Phase diagram of the massless Gross-Neveu model with two componentsRecently, Benini, Mamroud, Reis and Serone have presented exact results for the Gross-Neveu model at finite density, both at finite N and in the large N limit. Generalizing previous studies, they…Michael Thies·Jun 29, 2026SaveLearn
Higher-loop wormhole length in sine-dilaton gravity from DSSYK Krylov complexityThe quantum wormhole length in sine-dilaton gravity has been shown to equal the Krylov spread complexity in the double-scaled SYK model. In the infinite temperature limit, we compute the five-loop…Eleonora Alfinito, Matteo Beccaria·Jun 29, 2026SaveLearn
Double-Current Deformations of Two-Dimensional QFTs with AnomaliesWe construct the double-current deformations of two-dimensional quantum field theories whose partition functions have background gauge-field anomalies. Extending the path integral construction of…Zhengyuan Du·Jun 29, 2026SaveLearn
Constraints on four-party entanglement in holographyWe show that in pure time-reflection-symmetric holographic states several known four-party entanglement signals vanish unless the triple information I3 is non-zero. In this sense, our results show…Vijay Balasubramanian, William K. L. Chan, Monica Jinwoo Kang et al.·Jun 29, 2026SaveLearn
Examples of Invertible Gauging via Orbifold Data, Zesting, and EquivariantisationWe study the gauging of invertible symmetries, particularly in 3 dimensions, using equivariantisation, G-crossed braided zesting, and the generalised orbifold construction. We discuss how these…Benjamin Haake·Jun 29, 2026SaveLearn
Causal self-dual nonlinear electrodynamics from the Born-Infeld theoryRecently we have proposed a new auxiliary-field formulation for self-dual nonlinear electrodynamics (NLED) which makes use of two building blocks: (i) a seed self-dual theory L(Fμν;g), where…Sergei M. Kuzenko, Jonah Ruhl·Jun 29, 2026SaveLearn
Curvature-Assisted Dynamical Compactification in a Pre-Inflationary Higher-Dimensional UniverseWe investigate a pre-inflationary dynamical compactification scenario in which a higher-dimensional expanding universe evolves into an effectively four-dimensional one through curvature-assisted…Yusuke Yamada·Jun 29, 2026SaveLearn
Anisotropic drag force in finite-density QGP from charged rotating 5D black holesWe study the drag force acting on a heavy quark in a holographic plasma with rotational anisotropy and finite density. The bulk dual is the CCLP black hole of five-dimensional minimal gauged…Sergei G. Ovchinnikov·Jun 29, 2026SaveLearn
Kaluza-Klein trombone mass matrices and universal class R operator spectraWe determine universal sectors of the light operator spectrum that are present in all AN-1 superconformal field theories TN[Σ3] of class R, with Σ3 a compact hyperbolic…Martin Pico, Oscar Varela·Jun 29, 2026SaveLearn
Modular Theory and the Bell-CHSH inequality in relativistic scalar Quantum Field TheoryThe Tomita-Takesaki modular theory is employed to discuss the Bell-CHSH inequality in wedge regions. By using the Bisognano-Wichmann results, the construction of a set of wedge localized vectors in…J. G. A. Caribé, M. S. Guimaraes, I. Roditi et al.·Jun 29, 2026SaveLearn
Geometric Aspects of Covariant Phase Space Formalism: Solution Space Slicings and Surface Charge IntegrabilityThe Covariant Phase Space Formalism (CPSF) provides a robust framework for deriving symplectic structures and surface charges in diffeomorphism-invariant theories. By construction, the CPSF operates…M. Golshani, M. M. Sheikh-Jabbari, V. Taghiloo et al.·Jun 29, 2026SaveLearn
All 2D generalised dilaton theories from d≥ 4 gravitiesWe demonstrate that generic two-dimensional Horndeski theories can arise from the reduction of pure gravities in d ≥ 4 dimensions, and therefore generic onshell configurations for the…Johanna Borissova·Jun 29, 2026SaveLearn
