Stellar Revival and Repeated Flares in Deeply Plunging Tidal Disruption Events
Tidal disruption events with tidal radius r t and pericenter distance r p are characterized by the quantity β = r t / r p , and “deep encounters” have β ≫ 1. It has been assumed that there is a critical β ≡ β c ∼ 1 that differentiates between partial and full disruption: for β < β c a fraction of...
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description | Tidal disruption events with tidal radius
r
t
and pericenter distance
r
p
are characterized by the quantity
β
=
r
t
/
r
p
, and “deep encounters” have
β
≫ 1. It has been assumed that there is a critical
β
≡
β
c
∼ 1 that differentiates between partial and full disruption: for
β
<
β
c
a fraction of the star survives the tidal interaction with the black hole, while for
β
>
β
c
the star is completely destroyed, and hence all deep encounters should be full. Here we show that this assumption is incorrect by providing an example of a
β
= 16 encounter between a
γ
= 5/3, solar-like polytrope and a 10
6
M
⊙
black hole—for which previous investigations have found
β
c
≃ 0.9—that results in the reformation of a stellar core post-disruption that comprises approximately 25% of the original stellar mass. We propose that the core reforms under self-gravity, which remains important because of the compression of the gas both near pericenter, where the compression occurs out of the orbital plane, and substantially after pericenter, where compression is within the plane. We find that the core forms on a bound orbit about the black hole, and we discuss the corresponding implications of our findings in the context of recently observed, repeating nuclear transients. |
doi_str_mv | 10.3847/2041-8213/ac5118 |
format | Article |
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r
t
and pericenter distance
r
p
are characterized by the quantity
β
=
r
t
/
r
p
, and “deep encounters” have
β
≫ 1. It has been assumed that there is a critical
β
≡
β
c
∼ 1 that differentiates between partial and full disruption: for
β
<
β
c
a fraction of the star survives the tidal interaction with the black hole, while for
β
>
β
c
the star is completely destroyed, and hence all deep encounters should be full. Here we show that this assumption is incorrect by providing an example of a
β
= 16 encounter between a
γ
= 5/3, solar-like polytrope and a 10
6
M
⊙
black hole—for which previous investigations have found
β
c
≃ 0.9—that results in the reformation of a stellar core post-disruption that comprises approximately 25% of the original stellar mass. We propose that the core reforms under self-gravity, which remains important because of the compression of the gas both near pericenter, where the compression occurs out of the orbital plane, and substantially after pericenter, where compression is within the plane. We find that the core forms on a bound orbit about the black hole, and we discuss the corresponding implications of our findings in the context of recently observed, repeating nuclear transients.</description><identifier>ISSN: 2041-8205</identifier><identifier>EISSN: 2041-8213</identifier><identifier>DOI: 10.3847/2041-8213/ac5118</identifier><language>eng</language><publisher>Austin: The American Astronomical Society</publisher><subject>Astrophysical black holes ; Black hole physics ; Black holes ; Disruption ; Hydrodynamical simulations ; Stellar mass ; Supermassive black holes ; Tidal disruption ; Tidal interaction</subject><ispartof>Astrophysical journal. Letters, 2022-03, Vol.927 (2), p.L25</ispartof><rights>2022. The Author(s). Published by the American Astronomical Society.</rights><rights>2022. The Author(s). Published by the American Astronomical Society. This work is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c381t-b3fc8f8df6a5774e36bbdf47792fc7fe58447b0c0dee681d30222ef78d8b060a3</citedby><cites>FETCH-LOGICAL-c381t-b3fc8f8df6a5774e36bbdf47792fc7fe58447b0c0dee681d30222ef78d8b060a3</cites><orcidid>0000-0002-2137-4146 ; 0000-0003-3765-6401</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.3847/2041-8213/ac5118/pdf$$EPDF$$P50$$Giop$$Hfree_for_read</linktopdf><link.rule.ids>314,780,784,864,27924,27925,38868,38890,53840,53867</link.rule.ids></links><search><creatorcontrib>Nixon, C. J.</creatorcontrib><creatorcontrib>Coughlin, Eric R.</creatorcontrib><title>Stellar Revival and Repeated Flares in Deeply Plunging Tidal Disruption Events</title><title>Astrophysical journal. Letters</title><addtitle>APJL</addtitle><addtitle>Astrophys. J. Lett</addtitle><description>Tidal disruption events with tidal radius
r
t
and pericenter distance
r
p
are characterized by the quantity
β
=
r
t
/
r
p
, and “deep encounters” have
β
≫ 1. It has been assumed that there is a critical
β
≡
β
c
∼ 1 that differentiates between partial and full disruption: for
β
<
β
c
a fraction of the star survives the tidal interaction with the black hole, while for
β
>
β
c
the star is completely destroyed, and hence all deep encounters should be full. Here we show that this assumption is incorrect by providing an example of a
β
= 16 encounter between a
γ
= 5/3, solar-like polytrope and a 10
6
M
⊙
black hole—for which previous investigations have found
β
c
