A Common Central Engine for Long Gamma Ray Bursts and Type Ib/c Supernovae?
Long-duration, spectrally-soft Gamma-Ray Bursts (GRBs) are associated with Type Ic Core Collapse (CC) Supernovae (SNe), and thus arise from the death of massive stars. In the collapsar model, the jet launched by the central engine must bore its way out of the progenitor star before it can produce a...
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description | Long-duration, spectrally-soft Gamma-Ray Bursts (GRBs) are associated with Type Ic Core Collapse (CC) Supernovae (SNe), and thus arise from the death of massive stars. In the collapsar model, the jet launched by the central engine must bore its way out of the progenitor star before it can produce a GRB. Most of these jets do not break out, and are instead "choked" inside the star, as the central-engine activity time, \(t_{\rm e}\), is not long enough. Modelling the long-soft GRB duration distribution assuming a power-law distribution for their central-engine activity times, \(\propto t_{\rm e}^{-\alpha}\) for \(t_{\rm e}>t_{\rm b}\), we find a steep distribution (\(\alpha\sim4\)) and a typical GRB jet breakout time of \(t_{\rm b}\sim 60\text{ s}\) in the star's frame. The latter suggests the presence of a low-density, extended envelope surrounding the progenitor star, similar to that previously inferred for low-luminosity GRBs. Extrapolating the range of validity of this power law below what is directly observable, to \(t_{\rm e} |
doi_str_mv | 10.48550/arxiv.1705.00281 |
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In the collapsar model, the jet launched by the central engine must bore its way out of the progenitor star before it can produce a GRB. Most of these jets do not break out, and are instead "choked" inside the star, as the central-engine activity time, \(t_{\rm e}\), is not long enough. Modelling the long-soft GRB duration distribution assuming a power-law distribution for their central-engine activity times, \(\propto t_{\rm e}^{-\alpha}\) for \(t_{\rm e}>t_{\rm b}\), we find a steep distribution (\(\alpha\sim4\)) and a typical GRB jet breakout time of \(t_{\rm b}\sim 60\text{ s}\) in the star's frame. The latter suggests the presence of a low-density, extended envelope surrounding the progenitor star, similar to that previously inferred for low-luminosity GRBs. Extrapolating the range of validity of this power law below what is directly observable, to \(t_{\rm e}<t_{\rm b}\), by only a factor of \(\sim\)4-5 produces enough events to account for all Type Ib/c SNe. Such extrapolation is necessary to avoid fine-tuning the distribution of central engine activity times with the breakout time, which are presumably unrelated. We speculate that central engines launching relativistic jets may operate in all Type Ib/c SNe. In this case, the existence of a common central engine would imply that (i) the jet may significantly contribute to the energy of the SN; (ii) various observational signatures, like the asphericity of the explosion, could be directly related to jet's interaction with the star.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1705.00281</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Asphericity ; Collapse ; Gamma ray bursts ; Gamma rays ; Luminosity ; Massive stars ; Physics - High Energy Astrophysical Phenomena ; Power law ; Public enterprise ; Supernovae</subject><ispartof>arXiv.org, 2017-08</ispartof><rights>2017. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). 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In the collapsar model, the jet launched by the central engine must bore its way out of the progenitor star before it can produce a GRB. Most of these jets do not break out, and are instead "choked" inside the star, as the central-engine activity time, \(t_{\rm e}\), is not long enough. Modelling the long-soft GRB duration distribution assuming a power-law distribution for their central-engine activity times, \(\propto t_{\rm e}^{-\alpha}\) for \(t_{\rm e}>t_{\rm b}\), we find a steep distribution (\(\alpha\sim4\)) and a typical GRB jet breakout time of \(t_{\rm b}\sim 60\text{ s}\) in the star's frame. The latter suggests the presence of a low-density, extended envelope surrounding the progenitor star, similar to that previously inferred for low-luminosity GRBs. Extrapolating the range of validity of this power law below what is directly observable, to \(t_{\rm e}<t_{\rm b}\), by only a factor of \(\sim\)4-5 produces enough events to account for all Type Ib/c SNe. Such extrapolation is necessary to avoid fine-tuning the distribution of central engine activity times with the breakout time, which are presumably unrelated. We speculate that central engines launching relativistic jets may operate in all Type Ib/c SNe. In this case, the existence of a common central engine would imply that (i) the jet may significantly contribute to the energy of the SN; (ii) various observational signatures, like the asphericity of the explosion, could be directly related to jet's interaction with the star.