Research dossierORCID 0000-0002-1559-6965

Alexandru Lupsasca

Vanderbilt University · 4 affiliations on record

What this is

Valency read your published work and assembled this dossier automatically. Every figure links to the real paper behind it.

67 works, 1,822 citations, h-index 21, and a proposed space mission built around the ring you predicted.

Your work takes the Kerr metric apart and hands the pieces back as things an instrument can measure. The explicit null geodesics, the shape of the photon ring, the polarization pattern that reveals which way electromagnetic energy is flowing at the horizon: each one reduces a statement about strong-field general relativity to a number someone could read off an interferometric baseline. That program now has hardware attached, with the Black Hole Explorer designed around detecting and measuring the ring. Here is how it reads from outside.

67works in corpus
2014–2026active
Generated August 1, 2026
02
Your research program

Read as one thread, not a list

Two papers sit at 213 citations each and they do opposite halves of one job. 'Lensing by Kerr Black Holes' works out the analytic theory, the three parameters that govern how each successive image of a source is demagnified, rotated and delayed. 'The Shape of the Black Hole Photon Ring' turns that theory into an experiment by showing the ring's shape barely depends on the emitting plasma. Underneath both sits 'The Null Geodesics of the Kerr Exterior' at 129 citations, the explicit elliptic-function solution that other groups now reuse as their reference case. Polarimetry is the fourth line, starting from the self-similar polarization pattern of the photon ring in 2020 and running into your current work on what horizon polarization says about where a black hole's energy is going.

Where your output lives
  • General Relativity and Quantum Cosmologygr-qc37%
  • High Energy Astrophysical Phenomenaastro-ph.HE28%
  • High Energy Physics - Theoryhep-th26%
  • Instrumentation and Methods for Astrophysicsastro-ph.IM2%
  • Astrophysics of Galaxiesastro-ph.GA2%
Career, by the numbers
67works
1,822citations
21h-index

Your 67 works sit inside a narrow band of gravitational physics, and the citations concentrate harder still. The Kerr lensing and photon ring papers from 2019 and 2020 carry most of the total. The earlier force-free magnetosphere and pulsar work runs between 29 and 58 citations on its own track.

03
Where your work travels

Where the photon ring goes after you publish it

The heaviest citers are people asking whether the object is Kerr at all. Vagnozzi and colleagues run your ring-size logic across more than fifty alternative spacetimes at 645 citations, and the EHT collaboration's own metric test on Sgr A* sits just behind at 613. Below those, a long tail of modified-gravity shadow papers treats the analytic Kerr geodesics as the reference case they measure deviations against. The 2026 citers keep that shape: a non-singular black hole review, a study of the vortical geodesics that thread both Kerr horizons, image calculations for non-minimally coupled black holes, and strong-deflection formulas extended from photons to massive particles. The polarimetry line landed somewhere more observational, with the EHT's ring-asymmetry analysis of M87* using spin constraints to separate competing jet-launching mechanisms.

Highest-impact citations
  1. Horizon-scale tests of gravity theories and fundamental physics from the Event Horizon Telescope image of Sagittarius A*

    2023Class. Quant. Grav.645 citesSunny Vagnozzi, Rittick Roy, et al.

    Constrains more than fifty alternatives to the Kerr solution, from regular black holes to wormholes and naked singularities, by tying the bright emission ring of Sgr A* to the underlying shadow size.

    indexed
  2. First Sagittarius A* Event Horizon Telescope Results. VI: Testing the Black Hole Metric

    2023613 citesThe Event Horizon Telescope Collaboration

    The collaboration's own metric test on Sgr A*, the observational program your ring-shape prediction was written to sharpen.

    indexed
  3. Superradiance evolution of black hole shadows revisited

    2022129 citesRittick Roy, Sunny Vagnozzi, et al.

    indexed
Most recent citations
  1. Ring Asymmetry and Spin in M87*

    2026ApJ0 citesVadim Bernshteyn, Nicholas S. Conroy, et al.

    Compares three epochs of EHT brightness-asymmetry data against GRMHD models and marginally disfavors low spin for M87*, consistent with the Blandford-Znajek picture your polarimetry work built an observable test for.

    indexed
  2. Looking through the Kerr disk

    2026Phys. Rev. D0 citesMaciej Maliborski, Tobias C. Sutter

    Solves for the vortical null geodesics that cross both Kerr horizons into the negative-radius region, correcting and extending earlier formulae, and builds simulated views for an observer on the far side.

    indexed
  3. Strong deflection of massive particles in spherically symmetric spacetimes

    2026Phys. Rev. D10 citesFabiano Feleppa, Valerio Bozza, et al.

    Extends strong-deflection-limit analysis from light to massive particles for any static spherically symmetric spacetime, carrying the near-critical-orbit machinery beyond null geodesics.

    indexed
  4. Towards a Non-singular Paradigm of Black Hole Physics

    202540 citesRaúl Carballo-Rubio, Francesco Di Filippo, et al.

    indexed
Citing fields beyond your own
37%General Relativity and Quantum Cosmologygr-qc
2%Instrumentation and Methods for Astrophysicsastro-ph.IM

When a paper cites you but we do not hold its full text, we flag it, so you can tell first-hand sources from second-hand mentions.

