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Peer-reviewedCC BY 4.0The Astrophysical Journal

The Role of the Interferometric Phase in Measuring Black Hole Photon Rings

  1. 1Black Hole Initiative at Harvard University
  2. 2Center for Astrophysics ∣ Harvard & Smithsonian
  3. 3Harvard University

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 multiring 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 multiring systems using a series of (1) simple geometric toy models, (2) synthetic BHEX and EHT observations of geometric models, and (3) semianalytic 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 μ as per unit dimensionless spin, yielding an expected phase signature on a 25 G λ baseline of ∼44 ∘ per unit spin.

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BibTeX
@article{gutierrezlara2026role,
  title = {{The Role of the Interferometric Phase in Measuring Black Hole Photon Rings}},
  author = {Sol Gutiérrez-Lara and Daniel C. M. Palumbo and Michael D. Johnson},
  journal = {The Astrophysical Journal},
  year = {2026},
  month = oct,
  doi = {10.3847/1538-4357/ae9bb2},
  url = {https://iopscience.iop.org/article/10.3847/1538-4357/ae9bb2},
  note = {CC BY 4.0},
}
RIS
TY  - JOUR
TI  - The Role of the Interferometric Phase in Measuring Black Hole Photon Rings
AU  - Sol Gutiérrez-Lara
AU  - Daniel C. M. Palumbo
AU  - Michael D. Johnson
PY  - 2026
DA  - 2026/10/09
JO  - The Astrophysical Journal
DO  - 10.3847/1538-4357/ae9bb2
UR  - https://iopscience.iop.org/article/10.3847/1538-4357/ae9bb2
AB  - 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 multiring 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 multiring systems using a series of (1) simple geometric toy models, (2) synthetic BHEX and EHT observations of geometric models, and (3) semianalytic 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 μ as per unit dimensionless spin, yielding an expected phase signature on a 25 G λ baseline of ∼44 ∘ per unit spin.
SN  - 0004-637X
SN  - 1538-4357
ER  -