Towards W3 classical blocks with semi-degenerate operatorsWe consider 4-point W3 classical blocks focusing on the blocks level-1 and level-2 semi-degenerate operators. We derive BPZ-type equations for the auxiliary 5-point blocks with one additional…V. Belavin, Mikhail Pavlov·Jun 29, 2026SaveLearn
Tests of restricted Quantum Focusing and a new CFT boundThe restricted quantum focusing conjecture (rQFC) plays a central role in an axiomatic formulation of semiclassical gravity. Since much hinges on its validity, it is imperative to subject the rQFC to…Victor Franken, Sami Kaya, François Rondeau et al.·Jun 29, 2026SaveLearn
Massive Gauge Theories from Consistency Conditions of AmplitudesBased on the general principles of Lorentz symmetry and unitarity, we introduce two consistency conditions -- on-shell gauge symmetry and strong massive-massless continuation -- in constructing…Junmou Chen·Jun 29, 2026SaveLearn
Holographic solutions from 5D SO(2)× ISO(3) N=4 gauged supergravityWe study various types of holographic solutions from five-dimensional N=4 gauged supergravity coupled to three vector multiplets with SO(2)× ISO(3) gauge group. This gauged supergravity can…Parinya Karndumri·Jun 29, 2026SaveLearn
Virasoro OPE and Conformal Blocks from the Inverse Shapovalov FormWe derive expressions for the Virasoro OPE and four-point conformal blocks on the sphere via the resolution of identity recently determined in [Phys. Rev. D 111, 085010 (2025), arXiv:2409.12224].…Jean-François Fortin, Lorenzo Quintavalle, Witold Skiba·Jun 29, 2026SaveLearn
Axion Mixing in the String AxiverseString axiverse provides a fascinating and complex landscape for axion physics. The requirement in type IIB string axiverse models necessitates at least two axions to ensure the presence of both a…Hai-Jun Li, Yu-Feng Zhou·Jun 29, 2026SaveLearn
Realization of "ER=EPR"We provide a concrete and computable realization of the ER=EPR conjecture, by deriving the Einstein-Rosen bridge from the quantum entanglement in the thermofield double CFT. The Bekenstein-Hawking…Xin Jiang, Peng Wang, Houwen Wu et al.·Jun 29, 2026SaveLearn
Metric-like Cubic Vertices for Massless Bosonic Higher-Spin Fields in AdS3We derive parity-even transverse-traceless metric-like cubic vertices for massless bosonic higher-spin fields in AdS3. Starting from the known two- and three-derivative vertices in…Freddie King, Taylor Pomfret, Karapet Mkrtchyan·Jun 28, 2026SaveLearn
Landau's LeviathansWe present a new method together with a proof-of-concept implementation for determining the Landau singularities of Feynman integrals, read off directly from where the Euler characteristic of the…Vsevolod Chestnov, Giulio Crisanti, Mathieu Giroux·Jun 28, 2026SaveLearn
Asymptotic boundary structure of Lagrangian gauge theoriesGiven a local gauge theory on spacetime with boundary, it naturally defines another gauge theory which can be regarded as a theory of the boundary values. For Lagrangian theories, it comes equipped…Ivan Dneprov, Maxim Grigoriev, Mikhail Markov·Jun 28, 2026SaveLearn
Velocity dependence of holographic entanglement entropy in a charged plasmaWe have studied holographic entanglement entropy in a moving thermal gauge theory with a non-zero chemical potential. A sufficiently high velocity enhances the holographic entanglement entropy,…V. Esrafilian, M. Ali-Akbari·Jun 28, 2026SaveLearn
Observables in Schrödinger CFTs: How Aliens Built the PyramidsWe discuss the algebraic structure of observables in Schrödinger CFTs. These operators have zero mass (or particle number) and generically transform in staggered ''pyramid…Mathieu Boisvert, Shehab Hossam Fadda, Justin Kulp et al.·Jun 28, 2026SaveLearn
Gluon mass and small-x dynamics in hadronsPrecise derivation of the logarithmically scale-dependent Hamiltonian eigenstate picture for hadrons in the space of virtual quark and gluon states of the canonical front form of QCD requires…Stanisław D. Głazek·Jun 28, 2026SaveLearn