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A Self-Gravitating Exoring Around J1407b and Implications for In-Situ Exomoon Formation
We perform simulations of the M ⊕ self-gravitating exoring thought to orbit the large exoplanet J1407b. We use a mass of M J 1407 b = 20 M J (which is close to the revised upper limit) and a semi-major axis of a = 5 A U , equating to an orbital period of ∼ 11 y r s about the primary. As J1407b is ex...
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Published in: | Frontiers in astronomy and space sciences 2022-03, Vol.9 |
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container_title | Frontiers in astronomy and space sciences |
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creator | Sutton, Phil J Albery, Brayden Muff, Jake |
description | We perform simulations of the
M
⊕
self-gravitating exoring thought to orbit the large exoplanet J1407b. We use a mass of
M
J
1407
b
=
20
M
J
(which is close to the revised upper limit) and a semi-major axis of
a
=
5
A
U
, equating to an orbital period of
∼
11
y
r
s
about the primary. As J1407b is expected to have a high eccentricity, we test eight different models: where e = 0.2, 0.4, 0.6 and 0.8 in both the prograde and retrograde configurations. All prograde models show a strongly perturbed ring within the first orbit. As expected, the retrograde rings demonstrate a higher degree of stability, with the lower eccentricity models (e = 0.2 and 0.4) able to survive multiple orbits. However, even the higher eccentricity (e = 0.6 and 0.8) retrograde models quickly result in the loss of the ring after 200 years. Excitation of eccentricities in all retrograde rings are stable to gravitational collapse. When assuming the most recent mass estimate of
M
J
1407
b
=
20
M
J
the ring is unfavourable to the accretion of moons when J1407b is on an elliptical orbit. An interesting consequence of the strong perturbation for one model (retrograde and e = 0.6) during the first close passage is a transient gap located at 0.4AU. This is the same location as the inferred gap from the single transit in 2007 and does not require a nearby exomoon. |
doi_str_mv | 10.3389/fspas.2022.819933 |
format | article |
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M
⊕
self-gravitating exoring thought to orbit the large exoplanet J1407b. We use a mass of
M
J
1407
b
=
20
M
J
(which is close to the revised upper limit) and a semi-major axis of
a
=
5
A
U
, equating to an orbital period of
∼
11
y
r
s
about the primary. As J1407b is expected to have a high eccentricity, we test eight different models: where e = 0.2, 0.4, 0.6 and 0.8 in both the prograde and retrograde configurations. All prograde models show a strongly perturbed ring within the first orbit. As expected, the retrograde rings demonstrate a higher degree of stability, with the lower eccentricity models (e = 0.2 and 0.4) able to survive multiple orbits. However, even the higher eccentricity (e = 0.6 and 0.8) retrograde models quickly result in the loss of the ring after 200 years. Excitation of eccentricities in all retrograde rings are stable to gravitational collapse. When assuming the most recent mass estimate of
M
J
1407
b
=
20
M
J
the ring is unfavourable to the accretion of moons when J1407b is on an elliptical orbit. An interesting consequence of the strong perturbation for one model (retrograde and e = 0.6) during the first close passage is a transient gap located at 0.4AU. This is the same location as the inferred gap from the single transit in 2007 and does not require a nearby exomoon.</description><identifier>ISSN: 2296-987X</identifier><identifier>EISSN: 2296-987X</identifier><identifier>DOI: 10.3389/fspas.2022.819933</identifier><language>eng</language><publisher>Frontiers Media S.A</publisher><subject>Exomoon ; Exoplanet ; Exoring ; moon formation ; planetary Ring</subject><ispartof>Frontiers in astronomy and space sciences, 2022-03, Vol.9</ispartof><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c284t-1ab9cb47b4adbd3c15bbb162db66830abba47ada739efd9369e185f658e75c7a3</citedby><cites>FETCH-LOGICAL-c284t-1ab9cb47b4adbd3c15bbb162db66830abba47ada739efd9369e185f658e75c7a3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,777,781,27905,27906</link.rule.ids></links><search><creatorcontrib>Sutton, Phil J</creatorcontrib><creatorcontrib>Albery, Brayden</creatorcontrib><creatorcontrib>Muff, Jake</creatorcontrib><title>A Self-Gravitating Exoring Around J1407b and Implications for In-Situ Exomoon Formation</title><title>Frontiers in astronomy and space sciences</title><description>We perform simulations of the
M
⊕
self-gravitating exoring thought to orbit the large exoplanet J1407b. We use a mass of
M
J
1407
b
=
20
M
J
(which is close to the revised upper limit) and a semi-major axis of
a
=
5
A
U
, equating to an orbital period of
∼
11
y
r
s
