papers

Publications (16)

hep-th2025

Geometrodynamics of a 2D Curved Surface due to a Constrained Quantum Particle via its Gravitational Dual: Analytical Model Calculations

Shanshan Rodriguez, Leo Rodriguez, Zhenzhong Xing +2

We provide a unique and novel extension of da Costa's calculation of a quantum mechanically constrained particle. This is achieved by analyzing the perturbative back reaction of th…

hep-th2020

Exploration of The Duality Between Generalized Geometry and Extraordinary Magnetoresistance

Sathwik Bharadwaj, L. R. Ram-Mohan, Leo Rodriguez +1

We outline the duality between the extraordinary magnetoresistance (EMR), observed in semiconductor-metal hybrids, and non-symmetric gravity coupled to a diffusive gauge fie…

hep-th2016

On Quantum Microstates in the Near Extremal, Near Horizon Kerr Geometry

Ananda Guneratne, Leo Rodriguez, Sujeev Wickramasekara +1

We study the thermodynamics of near horizon near extremal Kerr (NHNEK) geometry within the framework of correspondence. We start by shifting the horizon of near horiz…

hep-th2013

Near-Extremal Black Hole Thermodynamics from AdS2/CFT1 Correspondence in The Low Energy Limit of 4D Heterotic String Theory

Bradly K. Button, Leo Rodriguez, Sujeev Wickramasekara

We compute the asymptotic symmetry group of the four dimensional near-extremal Kerr-Sen black hole within an AdS2/CFT1 correspondence. We do this by performing a Robinson-Wilczek t…

hep-th2026

Superradiant Suppression of Non-minimally Coupled Scalar fields for a Rotating Charged dS Black Hole in Conformal Weyl Gravity

Owen Gartlan, Jacob March, Leo Rodriguez +2

In this study, we present an analytical investigation of the superradiant scattering of a massive charged conformally coupled scalar field in rotating charged black hol…

hep-th2013

Near-Extremal Kerr AdS2xS2 Solution and Black-Hole/Near-Horizion-CFT Duality

Ananda Guneratne, Leo Rodriguez, Sujeev Wickramasekara +1

We study the thermodynamics of the near horizon of near extremal Kerr geometry (near-NHEK) within an AdS2/CFT1 correspondence. We do this by shifting the horizon by a general finit…