Probing the gas density in our Galactic Centre: moving mesh simulations of G2

Abstract The G2 object has recently passed its pericentre passage in our Galactic Centre. While the Brγ emission shows clear signs of tidal interaction, the change in the observed luminosity is only of about a factor of 2, in contention with all previous predictions. We present high-resolution simul...

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Veröffentlicht in:Monthly notices of the Royal Astronomical Society 2018-01, Vol.473 (2), p.1841-1849
Hauptverfasser: Steinberg, Elad, Sari, Re'em, Gnat, Orly, Gillessen, Stefan, Plewa, Philipp, Genzel, Reinhard, Eisenhauer, Frank, Ott, Thomas, Pfuhl, Oliver, Habibi, Maryam, Waisberg, Idel, von Fellenberg, Sebastiano, Dexter, Jason, Bauböck, Michi, Rosales, Alejandra Jimenez
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container_end_page 1849
container_issue 2
container_start_page 1841
container_title Monthly notices of the Royal Astronomical Society
container_volume 473
creator Steinberg, Elad
Sari, Re'em
Gnat, Orly
Gillessen, Stefan
Plewa, Philipp
Genzel, Reinhard
Eisenhauer, Frank
Ott, Thomas
Pfuhl, Oliver
Habibi, Maryam
Waisberg, Idel
von Fellenberg, Sebastiano
Dexter, Jason
Bauböck, Michi
Rosales, Alejandra Jimenez
description Abstract The G2 object has recently passed its pericentre passage in our Galactic Centre. While the Brγ emission shows clear signs of tidal interaction, the change in the observed luminosity is only of about a factor of 2, in contention with all previous predictions. We present high-resolution simulations performed with the moving mesh code, RICH, together with simple analytical arguments that reproduce the observed Brγ emission. In our model, G2 is a gas cloud that undergoes tidal disruption in a dilute ambient medium. We find that during pericentre passage, the efficient cooling of the cloud results in a vertical collapse, compressing the cloud by a factor of ∼5000. By properly taking into account the ionization state of the gas, we find that the cloud is UV starved and are able to reproduce the observed Brγ luminosity. For densities larger than ≈500 cm−3 at pericentre, the cloud fragments due to cooling instabilities and the emitted radiation is inconsistent with observations. For lower densities, the cloud survives the pericentre passage intact and its emitted radiation matches the observed light curve. From the duration of Brγ emission that contains both redshifted and blueshifted components, we show that the cloud is not spherical but rather elongated with a size ratio of 4 at year 2001. The simulated cloud's elongation grows as it travels towards pericentre and is consistent with observations, due to viewing angles. The simulation is also consistent with having a spherical shape at apocentre.
doi_str_mv 10.1093/mnras/stx2438
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While the Brγ emission shows clear signs of tidal interaction, the change in the observed luminosity is only of about a factor of 2, in contention with all previous predictions. We present high-resolution simulations performed with the moving mesh code, RICH, together with simple analytical arguments that reproduce the observed Brγ emission. In our model, G2 is a gas cloud that undergoes tidal disruption in a dilute ambient medium. We find that during pericentre passage, the efficient cooling of the cloud results in a vertical collapse, compressing the cloud by a factor of ∼5000. By properly taking into account the ionization state of the gas, we find that the cloud is UV starved and are able to reproduce the observed Brγ luminosity. For densities larger than ≈500 cm−3 at pericentre, the cloud fragments due to cooling instabilities and the emitted radiation is inconsistent with observations. For lower densities, the cloud survives the pericentre passage intact and its emitted radiation matches the observed light curve. From the duration of Brγ emission that contains both redshifted and blueshifted components, we show that the cloud is not spherical but rather elongated with a size ratio of 4 at year 2001. The simulated cloud's elongation grows as it travels towards pericentre and is consistent with observations, due to viewing angles. 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For lower densities, the cloud survives the pericentre passage intact and its emitted radiation matches the observed light curve. From the duration of Brγ emission that contains both redshifted and blueshifted components, we show that the cloud is not spherical but rather elongated with a size ratio of 4 at year 2001. The simulated cloud's elongation grows as it travels towards pericentre and is consistent with observations, due to viewing angles. 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subjects Clouds
Computer simulation
Cooling
Disruption
Elongation
Emission analysis
Finite element method
Gas density
Ionization
Light curve
Luminosity
Radiation
title Probing the gas density in our Galactic Centre: moving mesh simulations of G2
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