Truncated Disk Simulations

Hot coronae and truncated thin disks in simulations of accreting stellar-mass black holes

Executive Summary

This project studies how a cold, truncated thin disk and a hot X-ray-emitting corona can emerge naturally in simulations of accreting stellar-mass black holes. We used two-dimensional hydrodynamical simulations with radiative cooling to model accretion flows in X-ray binaries, varying the mass accretion rate across the range relevant for hard-state systems. The simulations show that as the accretion rate increases, the corona contracts and the inner edge of the thin disk moves closer to the black hole.

Black hole X-ray binaries cycle between hard and soft spectral states. In the hard state, observations are commonly interpreted with a geometry in which a hot corona coexists with a colder thin disk whose inner edge is truncated away from the event horizon. The physics that forms the corona, sets the truncation radius, and drives the hard-to-soft transition is still debated.

This work addresses that problem with numerical simulations designed to follow the collapse of a hot accretion flow when radiative cooling becomes dynamically important.

Temperature and density maps from five simulations with different accretion rates. The left side of each panel shows electron temperature, while the right side shows electron number density.

Scientific Motivation

In X-ray binaries, the hard state is associated with a hard power-law X-ray spectrum and is usually modeled with a hot corona or radiatively inefficient accretion flow inside a truncated thin disk. As the source brightens, the thin disk is expected to move inward and the system transitions toward the soft state.

The central questions are:

  • How does a hot corona form and survive around a stellar-mass black hole?
  • What controls the inner radius of the thin disk?
  • Does the disk truncation radius decrease as the accretion rate increases?

Numerical Experiment

We performed two-dimensional hydrodynamical simulations of accretion onto a $10 M_\odot$ black hole using the PLUTO code. This was a team effort including Ivan Almeida, Artur Vemado, Pedro Motta, and Javier Garcia. The simulations approximate Schwarzschild gravity with a pseudo-Newtonian potential and include radiative losses from bremsstrahlung, synchrotron emission, synchrotron self-Compton cooling, and optically thick cooling in dense regions.

The initial condition is a hot torus. After a burn-in phase, radiative cooling is enabled and the flow is allowed to evolve. We varied the accretion rate over $0.02 \leq \dot{M}/\dot{M}_{\rm Edd} \leq 0.35$, covering the regime where hard-state X-ray binaries are expected to transition between radiatively inefficient and thin-disk-dominated accretion.

Main Results

For $\dot{M}/\dot{M}_{\rm Edd} \geq 0.06$, the simulations form a cold thin disk embedded inside a hot corona. The disk is dense and geometrically thin, while the corona remains hot, with typical electron temperatures of $10^{9}$-$10^{10}$ K.

At the lowest simulated accretion rate, $\dot{M}/\dot{M}_{\rm Edd} = 0.02$, the thin disk disappears and the flow remains hot and geometrically thick. This constrains the critical accretion rate for the disk to disappear to roughly $0.02 < \dot{M}_{\rm crit}/\dot{M}_{\rm Edd} \lesssim 0.06$.

The corona height and thin disk inner radius both decrease as the accretion rate increases.

The trends are consistent with the standard picture of state transitions: increasing accretion rate leads to stronger cooling, a smaller corona, and a thin disk whose inner edge approaches the black hole.

Observational Relevance

The simulations provide a physical mechanism for the hard-state geometry inferred in X-ray binaries. They predict that the disk inner radius should anticorrelate with accretion rate and luminosity, matching the qualitative behavior expected from observations of systems such as GX 339-4.

The work also suggests that a compact corona can persist even at luminosities typical of softer states, potentially contributing to the hard X-ray tail observed in some systems.