04
Your collaboration network

Two centers of gravity

Andrew Strominger is the close collaborator pulling hardest in his own direction. You share 12 papers, but his output is 200 hep-th papers against 62 in gr-qc, and his densest ties run to Kapec, Wei Song and Raclariu rather than to anyone with a telescope. Samuel Gralla is the mirror image: 14 shared papers and nearly the same category ordering as yours, with his own network running through Wald, Zimmerman and Jacobson in classical relativity. The third corner is the imaging group, Johnson, Chael, Wong, Quataert and Cárdenas-Avendaño, which is where your recent output has concentrated and where the network opens out the furthest, since Michael Johnson's own top collaborators are the EHT core. Berens and Gravely sit on a fourth thread of their own, the Kerr metric-reconstruction papers.

Alexandru LupsascaSamuel E. Gralla · 14Andrew Strominger · 12Michael D. Johnson · 7Shahar Hadar · 7Eliot Quataert · 6George N. Wong · 6Andrew Chael · 6
Clusters
  • Black hole imaging and photon ring instrumentation
  • Analytic Kerr lensing and geodesics
  • Near-horizon symmetry and high energy theory
  • Kerr perturbation theory
Most frequent collaborators
  1. Samuel E. Grallagr-qc14papers
  2. Andrew Stromingerhep-th12papers
  3. Michael D. Johnsonastro-ph.HE7papers
  4. Shahar Hadargr-qc7papers
  5. Eliot Quataert6papers
  6. George N. Wong6papers
  7. Andrew Chael6papers
  8. Daniel Kapec5papers
  9. Alejandro Cárdenas-Avendaño5papers
  10. Trevor Gravely5papers
  11. Roman Berens5papers
  12. Peter Galison5papers
05
People you should meet

Close to your work, not yet in your network

Four researchers keep turning up next to your current directions, none at an institution you have held and none with a paper co-authored with you. Ben Achour is the closest fit, working both the beyond-Kerr photon ring and the analytic magnetosphere at once from the Lyon quantum gravity side. Cano comes at the near-extremal spectrum through effective field theory. Figueiredo brings kinetic plasma simulations to the tilted-field configurations your analytic work sets aside, and Tamar is building out the observational side of ring polarimetry.

Jibril Ben Achour

Established
integrable parametrizations of the photon ring beyond general relativityanalytic jet launching from the Kerr magnetosphere

He is working both of your lines at once from a completely separate tradition: an integrable parametrization that keeps photon ring calculations tractable outside Kerr, and an analytic electrogeodesic treatment of jet launching from the magnetosphere. That second paper is the theoretical counterpart of the energy-extraction observable you built.

He shares no institution with you, current or historical, and no co-authored papers; his 52 collaborators are the loop quantum gravity and Paris relativity communities.

Pablo A. Cano

Established
quasinormal mode spectra of rapidly rotating black holes beyond general relativity

He works the near-extremal corner of the quasinormal mode spectrum, where small departures from general relativity get amplified. That is the same regime your photon ring encodes through the eikonal spectrum, approached with effective-field-theory tools rather than lensing.

He shares no institution with you (KU Leuven, Madrid and Barcelona) and no co-authored papers.

Enzo Figueiredo

Rising
kinetic plasma simulations of black hole jet power and particle acceleration

He asks what happens to jet power and particle acceleration when the magnetic field is tilted relative to the spin axis, which is exactly the configuration your force-free and polarimetry results assume away with axisymmetry.

He shares no institution with you (CNRS and Grenoble) and no co-authored papers; his eight collaborators are the Grenoble plasma group.

Aditya Tamar

Rising
photon ring polarimetry for next-generation black hole imaging

He is pushing photon ring polarimetry toward what next-generation arrays could actually resolve on M87*, the observational half of the universal polarization pattern you derived.

He shares no institution with you (he is at NIT Karnataka in India) and no co-authored papers.

06
Frontiers in your fields, last 90 days

What just landed next to your work

The last 90 days have been about turning the photon ring from a prediction into a measurement plan, and about what stands in the way. Hioki and colleagues show a fragment of the critical curve is enough to fix spin and inclination. Wong and collaborators review horizon-scale polarimetry and conclude the current data pins down field geometry much better than spin. On the hardware side, the constraints are getting specific: which space clocks hold coherence at 345 GHz, which supermassive black holes come into range on an Earth-Moon baseline, where BHEX sits among the other space interferometry concepts. The theory side has stayed busy with exact WKB treatments of the extremal quasinormal spectrum and hidden conformal symmetry in modified-gravity Kerr.

