The Nature of Black Hole Shadows

A distinct visual signature occurs in black holes that are surrounded by optically thin and geometrically thick emission regions. This signature is a sharp-edged dip in brightness that is coincident with the black hole's shadow, which is the projection of the black hole's unstable-photon region on the observer's sky. We highlight two key mechanisms that are responsible for producing the sharp-edged dip: (i) the reduction of intensity observed in rays that intersect the unstable-photon region, and thus the perfectly absorbing event horizon, versus rays that do not (blocking); and (ii) the increase of intensity observed in rays that travel along extended, horizon-circling paths near the boundary of the unstable-photon region (path-lengthening). We demonstrate that the black hole shadow is a distinct phenomenon from the photon ring, and that models exist in which the former may be observed but not the latter. Additionally, we show that the black hole shadow and its associated visual signature differ from the more model-dependent brightness depressions associated with thin-disk models because the blocking and path-lengthening effects are quite general for geometrically thick and optically thin emission regions. Consequentially, the black hole shadow is a robust and fairly model-independent observable for accreting black holes that are in the deep sub-Eddington regime, such as low-luminosity active galactic nuclei.

Automated summary

Distinct visual signature occurs in black holes surrounded by optically thin and geometrically thick emission regions, resulting in a sharp-edged dip in brightness coincident with the black hole's shadow. This signature is due to the reduction of intensity observed in rays that intersect the unstable-photon region and the increase of intensity in rays that travel along extended paths near the boundary of the unstable-photon region. The black hole shadow is distinct from the photon ring and is a robust and fairly model-independent observable for accreting black holes in the deep sub-Eddington regime.