≃ 0.9—that results in the reformation of a stellar core post-disruption that comprises approximately 25% of the original stellar mass. We propose that the core reforms under self-gravity, which remains important because of the compression of the gas both near pericenter, where the compression occurs out of the orbital plane, and substantially after pericenter, where compression is within the plane. We find that the core forms on a bound orbit about the black hole, and we discuss the corresponding implications of our findings in the context of recently observed, repeating nuclear transients.</description><subject>Astrophysical black holes</subject><subject>Black hole physics</subject><subject>Black holes</subject><subject>Disruption</subject><subject>Hydrodynamical simulations</subject><subject>Stellar mass</subject><subject>Supermassive black holes</subject><subject>Tidal disruption</subject><subject>Tidal interaction</subject><issn>2041-8205</issn><issn>2041-8213</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><sourceid>O3W</sourceid><recordid>eNp9kM1Lw0AQxRdRsFbvHgOCJ2P3I9ndHqW2KhQVredlk50tW2Ky7iaF_vemROpFPM1j5vdmmIfQJcG3TGZiQnFGUkkJm-gyJ0QeodGhdXzQOD9FZzFuMKaYEzlCz-8tVJUOyRts3VZXia5Nrz3oFkyy6CcQE1cn9wC-2iWvVVevXb1OVs708L2LofOta-pkvoW6jefoxOoqwsVPHaOPxXw1e0yXLw9Ps7tlWjJJ2rRgtpRWGst1LkQGjBeFsZkQU2pLYSGXWSYKXGIDwCUxDFNKwQppZIE51myMroa9PjRfHcRWbZou1P1JRTknGWek_3uM8ECVoYkxgFU-uE8ddopgtU9N7WNR-4jUkFpvuRksrvG_O__Br__Atd9Uakp7Xi1prryx7Bvy4HpM</recordid><startdate>20220301</startdate><enddate>20220301</enddate><creator>Nixon, C. J.</creator><creator>Coughlin, Eric R.</creator><general>The American Astronomical Society</general><general>IOP Publishing</general><scope>O3W</scope><scope>TSCCA</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>8FD</scope><scope>H8D</scope><scope>KL.</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-2137-4146</orcidid><orcidid>https://orcid.org/0000-0003-3765-6401</orcidid></search><sort><creationdate>20220301</creationdate><title>Stellar Revival and Repeated Flares in Deeply Plunging Tidal Disruption Events</title><author>Nixon, C. J. ; Coughlin, Eric R.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c381t-b3fc8f8df6a5774e36bbdf47792fc7fe58447b0c0dee681d30222ef78d8b060a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Astrophysical black holes</topic><topic>Black hole physics</topic><topic>Black holes</topic><topic>Disruption</topic><topic>Hydrodynamical simulations</topic><topic>Stellar mass</topic><topic>Supermassive black holes</topic><topic>Tidal disruption</topic><topic>Tidal interaction</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Nixon, C. J.</creatorcontrib><creatorcontrib>Coughlin, Eric R.</creatorcontrib><collection>IOP Publishing Free Content</collection><collection>IOPscience (Open Access)</collection><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Astrophysical journal. Letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Nixon, C. J.</au><au>Coughlin, Eric R.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Stellar Revival and Repeated Flares in Deeply Plunging Tidal Disruption Events</atitle><jtitle>Astrophysical journal. Letters</jtitle><stitle>APJL</stitle><addtitle>Astrophys. J. Lett</addtitle><date>2022-03-01</date><risdate>2022</risdate><volume>927</volume><issue>2</issue><spage>L25</spage><pages>L25-</pages><issn>2041-8205</issn><eissn>2041-8213</eissn><abstract>Tidal disruption events with tidal radius
r
t
and pericenter distance
r
p
are characterized by the quantity
β
=
r
t
/
r
p
, and “deep encounters” have
β
≫ 1. It has been assumed that there is a critical
β
≡
β
c
∼ 1 that differentiates between partial and full disruption: for
β
<
β
c
a fraction of the star survives the tidal interaction with the black hole, while for
β
>
β
c
the star is completely destroyed, and hence all deep encounters should be full. Here we show that this assumption is incorrect by providing an example of a
β
= 16 encounter between a
γ
= 5/3, solar-like polytrope and a 10
6
M
⊙
black hole—for which previous investigations have found
β
c
≃ 0.9—that results in the reformation of a stellar core post-disruption that comprises approximately 25% of the original stellar mass. We propose that the core reforms under self-gravity, which remains important because of the compression of the gas both near pericenter, where the compression occurs out of the orbital plane, and substantially after pericenter, where compression is within the plane. We find that the core forms on a bound orbit about the black hole, and we discuss the corresponding implications of our findings in the context of recently observed, repeating nuclear transients.</abstract><cop>Austin</cop><pub>The American Astronomical Society</pub><doi>10.3847/2041-8213/ac5118</doi><tpages>4</tpages><orcidid>https://orcid.org/0000-0002-2137-4146</orcidid><orcidid>https://orcid.org/0000-0003-3765-6401</orcidid><oa>free_for_read</oa></addata></record> |
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source | IOP Publishing Free Content; DOAJ Directory of Open Access Journals; EZB-FREE-00999 freely available EZB journals; IOPscience extra; Alma/SFX Local Collection |
subjects | Astrophysical black holes Black hole physics Black holes Disruption Hydrodynamical simulations Stellar mass Supermassive black holes Tidal disruption Tidal interaction |
title | Stellar Revival and Repeated Flares in Deeply Plunging Tidal Disruption Events |
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