07
Where your next paper should go

Five directions, grounded in your work

All five sit where your analytic work meets something that could be measured. The lunar target list and the joint spin likelihood are close to ready, needing a forecast run and a merged inference rather than new theory. Couch-Torrence symmetry and second-order reconstruction are questions your own recent papers opened and then set down. The electrogeodesic test points at Jibril Ben Achour, already on your fresh-collaborators list, whose analytic magnetosphere is the missing input.

Every source below is real and linked. The directions, and the reading of them, are generated. Check anything you would lean on against your own knowledge of the field.

  1. 01

    Photon ring shape forecasts for the lunar-baseline target list

    Your shape prediction and the width observable were developed for BHEX pointed at M87* and Sgr A*. A lunar-baseline study has now named six supermassive black holes whose shadows become detectable at roughly 0.7 microarcseconds, and a dozen more where the n=1 ring comes into range, but it works from a geometric ring model rather than the Kerr shape function.

    The gap

    A search for photon ring shape measurement on lunar or Earth-Moon baselines beyond M87* and Sgr A* returns the lunar shadow-detection study, orbital-configuration studies for spaceborne interferometers, and your own BHEX papers. Nothing applies the shape or width machinery to that target list.

    First step

    Run the six lunar-detectable candidates from Zhao et al. through AART and forecast whether the n=1 ring diameter and its width are measurable at the predicted baseline coverage.

    Bridgesgr-qcastro-ph.IMastro-ph.GA
  2. 02

    One likelihood for spin from ring width and horizon polarization together

    Black Hole Polarimetry III gives a horizon polarization pattern fixed entirely by spin and inclination, independent of the field geometry. The interferometric width work constrains the same two parameters to about 20 percent from ring size and brightness. They are separate papers with separate likelihoods, aimed at the same two numbers, and the systematics that limit each one are different.

    The gap

    A search for joint spin inference combining photon ring width and horizon polarization returns the ingredients on their own: your width paper, the geometric ring approach of Keeble and colleagues, and the Wong review of polarimetric spin signatures. No paper combines them into a single inference.

    First step

    Write down a joint likelihood over spin and inclination from the photon ring width observable and the horizon polarization pattern, and test it on synthetic BHEX data generated from GRMHD snapshots.

    Bridgesastro-ph.HEgr-qc
  3. 03

    Does Couch-Torrence inversion leave a mark on the photon ring?

    You just reinterpreted Couch-Torrence inversions through their action on photon spheres and found a relation between the fixed point of the inversion and the superradiant scattering coefficient. Separately, your holographic toy model ties photon ring structure to the eikonal quasinormal spectrum. The symmetry acts on the same object the ring measures, and nobody has asked whether that shows up in an observable.

    The gap

    A search for Couch-Torrence inversion symmetry connected to photon ring or quasinormal mode observables returns nothing in gravitational physics at all. The results are quantum optics papers about photon interference and parity-time symmetry.

    First step

    Work out how a Couch-Torrence inversion acts on the interferometric ring observables for extremal Kerr-Newman, and check whether the superradiance relation you found survives as a constraint between the ring shape and the ringdown spectrum.

    Bridgesgr-qchep-thastro-ph.HE
  4. 04

    Second-order metric reconstruction for a binary orbiting a supermassive black hole

    You wrote the explicit radiation-gauge metric perturbations precisely because second-order perturbation theory needs them, and you noted the formulas had never actually been worked out. Your resonance paper then found a rich structure in the energy fluxes a stellar-mass binary drives in a supermassive black hole, computed at linear order, including an offset between the flux maximum and the quasinormal frequency that grows with separation.

    The gap

    A search for second-order radiation-gauge reconstruction applied to resonant excitation by a binary near a supermassive black hole returns linear-order reconstruction work for eccentric precessing small-mass-ratio binaries, ringdown surrogates, and post-Newtonian resonance studies. Nothing carries explicit reconstruction into the second-order source for that problem.

    First step

    Feed the explicit radiation-gauge modes from Gravitational Waves on Kerr I into a second-order source term for the resonant flux calculation, and check whether the offset from the mode frequency survives the nonlinear correction.

    Bridgesgr-qcastro-ph.HE
  5. 05

    Run an electrogeodesic jet-launching model through your energy-extraction observable

    Your polarimetric phase turns the sign of the near-horizon Poynting flux into something an interferometer can read, and the 2017 EHT data already leans toward outflow. Ben Achour, El Mellah and Gourgoulhon have since built an analytic electrogeodesic model of jet launching from the Kerr magnetosphere, with no observable yet attached to it.

    The gap

    A search for a force-free or electrogeodesic jet-launching model tested against a horizon polarimetric energy-extraction observable returns the electrogeodesic paper, a scattered set of magnetic-reconnection energy-extraction calculations, and solar and magnetospheric plasma work. No paper connects the two.

    First step

    Ray trace polarized synchrotron emission through the electrogeodesic magnetosphere solution, compute the polarimetric phase, and check it against the universal horizon pattern. Jibril Ben Achour at ENS Lyon is the natural first contact.

    Bridgesastro-ph.HEgr-qc
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