</description><subject>Asphericity</subject><subject>Collapse</subject><subject>Gamma ray bursts</subject><subject>Gamma rays</subject><subject>Luminosity</subject><subject>Massive stars</subject><subject>Physics - High Energy Astrophysical Phenomena</subject><subject>Power law</subject><subject>Public enterprise</subject><subject>Supernovae</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNotj1tLwzAAhYMgOOZ-gE8GfG6XS5OmTzLLnMOC4PZecuvoWJOatsP--9XNpwMfh8P5AHjCKE4EY2gpw299jnGKWIwQEfgOzAilOBIJIQ9g0XVHNHGeEsboDHyuYO6bxjuYW9cHeYJrd6idhZUPsPDuADeyaST8liN8G0LXd1A6A_dja-FWLTXcDa0Nzp-lfX0E95U8dXbxn3Owe1_v84-o-Nps81URSUbSiArNjUUmEYJykWGFmMTK6CxTBk2cksQwTbVGUvPM2gprpDhnlVCGGEzn4Pm2ehUt21A3Mozln3B5FZ4aL7dGG_zPYLu-PPohuOlSSVDKWco4TekFpUVXWA</recordid><startdate>20170810</startdate><enddate>20170810</enddate><creator>Sobacchi, E</creator><creator>Granot, J</creator><creator>Bromberg, O</creator><creator>Sormani, M C</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20170810</creationdate><title>A Common Central Engine for Long Gamma Ray Bursts and Type Ib/c Supernovae?</title><author>Sobacchi, E ; Granot, J ; Bromberg, O ; Sormani, M C</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a527-38c6de0d48836891b05a1bdc99bd0e0d324d5c3cc0ac69eef1c0b665f8bd2d13</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Asphericity</topic><topic>Collapse</topic><topic>Gamma ray bursts</topic><topic>Gamma rays</topic><topic>Luminosity</topic><topic>Massive stars</topic><topic>Physics - High Energy Astrophysical Phenomena</topic><topic>Power law</topic><topic>Public enterprise</topic><topic>Supernovae</topic><toplevel>online_resources</toplevel><creatorcontrib>Sobacchi, E</creatorcontrib><creatorcontrib>Granot, J</creatorcontrib><creatorcontrib>Bromberg, O</creatorcontrib><creatorcontrib>Sormani, M C</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sobacchi, E</au><au>Granot, J</au><au>Bromberg, O</au><au>Sormani, M C</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A Common Central Engine for Long Gamma Ray Bursts and Type Ib/c Supernovae?</atitle><jtitle>arXiv.org</jtitle><date>2017-08-10</date><risdate>2017</risdate><eissn>2331-8422</eissn><abstract>Long-duration, spectrally-soft Gamma-Ray Bursts (GRBs) are associated with Type Ic Core Collapse (CC) Supernovae (SNe), and thus arise from the death of massive stars. In the collapsar model, the jet launched by the central engine must bore its way out of the progenitor star before it can produce a GRB. Most of these jets do not break out, and are instead "choked" inside the star, as the central-engine activity time, \(t_{\rm e}\), is not long enough. Modelling the long-soft GRB duration distribution assuming a power-law distribution for their central-engine activity times, \(\propto t_{\rm e}^{-\alpha}\) for \(t_{\rm e}>t_{\rm b}\), we find a steep distribution (\(\alpha\sim4\)) and a typical GRB jet breakout time of \(t_{\rm b}\sim 60\text{ s}\) in the star's frame. The latter suggests the presence of a low-density, extended envelope surrounding the progenitor star, similar to that previously inferred for low-luminosity GRBs. Extrapolating the range of validity of this power law below what is directly observable, to \(t_{\rm e}<t_{\rm b}\), by only a factor of \(\sim\)4-5 produces enough events to account for all Type Ib/c SNe. Such extrapolation is necessary to avoid fine-tuning the distribution of central engine activity times with the breakout time, which are presumably unrelated. We speculate that central engines launching relativistic jets may operate in all Type Ib/c SNe. In this case, the existence of a common central engine would imply that (i) the jet may significantly contribute to the energy of the SN; (ii) various observational signatures, like the asphericity of the explosion, could be directly related to jet's interaction with the star.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1705.00281</doi><oa>free_for_read</oa></addata></record> |
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subjects | Asphericity Collapse Gamma ray bursts Gamma rays Luminosity Massive stars Physics - High Energy Astrophysical Phenomena Power law Public enterprise Supernovae |
title | A Common Central Engine for Long Gamma Ray Bursts and Type Ib/c Supernovae? |
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