Misaligned Jets from Sgr A* and the Origin of Fermi/eROSITA Bubbles

One of the leading explanations for the origin of Fermi Bubbles is past jet activity in the Galactic center supermassive black hole Sgr A ^* . The claimed jets are often assumed to be perpendicular to the Galactic plane. Motivated by the orientation of pc-scale nuclear stellar disk and gas streams,...

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Main Authors: Kartick C. Sarkar, Santanu Mondal, Prateek Sharma, Tsvi Piran
Format: Article
Language:English
Published: IOP Publishing 2023-01-01
Series:The Astrophysical Journal
Subjects:
Online Access:https://doi.org/10.3847/1538-4357/acd75d
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author Kartick C. Sarkar
Santanu Mondal
Prateek Sharma
Tsvi Piran
author_facet Kartick C. Sarkar
Santanu Mondal
Prateek Sharma
Tsvi Piran
author_sort Kartick C. Sarkar
collection DOAJ
description One of the leading explanations for the origin of Fermi Bubbles is past jet activity in the Galactic center supermassive black hole Sgr A ^* . The claimed jets are often assumed to be perpendicular to the Galactic plane. Motivated by the orientation of pc-scale nuclear stellar disk and gas streams, as well as a low inclination of the accretion disk around Sgr A ^* inferred by the Event Horizon Telescope, we perform hydrodynamical simulations of nuclear jets significantly tilted relative to the Galactic rotation axis. The observed axisymmetry and hemisymmetry (north–south symmetry) of Fermi/eROSITA bubbles (FEBs) due to quasi-steady jets in Sgr A ^* could be produced if the jet had a super-Eddington power (≳5 × 10 ^44 erg s ^−1 ) for a short time (jet active period ≲6 kyr) for a reasonable jet opening angle (≲10°). Such powerful explosions are, however, incompatible with the observed O viii /O vii line ratio toward the bubbles, even after considering electron–proton temperature nonequilibrium. We argue that the only remaining options for producing FEBs are (i) a low-luminosity (≈10 ^40.5−41 erg s ^−1 ) magnetically dominated jet or accretion wind from the Sgr A ^* , or (ii) a supernovae or tidal disruption event driven wind of a similar luminosity from the Galactic center.
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spelling doaj.art-1cb18d3c2b7d45a082cef722545446072024-01-05T14:50:56ZengIOP PublishingThe Astrophysical Journal1538-43572023-01-0195113610.3847/1538-4357/acd75dMisaligned Jets from Sgr A* and the Origin of Fermi/eROSITA BubblesKartick C. Sarkar0https://orcid.org/0000-0002-7767-8472Santanu Mondal1https://orcid.org/0000-0003-0793-6066Prateek Sharma2https://orcid.org/0000-0003-2635-4643Tsvi Piran3https://orcid.org/0000-0002-7964-5420School of Physics and Astronomy, Tel Aviv University , Tel Aviv, Israel ; kcsarkar@tauex.tau.ac.il, kartick.c.sarkar100@gmail.com; Racah Institute of Physics, The Hebrew University of Jerusalem , IsraelIndian Institute of Astrophysics , 2nd Block, Koramangala, Bangalore 560034, IndiaDepartment of Physics and Joint Astronomy Program, Indian Institute of Science , Bangalore 560012, IndiaRacah Institute of Physics, The Hebrew University of Jerusalem , IsraelOne of the leading explanations for the origin of Fermi Bubbles is past jet activity in the Galactic center supermassive black hole Sgr A ^* . The claimed jets are often assumed to be perpendicular to the Galactic plane. Motivated by the orientation of pc-scale nuclear stellar disk and gas streams, as well as a low inclination of the accretion disk around Sgr A ^* inferred by the Event Horizon Telescope, we perform hydrodynamical simulations of nuclear jets significantly tilted relative to the Galactic rotation axis. The observed axisymmetry and hemisymmetry (north–south symmetry) of Fermi/eROSITA bubbles (FEBs) due to quasi-steady jets in Sgr A ^* could be produced if the jet had a super-Eddington power (≳5 × 10 ^44 erg s ^−1 ) for a short time (jet active period ≲6 kyr) for a reasonable jet opening angle (≲10°). Such powerful explosions are, however, incompatible with the observed O viii /O vii line ratio toward the bubbles, even after considering electron–proton temperature nonequilibrium. We argue that the only remaining options for producing FEBs are (i) a low-luminosity (≈10 ^40.5−41 erg s ^−1 ) magnetically dominated jet or accretion wind from the Sgr A ^* , or (ii) a supernovae or tidal disruption event driven wind of a similar luminosity from the Galactic center.https://doi.org/10.3847/1538-4357/acd75dJetsMilky Way GalaxyGalactic centerCircumgalactic mediumDiffuse x-ray backgroundHydrodynamical simulations
spellingShingle Kartick C. Sarkar
Santanu Mondal
Prateek Sharma
Tsvi Piran
Misaligned Jets from Sgr A* and the Origin of Fermi/eROSITA Bubbles
The Astrophysical Journal
Jets
Milky Way Galaxy
Galactic center
Circumgalactic medium
Diffuse x-ray background
Hydrodynamical simulations
title Misaligned Jets from Sgr A* and the Origin of Fermi/eROSITA Bubbles
title_full Misaligned Jets from Sgr A* and the Origin of Fermi/eROSITA Bubbles
title_fullStr Misaligned Jets from Sgr A* and the Origin of Fermi/eROSITA Bubbles
title_full_unstemmed Misaligned Jets from Sgr A* and the Origin of Fermi/eROSITA Bubbles
title_short Misaligned Jets from Sgr A* and the Origin of Fermi/eROSITA Bubbles
title_sort misaligned jets from sgr a and the origin of fermi erosita bubbles
topic Jets
Milky Way Galaxy
Galactic center
Circumgalactic medium
Diffuse x-ray background
Hydrodynamical simulations
url https://doi.org/10.3847/1538-4357/acd75d
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AT tsvipiran misalignedjetsfromsgraandtheoriginoffermierositabubbles