray repeaters: The case of the 2004 December 27 event from SGR 1806-20
Authors
KeywordsAcceleration of particles
Elementary particles
Gamma-rays: bursts
Hydrodynamics
Stars: neutron
Stars: winds, outflows
Issue Date2005
Citation
Monthly Notices of the Royal Astronomical Society, 2005, v. 361, n. 3, p. 965-970 How to Cite?
AbstractWe discuss the high-energy afterglow emission (including high-energy photons, neutrinos and cosmic rays) following the 2004 December 27 giant flare from the soft gamma-ray repeater (SGR) 1806-20. If the initial outflow is relativistic with a bulk Lorentz factor Γ0 ∼ tens, the high-energy tail of the synchrotron emission from electrons in the forward shock region gives rise to a prominent sub-GeV emission, if the electron spectrum is hard enough and if the initial Lorentz factor is high enough. This signal could serve as a diagnosis of the initial Lorentz factor of the giant flare outflow. This component is potentially detectable by the Gamma-Ray Large Area Telescope (GLAST) if a similar giant flare occurs in the GLAST era. With the available 10-MeV data, we constrain that Γ0 < 50 if the electron distribution is a single power law. For a broken power-law distribution of electrons, a higher Γ0 is allowed. At energies higher than 1 GeV, the flux is lower because of a high-energy cut-off of the synchrotron emission component. The synchrotron self-Compton emission component and the inverse Compton scattering component off the photons in the giant flare oscillation tail are also considered, but they are found not significant given a moderate Γ0 (e.g. ≤ 10). The forward shock also accelerates cosmic rays to the maximum energy 1017 eV, and generates neutrinos with a typical energy 1014 eV through photomeson interaction with the X-ray tail photons. However, they are too weak to be detectable. © 2005 RAS.
Persistent Identifierhttp://hdl.handle.net/10722/360991
ISSN
2023 Impact Factor: 4.7
2023 SCImago Journal Rankings: 1.621

 

DC FieldValueLanguage
dc.contributor.authorFan, Y. Z.-
dc.contributor.authorZhang, Bing-
dc.contributor.authorWei, D. M.-
dc.date.accessioned2025-09-16T04:14:10Z-
dc.date.available2025-09-16T04:14:10Z-
dc.date.issued2005-
dc.identifier.citationMonthly Notices of the Royal Astronomical Society, 2005, v. 361, n. 3, p. 965-970-
dc.identifier.issn0035-8711-
dc.identifier.urihttp://hdl.handle.net/10722/360991-
dc.description.abstractWe discuss the high-energy afterglow emission (including high-energy photons, neutrinos and cosmic rays) following the 2004 December 27 giant flare from the soft gamma-ray repeater (SGR) 1806-20. If the initial outflow is relativistic with a bulk Lorentz factor Γ<inf>0</inf> ∼ tens, the high-energy tail of the synchrotron emission from electrons in the forward shock region gives rise to a prominent sub-GeV emission, if the electron spectrum is hard enough and if the initial Lorentz factor is high enough. This signal could serve as a diagnosis of the initial Lorentz factor of the giant flare outflow. This component is potentially detectable by the Gamma-Ray Large Area Telescope (GLAST) if a similar giant flare occurs in the GLAST era. With the available 10-MeV data, we constrain that Γ<inf>0</inf> < 50 if the electron distribution is a single power law. For a broken power-law distribution of electrons, a higher Γ<inf>0</inf> is allowed. At energies higher than 1 GeV, the flux is lower because of a high-energy cut-off of the synchrotron emission component. The synchrotron self-Compton emission component and the inverse Compton scattering component off the photons in the giant flare oscillation tail are also considered, but they are found not significant given a moderate Γ<inf>0</inf> (e.g. ≤ 10). The forward shock also accelerates cosmic rays to the maximum energy 10<sup>17</sup> eV, and generates neutrinos with a typical energy 10<sup>14</sup> eV through photomeson interaction with the X-ray tail photons. However, they are too weak to be detectable. © 2005 RAS.-
dc.languageeng-
dc.relation.ispartofMonthly Notices of the Royal Astronomical Society-
dc.subjectAcceleration of particles-
dc.subjectElementary particles-
dc.subjectGamma-rays: bursts-
dc.subjectHydrodynamics-
dc.subjectStars: neutron-
dc.subjectStars: winds, outflows-
dc.titleHigh-energy afterglow emission from giant flares of soft gamma-ray repeaters: The case of the 2004 December 27 event from SGR 1806-20-
dc.typeArticle-
dc.description.naturelink_to_subscribed_fulltext-
dc.identifier.doi10.1111/j.1365-2966.2005.09221.x-
dc.identifier.scopuseid_2-s2.0-23844460606-
dc.identifier.volume361-
dc.identifier.issue3-
dc.identifier.spage965-
dc.identifier.epage970-

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