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, and put constraints on competing models for their origin. Our analysis includes for the first time the joint effects of Newtonian and relativistic perturbati...
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Published in | Astrophysical journal. Letters Vol. 763; no. 1; pp. L10 - 6 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
United States
20.01.2013
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Subjects | |
Online Access | Get full text |
ISSN | 2041-8205 2041-8213 |
DOI | 10.1088/2041-8205/763/1/L10 |
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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, 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 sub([middot in circle]) blackholes. 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, 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 sub([middot in circle]) blackholes. 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, 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 {approx}> 10 Myr, regardless of the initial distribution of eccentricities, in nuclear models that include a dense cluster of 10 M{sub Sun} black holes. We find a probability of {approx}< 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://www.osti.gov/biblio/22078323$$D View this record in Osti.gov |
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SubjectTerms | Astronomical models ASTROPHYSICS, COSMOLOGY AND ASTRONOMY ASYMMETRY Barriers BINARY STARS BLACK HOLES CUSPED GEOMETRIES Cusps DISTURBANCES Eccentric orbits Eccentricity GALACTIC EVOLUTION LIFETIME MAIN SEQUENCE STARS NUCLEAR MODELS Orbits PROBABILITY RELATIVISTIC RANGE RELAXATION SCHWARZSCHILD METRIC Stars TORQUE |
Title | RELATIVITY AND THE EVOLUTION OF THE GALACTIC CENTER S-STAR ORBITS |
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