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Article: Hyperaccreting black hole as gamma-ray burst central engine. I. Baryon loading in gamma-ray burst jets

TitleHyperaccreting black hole as gamma-ray burst central engine. I. Baryon loading in gamma-ray burst jets
Authors
Keywordsaccretion, accretion disks
black hole physics
magnetic fields
Issue Date2013
Citation
Astrophysical Journal, 2013, v. 765, n. 2, article no. 125 How to Cite?
AbstractA hyperaccreting stellar-mass black hole has been long speculated as the best candidate for the central engine of gamma-ray bursts (GRBs). Recent rich observations of GRBs by space missions such as Swift and Fermi pose new constraints on GRB central engine models. In this paper, we study the baryon-loading processes of a GRB jet launched from a black hole central engine. We consider a relativistic jet powered by -annihilation or by the Blandford-Znajek (BZ) mechanism. We consider baryon loading from a neutrino-driven wind launched from a neutrino-cooling-dominated accretion flow. For a magnetically dominated BZ jet, we consider neutron drifting from the magnetic wall surrounding the jet and subsequent positron capture and proton-neutron inelastic collisions. The minimum baryon loads in both types of jet are calculated. We find that in both cases a more luminous jet tends to be more baryon poor. A neutrino-driven "fireball" is typically "dirtier" than a magnetically dominated jet, while a magnetically dominated jet can be much cleaner. Both models have the right scaling to interpret the empirical Γ-L iso relation discovered recently. Since some neutrino-driven jets have too much baryon loading as compared with the data, we suggest that at least a good fraction of GRBs should have a magnetically dominated central engine. © 2013. The American Astronomical Society. All rights reserved..
Persistent Identifierhttp://hdl.handle.net/10722/361226
ISSN
2023 Impact Factor: 4.8
2023 SCImago Journal Rankings: 1.905

 

DC FieldValueLanguage
dc.contributor.authorLei, Wei Hua-
dc.contributor.authorZhang, Bing-
dc.contributor.authorLiang, En Wei-
dc.date.accessioned2025-09-16T04:15:28Z-
dc.date.available2025-09-16T04:15:28Z-
dc.date.issued2013-
dc.identifier.citationAstrophysical Journal, 2013, v. 765, n. 2, article no. 125-
dc.identifier.issn0004-637X-
dc.identifier.urihttp://hdl.handle.net/10722/361226-
dc.description.abstractA hyperaccreting stellar-mass black hole has been long speculated as the best candidate for the central engine of gamma-ray bursts (GRBs). Recent rich observations of GRBs by space missions such as Swift and Fermi pose new constraints on GRB central engine models. In this paper, we study the baryon-loading processes of a GRB jet launched from a black hole central engine. We consider a relativistic jet powered by -annihilation or by the Blandford-Znajek (BZ) mechanism. We consider baryon loading from a neutrino-driven wind launched from a neutrino-cooling-dominated accretion flow. For a magnetically dominated BZ jet, we consider neutron drifting from the magnetic wall surrounding the jet and subsequent positron capture and proton-neutron inelastic collisions. The minimum baryon loads in both types of jet are calculated. We find that in both cases a more luminous jet tends to be more baryon poor. A neutrino-driven "fireball" is typically "dirtier" than a magnetically dominated jet, while a magnetically dominated jet can be much cleaner. Both models have the right scaling to interpret the empirical Γ-L <inf>iso</inf> relation discovered recently. Since some neutrino-driven jets have too much baryon loading as compared with the data, we suggest that at least a good fraction of GRBs should have a magnetically dominated central engine. © 2013. The American Astronomical Society. All rights reserved..-
dc.languageeng-
dc.relation.ispartofAstrophysical Journal-
dc.subjectaccretion, accretion disks-
dc.subjectblack hole physics-
dc.subjectmagnetic fields-
dc.titleHyperaccreting black hole as gamma-ray burst central engine. I. Baryon loading in gamma-ray burst jets-
dc.typeArticle-
dc.description.naturelink_to_subscribed_fulltext-
dc.identifier.doi10.1088/0004-637X/765/2/125-
dc.identifier.scopuseid_2-s2.0-84874466097-
dc.identifier.volume765-
dc.identifier.issue2-
dc.identifier.spagearticle no. 125-
dc.identifier.epagearticle no. 125-
dc.identifier.eissn1538-4357-

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