Relativity and the evolution of the Galactic center S-star orbits
We consider the orbital evolution of the S-stars, the young main-sequence stars near the supermassive black hole (SBH) at the Galactic center (GC), and put constraints on competing models for their origin. Our analysis includes for the first time the joint effects of Newtonian and relativistic pertu...
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Published in | arXiv.org |
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Main Authors | , |
Format | Paper Journal Article |
Language | English |
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07.01.2013
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ISSN | 2331-8422 |
DOI | 10.48550/arxiv.1211.4594 |
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Abstract | We consider the orbital evolution of the S-stars, the young main-sequence stars near the supermassive black hole (SBH) at the Galactic center (GC), and put constraints on competing models for their origin. Our analysis includes for the first time the joint effects of Newtonian and relativistic perturbations to the motion, including the dragging of inertial frames by a spinning SBH as well as torques due to finite-N asymmetries in the field-star distribution (resonant relaxation, RR). The evolution of the S-star orbits is strongly influenced by the Schwarzschild barrier (SB), the locus in the (E,L) plane where RR is ineffective at driving orbits to higher eccentricities. Formation models that invoke tidal disruption of binary stars by the SBH tend to place stars below (i.e., at higher eccentricities than) the SB; some stars remain below the barrier, but most stars are able to penetrate it, after which they are subject to RR and achieve a nearly thermal distribution of eccentricities. This process requires roughly 50 Myr in nuclear models with relaxed stellar cusps, or >~10 Myr, regardless of the initial distribution of eccentricities, in nuclear models that include a dense cluster of 10 M_Sun black holes. We find a probability of <~1% for any S-star to be tidally disrupted by the SBH over its lifetime. |
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AbstractList | We consider the orbital evolution of the S-stars, the young main-sequence
stars near the supermassive black hole (SBH) at the Galactic center (GC), and
put constraints on competing models for their origin. Our analysis includes for
the first time the joint effects of Newtonian and relativistic perturbations to
the motion, including the dragging of inertial frames by a spinning SBH as well
as torques due to finite-N asymmetries in the field-star distribution (resonant
relaxation, RR). The evolution of the S-star orbits is strongly influenced by
the Schwarzschild barrier (SB), the locus in the (E,L) plane where RR is
ineffective at driving orbits to higher eccentricities. Formation models that
invoke tidal disruption of binary stars by the SBH tend to place stars below
(i.e., at higher eccentricities than) the SB; some stars remain below the
barrier, but most stars are able to penetrate it, after which they are subject
to RR and achieve a nearly thermal distribution of eccentricities. This process
requires roughly 50 Myr in nuclear models with relaxed stellar cusps, or >~10
Myr, regardless of the initial distribution of eccentricities, in nuclear
models that include a dense cluster of 10 M_Sun black holes. We find a
probability of <~1% for any S-star to be tidally disrupted by the SBH over its
lifetime. We consider the orbital evolution of the S-stars, the young main-sequence stars near the supermassive black hole (SBH) at the Galactic center (GC), and put constraints on competing models for their origin. Our analysis includes for the first time the joint effects of Newtonian and relativistic perturbations to the motion, including the dragging of inertial frames by a spinning SBH as well as torques due to finite-N asymmetries in the field-star distribution (resonant relaxation, RR). The evolution of the S-star orbits is strongly influenced by the Schwarzschild barrier (SB), the locus in the (E,L) plane where RR is ineffective at driving orbits to higher eccentricities. Formation models that invoke tidal disruption of binary stars by the SBH tend to place stars below (i.e., at higher eccentricities than) the SB; some stars remain below the barrier, but most stars are able to penetrate it, after which they are subject to RR and achieve a nearly thermal distribution of eccentricities. This process requires roughly 50 Myr in nuclear models with relaxed stellar cusps, or >~10 Myr, regardless of the initial distribution of eccentricities, in nuclear models that include a dense cluster of 10 M_Sun black holes. We find a probability of <~1% for any S-star to be tidally disrupted by the SBH over its lifetime. |
Author | Merritt, David Antonini, Fabio |
Author_xml | – sequence: 1 givenname: Fabio surname: Antonini fullname: Antonini, Fabio – sequence: 2 givenname: David surname: Merritt fullname: Merritt, David |
BackLink | https://doi.org/10.48550/arXiv.1211.4594$$DView paper in arXiv https://doi.org/10.1088/2041-8205/763/1/L10$$DView published paper (Access to full text may be restricted) |
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Snippet | We consider the orbital evolution of the S-stars, the young main-sequence stars near the supermassive black hole (SBH) at the Galactic center (GC), and put... We consider the orbital evolution of the S-stars, the young main-sequence stars near the supermassive black hole (SBH) at the Galactic center (GC), and put... |
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SubjectTerms | Astronomical models Binary stars Constraint modelling Cusps Disruption Eccentric orbits Galactic evolution Globular clusters Main sequence stars Nuclear models Orbital mechanics Physics - Astrophysics of Galaxies Physics - General Relativity and Quantum Cosmology Relativity Star & galaxy formation Star distribution Stellar evolution |
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Title | Relativity and the evolution of the Galactic center S-star orbits |
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