Abstract

We investigate the effect of black hole spin on warped or misaligned accretion discs - in particular i) whether or not the inner disc edge aligns with the black hole spin and ii) whether the disc can maintain a smooth transition between an aligned inner disc and a misaligned outer disc, known as the Bardeen-Petterson effect. We employ high resolution 3D smoothed particle hydrodynamics simulations of $\alpha$-discs subject to Lense-Thirring precession, focussing on the bending wave regime where the disc viscosity is smaller than the aspect ratio $\alpha \lesssim H/R$. We first address the controversy in the literature regarding possible steady-state oscillations of the tilt close to the black hole. We successfully recover such oscillations in 3D at both small and moderate inclinations ($\lesssim 15^{\circ}$), provided both Lense-Thirring and Einstein precession are present, sufficient resolution is employed, and provided the disc is not so thick so as to simply accrete misaligned. Second, we find that discs inclined by more than a few degrees in general steepen and break rather than maintain a smooth transition, again in contrast to previous findings, but only once the disc scale height is adequately resolved. Finally, we find that when the disc plane is misaligned to the black hole spin by a large angle, the disc 'tears' into discrete rings which precess effectively independently and cause rapid accretion, consistent with previous findings in the diffusive regime ($\alpha \gtrsim H/R$). Thus misalignment between the disc and the spin axis of the black hole provides a robust mechanism for growing black holes quickly, regardless of whether the disc is thick or thin.

Highlights

  • Bardeen & Petterson (1975) first computed the evolution of a warped accretion disc subjected to Lense-Thirring precession (Lense & Thirring 1918) caused by frame-dragging from the spin of a central black hole

  • In this work we have re-examined the Bardeen-Petterson effect in 3D using hydrodynamical simulations of accretion discs subject to Lense-Thirring precession, in the regime where warps propagate in a wavelike manner (α H/R)

  • Our detailed conclusions are as follows: (i) The Bardeen-Petterson picture of an aligned inner disc smoothly connected to a misaligned outer disc occurs only at low inclinations and only when Einstein precession is not accounted for

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Summary

Introduction

Bardeen & Petterson (1975) first computed the evolution of a warped accretion disc subjected to Lense-Thirring precession (Lense & Thirring 1918) caused by frame-dragging from the spin of a central black hole. The first studies performed in the bending wave regime (Ivanov & Illarionov 1997; Lubow, Ogilvie & Pringle 2002, hereafter LOP02) suggested a conflict with the Bardeen-Petterson picture — finding that the black hole spin could drive the disc tilt into a steady state that is oscillatory and non-zero. This implies that the inner edge of the disc may be misaligned with respect to the black hole spin. Unlike the diffusive regime for which there exists a full non-linear theory describing warps of arbitrary amplitude and α (Ogilvie 1999, 2000) only linear theory exists for the bending wave regime (Papaloizou & Lin 1995; Lubow & Ogilvie 2000; LOP02; though see Ogilvie 2006); these studies apply only to small amplitude warps and could not account for non-linear effects

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