The Role of Interferometric Phase in Measuring Black Hole Photon Rings

TL;DR

This paper investigates how interferometric phase and amplitude responses can be used to measure black hole parameters, especially spin, by analyzing multi-ring images from VLBI observations like EHT and BHEX.

Contribution

It introduces a detailed analysis of interferometric responses to multi-ring black hole images, highlighting phase sensitivity to spin and amplitude to shape, aiding parameter estimation.

Findings

Interferometric amplitude is more sensitive to photon ring shape.

Interferometric phase is more sensitive to ring displacement and black hole spin.

Expected phase signature is approximately 44° per unit spin for M87* models.

Abstract

The Event Horizon Telescope (EHT) captured the first images of a black hole using Very Long Baseline Interferometry (VLBI). In the near future, extensions of the EHT such as the Black Hole Explorer (BHEX) will allow access to finer-scale features, such as a black hole's ''photon ring.'' In the Kerr spacetime, this image structure arises from strong gravitational lensing near the black hole that results in a series of increasingly demagnified images of each emitting region that exponentially converge to a limiting critical curve. Exotic black hole alternatives, such as wormholes, can introduce additional photon rings. Hence, precisely characterizing multi-ring images is a promising pathway for measuring black hole parameters, such as spin, as well as exploring non-Kerr spacetimes. Here, we examine the interferometric response of multi-ring systems using a series of 1) simple geometric toy models, 2) synthetic BHEX and EHT observations of geometric models, and 3) semi-analytic accretion models with ray-tracing in the Kerr spacetime. We find that interferometric amplitude is more sensitive to the shape of the photon ring, while interferometric phase is more sensitive to its displacement, which is most sensitive to black hole spin. We find that for models similar to Messier 87* (M87*), the relative displacement of the first strongly lensed image from the weakly lensed direct image is approximately $1\,\mu {\rm as}$ per unit dimensionless spin, yielding an expected phase signature on a 25 G$\lambda$ baseline of $\sim44^\circ$ per unit spin.