Abstract

Gravitational-wave recoil of merging supermassive black holes (SMBHs) may influence the co-evolution of SMBHs and their host galaxies. We examine this possibility using smoothed particle hydrodynamic/N-body simulations of gaseous galaxy mergers, including SMBH accretion, in which the merged BH receives a recoil kick. This enables us to follow the trajectories and accretion of recoiling BHs in self-consistent, evolving merger remnants. In contrast to recent studies on similar topics, we conduct a large parameter study, generating a suite of over 200 simulations with more than 60 merger models and a range of recoil velocities (vk). With this, we can identify systematic trends in the behaviour of recoiling BHs. Our main results are as follows. (1) BHs kicked at nearly the central escape speed (vesc) may oscillate on large orbits for up to a Hubble time, but in gas-rich mergers, BHs kicked with up to ∼0.7vesc may be confined to the central few kpc of the galaxy, owing to gas drag and steep central potentials. (2) vesc in gas-rich mergers may increase rapidly during final coalescence, in which case recoil trajectories may depend sensitively on the timing of the BH merger relative to the formation of the central potential well. Delays of even a few times 107 yr in the BH merger time may substantially suppress recoiling BH motion for a fixed kick speed. (3) Recoil events generally reduce the lifetimes of bright active galactic nuclei (AGNs), but short-period recoil oscillations may actually extend AGN lifetimes at lower luminosities. (4) Bondi–Hoyle accretion dominates recoiling BH growth for vk/vesc≲ 0.6–0.8; for higher vk, the BH accretes primarily from its ejected gas disc, which we model as a time-dependent accretion disc. (5) Kinematically offset AGNs may be observable either immediately after a high-velocity recoil or during pericentric passages through a gas-rich remnant. In either case, AGN lifetimes may be up to ∼10 Myr (for Δv > 800 km s−1), though the latter generally have higher luminosities. (6) Spatially offset AGNs can occur for vk≳ 0.5–0.7vesc (for ΔR > 1 kpc); these generally have low luminosities and lifetimes of ∼1–100 Myr. (7) Rapidly recoiling BHs may be up to approximately five times less massive than their stationary counterparts. These mass deficits lower the normalization of the MBH–σ* relation and contribute to both intrinsic and overall scatter. (8) Finally, the displacement of AGN feedback after a recoil event enhances central star formation rates in the merger remnant, thereby extending the starburst phase of the merger and creating a denser, more massive stellar cusp.

Highlights

  • It has recently been demonstrated that “central" supermassive black holes (SMBHs) may spend substantial time in motion and offset from the galactic center, owing to gravitationalwave (GW) recoil

  • (2) The inflow of cold gas during a gas-rich major merger may cause a rapid increase in central escape speed; in such cases recoil trajectories will depend on the timing of the BH merger relative to the change in vesc

  • The BH displacement is smaller in the gas-rich case, and BHs with vk 0.7 vesc (640 km s−1 in this merger model) are confined to the central few kpc of the galaxy

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Summary

Introduction

It has recently been demonstrated that “central" supermassive black holes (SMBHs) may spend substantial time in motion and offset from the galactic center, owing to gravitationalwave (GW) recoil. Numerical relativity simulations of binary black hole (BH) mergers have revealed that GW recoil may impart a kick to a merged BH of up to 4000 km s−1 [1]. The actual distribution of GW kick velocities is not known, estimates using optimistic assumptions indicate that more than a third of major galaxy mergers could result in kicks greater than 1000 km s−1 [1 – 4]. This fraction would be smaller if the progenitor BH spins are not large, or if the spins could be partially aligned prior to merger via gas processes or GR precession [5 – 7]. The sudden displacement of the central AGN from these merging systems could affect starburst properties or the gas and stellar distributions [13, 11]

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