Magnetic flux plays an important role during a BHXRB outburst in radiative 2T GRMHD simulations

TL;DR

This study uses advanced radiative 2T GRMHD simulations to explore how magnetic flux influences state transitions in black hole X-ray binaries across a wide range of accretion rates.

Contribution

First radiative 2T GRMHD simulations demonstrating magnetic flux's critical role in BHXRB state transitions over a broad accretion rate spectrum.

Findings

Magnetically arrested disks maintain hot plasma at higher accretion rates.

Unsaturated magnetic flux leads to disk cooling and collapse.

Magnetic flux saturation correlates with spectral state signatures.

Abstract

Black hole (BH) X-ray binaries cycle through different spectral states of accretion over the course of months to years. Although fluctuations in the BH mass accretion rate are generally recognized as the most important component of state transitions, it is becoming increasingly evident that magnetic fields play a similarly important role. In this article, we present the first radiative two-temperature (2T) general relativistic magnetohydrodynamics (GRMHD) simulations in which an accretion disk transitions from a quiescent state at an accretion rate of $\dot{M} \sim 10^{-10} \dot{M}_{\rm Edd}$ to a hard-intermediate state at an accretion rate of $\dot{M} \sim 10^{-2} \dot{M}_{\rm Edd}$. This huge parameter space in mass accretion rate is bridged by artificially rescaling the gas density scale of the simulations. We present two jetted BH models with varying degrees of magnetic flux saturation. We demonstrate that in `Standard and Normal Evolution' models, which are unsaturated with magnetic flux, the hot torus collapses into a thin and cold accretion disk when $\dot{M} \gtrsim 5\times 10^{-3} \dot{M}_{\rm Edd}$. On the other hand, in `Magnetically Arrested Disk' models, which are fully saturated with vertical magnetic flux, the plasma remains mostly hot with substructures that condense into cold clumps of gas when $\dot{M} \gtrsim 1 \times 10^{-2} \dot{M}_{\rm Edd}$. This suggests that the spectral signatures observed during state transitions are closely tied to the level of magnetic flux saturation.