4.7 Article

Interactions between multiple supermassive black holes in galactic nuclei: a solution to the final parsec problem

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 473, Issue 3, Pages 3410-3433

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stx2524

Keywords

gravitational waves; Galaxy: evolution; Galaxy: kinematics and dynamics Galaxy: nucleus; quasars: general

Funding

  1. Simons Fellowship in Theoretical Physics
  2. NASA [NNX15AB19G]
  3. NASA through Einstein Postdoctoral Fellowship [PF5-160145]
  4. Empire State Development grant NYS [28451]

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Using few-body simulations, we investigate the evolution of supermassive black holes (SMBHs) in galaxies (M* = 10(10)-10(12)M(circle dot) at z = 0) at 0 < z < 4. Following galaxy merger trees from the Millennium simulation, we model BH mergers with two extreme binary decay scenarios for the ` hard binary' stage: a full or an empty loss cone. These two models should bracket the true evolution, and allow us to separately explore the role of dynamical friction and that of multibody BH interactions on BH mergers. Using the computed merger rates, we infer the stochastic gravitational wave background (GWB). Our dynamical approach is a first attempt to study the dynamical evolution of multiple SMBHs in the host galaxies undergoing mergers with various mass ratios (10(-4) < q(*) < 1). Our main result demonstrates that SMBH binaries are able to merge in both scenarios. In the empty loss cone case, we find that BHs merge via multibody interactions, avoiding the ` final parsec' problem, and entering the pulsar timing arrays band with substantial orbital eccentricity. Our full loss cone treatment, albeit more approximate, suggests that the eccentricity becomes even higher when GWs become dominant, leading to rapid coalescences (binary lifetime <= 1Gyr). Despite the lower merger rates in the empty loss cone case, due to their higher mass ratios and lower redshifts, the GWB in the full/empty loss cone models are comparable (0.70 x 10(-15) and 0.53 x 10(-15) at a frequency of 1 yr(-1), respectively). Finally, we compute the effects of high eccentricities on the GWB spectrum.

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