Are S1× S2 wormholes generic with large sources?Euclidean path integrals can be used to prepare states of a Lorentzian QFT. So long as any sources are turned off on the t=0 surface, the resulting Lorentzian states all belong to the same Hilbert…Xiaoyi Liu, Donald Marolf, Jorge E. Santos·Oct 1, 2025SaveLearn
Complex Kerr-AdS Black HolesWe revisit thermodynamics of five-dimensional AdS spacetime at finite temperature and rotation using the Euclidean path integral. It is generally believed that at low temperatures and finite…Kaustubh Singhi·Oct 1, 2025SaveLearn
Algebra of operators for Q-Schur polynomialsWe consider algebras acting on Schur and Q-Schur polynomials, corresponding to Kadomtsev-Petviashvili (KP) and BKP hierarchies. We present them in the spirit of affine Yangians, paying special…Nikita Tselousov·Oct 1, 2025SaveLearn
New variants of N=3,4 superconformal mechanicsWe construct superconformal mechanics with N=3 and N=4 supersymmetries that were inspired by analogies with the supersymmetric Schwarzian mechanics. The Schwarzian, being another system with…Nikolay Kozyrev, Sergey Krivonos·Oct 1, 2025SaveLearn
Nonresonant renormalization scheme for twist-2 operators in N=1 SUSY SU(N) Yang-Mills theoryThe short-distance asymptotics of the generating functional for n-point correlators of twist-2 operators in N=1 supersymmetric (SUSY) SU(N) Yang-Mills (SYM) theory were recently…Francesco Scardino·Oct 1, 2025SaveLearn
Spinning Boundary Correlators from (A)dS4 TwistorsWe develop a twistor-space framework to compute boundary correlators via a boundary limit of nested Penrose transforms in (A)dS4. Starting from correlators of (anti-)self-dual bulk fields, the…Mariana Carrillo González, Théo Keseman·Sep 30, 2025SaveLearn
Consequences of symmetry-breaking on conformal defect dataConformal defects spontaneously break part of the symmetry algebra of a bulk CFT. We show that the broken Ward identities imply very general sum rules on the defect CFT data as well as on the DOE…Bastien Girault, Miguel F. Paulos, Philine van Vliet·Sep 30, 2025SaveLearn
Long-range minimal modelsWe study a class of nonlocal conformal field theories in two dimensions which are obtained as deformations of the Virasoro minimal models. The construction proceeds by coupling a relevant primary…Connor Behan, Dario Benedetti, Fanny Eustachon et al.·Sep 30, 2025SaveLearn
A review on the equation of state of color superconductivity via holographyIn this project, we will study a bottom-up holographic model for the color superconductivity (CSC) phase in the Einstein-Gauss-Bonnet (EGB) gravity. We study the color superconductivity phase in the…Nguyen Hoang Vu·Sep 30, 2025SaveLearn
Study of chaos and scrambling in hairy AdS SolitonIn this work, we perform a comprehensive study of the classical and quantum chaos in a candidate five-dimensional hairy AdS soliton. It is a horizonless geometry holographically dual to a confining…Adrita Chakraborty, Balbeer Singh·Sep 30, 2025SaveLearn
Hyperfunctions in A-model LocalizationWe apply localization techniques to topologically A-twisted N=(2,2) supersymmetric theories of vector and chiral multiplets on S2 and derive a novel exact formula for abelian…Emil Hakan Leeb-Lundberg·Sep 30, 2025SaveLearn
Limits of Symmetry in Schwarzschild: CKVs and BRST Triviality in the Kerr-Schild Double CopyWe complete our investigation into the residual symmetries of the Kerr-Schild double copy for the Schwarzschild solution. In the first paper in this series, we showed that the infinite-dimensional…Brandon Holton·Sep 30, 2025SaveLearn
Local vertices, quadratic propagators and double-copy structure of one-loop integrands from forward limitsBy worldsheet approach, n-point one-loop integrand can be expressed as a combination of (n+2)-point tree-level bi-adjoint scalar (BS) amplitudes under forward limit. The integrands constructed by…Chongsi Xie, Yi-Jian Du·Sep 30, 2025SaveLearn
