A Steady-State Alignment Front in an Accretion Disk Subjected to Lense-Thirring Torques

TL;DR

This paper uses 3D MHD simulations to study how accretion disks align with a spinning black hole's axis under gravitomagnetic torques, revealing a steady-state transition influenced by turbulence and challenging traditional models.

Contribution

First simulation demonstrating a steady-state alignment front in MHD accretion disks under gravitomagnetic torques without phenomenological viscosity.

Findings

A stable alignment transition forms between inner and outer disk regions.

The equilibrium position depends on a balance between gravitomagnetic torque and warp-induced mixing.

The diffusion coefficient for angular momentum transport is estimated as ~(0.6--0.8)c_s^2/Omega.

Abstract

Using only physical mechanisms, i.e., 3D MHD with no phenomenological viscosity, we have simulated the dynamics of a moderately thin accretion disk subject to torques whose radial scaling mimics those produced by lowest-order post-Newtonian gravitomagnetism. In this simulation, we have shown how, in the presence of MHD turbulence, a time-steady transition can be achieved between an inner disk region aligned with the equatorial plane of the central mass's spin and an outer region orbiting in a different plane. The position of the equilibrium orientation transition is determined by a balance between gravitomagnetic torque and warp-induced inward mixing of misaligned angular momentum from the outer disk. If the mixing is interpreted in terms of diffusive transport, the implied diffusion coefficient is ~(0.6--0.8)c_s^2/Omega for sound speed c_s and orbital frequency Omega. This calibration permits estimation of the orientation transition's equilibrium location given the central mass, its spin parameter, and the disk's surface density and scaleheight profiles. However, the alignment front overshoots before settling into an equilibrium, signaling that a diffusive model does not fully represent the time-dependent properties of alignment fronts under these conditions. Because the precessional torque on the disk at the alignment front is always comparable to the rate at which misaligned angular momentum is brought inward to the front by warp-driven radial motions, no break forms between the inner and outer portions of the disk in our simulation. Our results also raise questions about the applicability to MHD warped disks of the traditional distinction between "bending wave" and "diffusive" regimes.