about the primary. As J1407b is expected to have a high eccentricity, we test eight different models: where e = 0.2, 0.4, 0.6 and 0.8 in both the prograde and retrograde configurations. All prograde models show a strongly perturbed ring within the first orbit. As expected, the retrograde rings demonstrate a higher degree of stability, with the lower eccentricity models (e = 0.2 and 0.4) able to survive multiple orbits. However, even the higher eccentricity (e = 0.6 and 0.8) retrograde models quickly result in the loss of the ring after 200 years. Excitation of eccentricities in all retrograde rings are stable to gravitational collapse. When assuming the most recent mass estimate of
M
J
1407
b
=
20
M
J
the ring is unfavourable to the accretion of moons when J1407b is on an elliptical orbit. An interesting consequence of the strong perturbation for one model (retrograde and e = 0.6) during the first close passage is a transient gap located at 0.4AU. This is the same location as the inferred gap from the single transit in 2007 and does not require a nearby exomoon.</description><subject>Exomoon</subject><subject>Exoplanet</subject><subject>Exoring</subject><subject>moon formation</subject><subject>planetary Ring</subject><issn>2296-987X</issn><issn>2296-987X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><sourceid>DOA</sourceid><recordid>eNpNkMtKw0AUhgdRsGgfwF1eIHUuyVyWpbQ1UnBRRXfDmZlMSUkyZSYVfXubVsTV_3Mu3-JD6IHgGWNSPfp0gDSjmNKZJEoxdoUmlCqeKyk-rv_1WzRNaY8xJlJIxdkEvc-zbd36fB3hsxlgaPpdtvwKccx5DMfeZc-kwMJkcKpVd2gbe7oKfcp8iFnV59tmOI4vXQh9tgqxO6_v0Y2HNtXT37xDb6vl6-Ip37ysq8V8k1sqiyEnYJQ1hTAFOOOYJaUxhnDqDOeSYTAGCgEOBFO1d4pxVRNZel7KWpRWALtD1YXrAuz1ITYdxG8doNHnQYg7DXFobFtrYXHJgRinOCmc9aAYcYRQZoDLkpETi1xYNoaUYu3_eATrUbQ-i9ajaH0RzX4AlF1yYg</recordid><startdate>20220314</startdate><enddate>20220314</enddate><creator>Sutton, Phil J</creator><creator>Albery, Brayden</creator><creator>Muff, Jake</creator><general>Frontiers Media S.A</general><scope>AAYXX</scope><scope>CITATION</scope><scope>DOA</scope></search><sort><creationdate>20220314</creationdate><title>A Self-Gravitating Exoring Around J1407b and Implications for In-Situ Exomoon Formation</title><author>Sutton, Phil J ; Albery, Brayden ; Muff, Jake</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c284t-1ab9cb47b4adbd3c15bbb162db66830abba47ada739efd9369e185f658e75c7a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Exomoon</topic><topic>Exoplanet</topic><topic>Exoring</topic><topic>moon formation</topic><topic>planetary Ring</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Sutton, Phil J</creatorcontrib><creatorcontrib>Albery, Brayden</creatorcontrib><creatorcontrib>Muff, Jake</creatorcontrib><collection>CrossRef</collection><collection>DOAJ Directory of Open Access Journals</collection><jtitle>Frontiers in astronomy and space sciences</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sutton, Phil J</au><au>Albery, Brayden</au><au>Muff, Jake</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A Self-Gravitating Exoring Around J1407b and Implications for In-Situ Exomoon Formation</atitle><jtitle>Frontiers in astronomy and space sciences</jtitle><date>2022-03-14</date><risdate>2022</risdate><volume>9</volume><issn>2296-987X</issn><eissn>2296-987X</eissn><abstract>We perform simulations of the
M
⊕
self-gravitating exoring thought to orbit the large exoplanet J1407b. We use a mass of
M
J
1407
b
=
20
M
J
(which is close to the revised upper limit) and a semi-major axis of
a
=
5
A
U
, equating to an orbital period of
∼
11
y
r
s
about the primary. As J1407b is expected to have a high eccentricity, we test eight different models: where e = 0.2, 0.4, 0.6 and 0.8 in both the prograde and retrograde configurations. All prograde models show a strongly perturbed ring within the first orbit. As expected, the retrograde rings demonstrate a higher degree of stability, with the lower eccentricity models (e = 0.2 and 0.4) able to survive multiple orbits. However, even the higher eccentricity (e = 0.6 and 0.8) retrograde models quickly result in the loss of the ring after 200 years. Excitation of eccentricities in all retrograde rings are stable to gravitational collapse. When assuming the most recent mass estimate of
M
J
1407
b
=
20
M
J
the ring is unfavourable to the accretion of moons when J1407b is on an elliptical orbit. An interesting consequence of the strong perturbation for one model (retrograde and e = 0.6) during the first close passage is a transient gap located at 0.4AU. This is the same location as the inferred gap from the single transit in 2007 and does not require a nearby exomoon.</abstract><pub>Frontiers Media S.A</pub><doi>10.3389/fspas.2022.819933</doi><oa>free_for_read</oa></addata></record> |
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subjects | Exomoon Exoplanet Exoring moon formation planetary Ring |
title | A Self-Gravitating Exoring Around J1407b and Implications for In-Situ Exomoon Formation |
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