Lectures on Open Effective Field TheoriesEffective field theories offer a powerful method to unify diverse models under a small set of control parameters, allowing systematic expansions around well-established theories. These techniques,…Thomas Colas·Sep 30, 2025SaveLearn
Quantum fermion emission from excited kinksThe amplitude of an excited shape mode in a kink is expected to decay with a well-known power law via scalar radiation emission due to the nonlinear self-coupling of the scalar field. In this work we…Sergio Alameda-Calvo, Jose J. Blanco-Pillado, Alberto García Martín-Caro·Sep 30, 2025SaveLearn
On sufficient conditions for holographic scatteringHolography implies scattering in the bulk can be mediated by entanglement on the boundary. The connected wedge theorem (CWT) of May, Penington, and Sorce is a concrete example where bulk scattering…Caroline Lima, Sabrina Pasterski, Chris Waddell·Sep 30, 2025SaveLearn
Abelian 3D TQFT gravity, ensemble holography and stabilizer statesWe construct a model of 3D quantum gravity based on abelian topological quantum field theory (TQFT), by defining the gravitational path-integral as a sum over all 3D topologies with genus-g…Nikolaos Angelinos·Sep 30, 2025SaveLearn
On correlation numbers V0,4 and V1,1 in Virasoro Minimal String TheoryWe study correlation numbers in Virasoro minimal string Collier:2023cyw. Using analytic properties of correlation functions in spacelike and timelike Liouville theories, we verify exact…Dmitry Khromov, Alexey Litvinov·Sep 30, 2025SaveLearn
Casimir effect between semitransparent mirrors in a Lorentz-violating backgroundWe investigate the Casimir effect for a massless scalar field confined between two parallel semitransparent mirrors in a vacuum modified by spontaneous Lorentz symmetry breaking. Using Green's…Román Linares, C. A. Escobar, A. Martín-Ruiz et al.·Sep 30, 2025SaveLearn
Horowitz-Polchinski Solutions at Large kIn arXiv:2509.02905 [hep-th], we introduced an approximation that allows one to study Horowitz-Polchinski backgrounds beyond the weak coupling regime. In this paper we describe the resulting…Jinwei Chu, David Kutasov·Sep 29, 2025SaveLearn
Renormalization Group Running of the Parity Operator in Lorentz-Violating Quantum Field TheoryIn conventional relativistic quantum field theory, the discrete operators C, P, and T are matrix operators with no renormalization scale dependence. However, in a…Brett Altschul·Sep 29, 2025SaveLearn
An analytic approach for holographic entanglement entropy at (quantum) criticalityWe consider holographic entanglement entropy in AdS black hole backgrounds by using the limit of large number of dimensions. By dividing the geometry to two patches (with one patch covering the…Parul Jain, Matti Järvinen·Sep 29, 2025SaveLearn
Renormalization of Chern-Simons Wilson Loops via Flux Quantization in CohomotopyIn the practice of physics model building, the process of renormalization, resummation, and anomaly cancellation is to incrementally repair initially ill-defined Lagrangian quantum field theories.…Hisham Sati, Urs Schreiber·Sep 29, 2025SaveLearn
Holography vs. Scale SeparationIn this work, we point out a contradiction between holography and scale-separated AdS (i.e. parametrically large mass gap) in string theory, making the standard assumption that the holographic CFT…Alek Bedroya, Paul J. Steinhardt·Sep 29, 2025SaveLearn
Aspects of holographic entanglement using physics-informed-neural-networksWe implement physics-informed-neural-networks (PINNs) to compute holographic entanglement entropy and entanglement wedge cross section. This technique allows us to compute these quantities for…Anirudh Deb, Yaman Sanghavi·Sep 29, 2025SaveLearn