Abstract

ABSTRACT Jets launched by active galactic nuclei (AGN) are believed to play a significant role in shaping the properties of galaxies and provide an energetically viable mechanism through which galaxies can become quenched. Here, we present a novel AGN feedback model, which we have incorporated into the arepo code, that evolves the black hole mass and spin as the accretion flow proceeds through a thin α-disc that we self-consistently couple to a Blandford–Znajek jet. We apply our model to the central region of a typical radio-loud Seyfert galaxy embedded in a hot circumgalactic medium (CGM). We find that jets launched into high-pressure environments thermalize efficiently due to the formation of recollimation shocks and the vigorous instabilities that these shocks excite increase the efficiency of the mixing of CGM and jet material. The beams of more overpressured jets, however, are not as readily disrupted by instabilities so the majority of the momentum flux at the jet base is retained out to the head, where the jet terminates in a reverse shock. All jets entrain a significant amount of cold circumnuclear disc material that, while energetically insignificant, dominates the lobe mass together with the hot, entrained CGM material. The jet power evolves significantly due to effective self-regulation by the black hole, fed by secularly driven, intermittent mass flows. The direction of jets launched directly into the circumnuclear disc changes considerably due to effective Bardeen–Petterson torquing. Interestingly, these jets obliterate the innermost regions of the disc and drive large-scale, multiphase, turbulent, bipolar outflows.

Highlights

  • In the centres of many galaxy clusters the hot, X-ray emitting gas is observed to have rapid ( 1 Gyr) cooling times

  • In this work we aim to improve on existing models of active galactic nuclei (AGN) jet feedback in galaxy-scale simulations by self-consistently predicting the jet power and direction based on the black hole properties and those of the surrounding accretion flow

  • An estimate for the mass accretion rate is determined from the gas properties in the simulation and there are a variety of ways of making such an estimate in the literature; for example, Dubois et al (2010, 2012) adopt the Bondi-Hoyle-like accretion rate as a measure of the hot gas accretion rate, while (Yang & Reynolds 2016b; Li et al 2017, 2015; Li & Bryan 2014b) have prescriptions for cold gas accretion via a gas dropout time

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Summary

Introduction

In the centres of many galaxy clusters the hot, X-ray emitting gas is observed to have rapid ( 1 Gyr) cooling times. Without invoking some heating mechanism, significant quantities of cold gas should flow towards the centre of these clusters (Peterson & Fabian 2006; Fabian 1994) Many such clusters, do not show evidence of high levels of star formation (Cooke et al 2016; Donahue et al 2010) nor do they have large reservoirs of molecular gas (Fogarty et al 2019; Russell et al 2019, 2017), both of which should be present if such a cooling flow were to exist. Jet feedback from the AGN associated with the central brightest cluster galaxy is often invoked as such a mechanism (McNamara & Nulsen 2012, 2007) and in many cases there is direct observational evidence of the interaction of jet lobes with the surrounding medium with estimated cavity energies comparable to that required to offset catastrophic cooling.

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