Illustration for large D gravity
Large D Gravity

The large number-of-dimensions limit of General Relativity

When the number of spacetime dimensions D is taken to be very large, Einstein's equations simplify dramatically: gravity becomes localized near horizons and behaves like an effective theory of a membrane embedded in flat space. This "large D" expansion turns notoriously hard problems — black hole instabilities, collisions, and the fate of cosmic censorship — into tractable effective equations. My work has used this limit to study black string instabilities, black hole fusion and fission, and violations of cosmic censorship in higher dimensions.

Illustration for numerical relativity
Numerical Relativity

Simulating strong-field gravity

Many of the most interesting regimes of gravity — black hole mergers, exotic compact object collisions, the nonlinear development of instabilities — have no closed-form solution and have to be evolved numerically. I work on numerical relativity simulations of these systems, including head-on mergers of Proca stars, charged black hole binaries, and the nonlinear development of strong cosmic censorship violation, often building surrogate waveform models that make these simulations usable for gravitational-wave parameter estimation.

Illustration for AdS/CFT holography
AdS/CFT Holography

Black holes as holographic duals

The AdS/CFT correspondence relates gravity in Anti-de Sitter space to a conformal field theory living on its boundary. I have used this duality, together with the large D limit, to study the holographic duals of evaporating black holes, plasma polarization and Love numbers of black branes, and high-energy holographic collisions — connecting gravitational dynamics to the language of strongly coupled quantum field theory.

Illustration for machine learning in gravity
Machine Learning for Strong Gravity

Physics-informed neural networks as differential equation solvers

A more recent thread of my research uses physics-informed neural networks (PINNs) to solve the differential equations that govern black hole perturbation theory and modified gravity — including the Teukolsky and Regge–Wheeler–Zerilli equations, and quasinormal mode problems beyond General Relativity. These methods offer a fast, flexible alternative to traditional numerical solvers and are increasingly useful for modeling protoneutron star oscillations and other time-dependent strong-gravity systems.

Illustration for gravitational wave astronomy
Gravitational-Wave Astrophysics

From simulations to observable signals

Ultimately, much of this work feeds into gravitational-wave astrophysics: building waveform models for exotic compact objects and hyperbolic encounters, understanding parameter-estimation biases when comparing models to data, and connecting strong-field simulations to what current and future detectors can actually observe.