A Quantum Circuit Model of Black Hole Evaporation with Tunable Semi-Causality ViolationWe present a four-qubit quantum circuit model of black hole evaporation with a controlled violation of semi-causality, understood as the condition that information may fall into the black hole but…Sourav Ballav, Wen-Yu Wen, Chi-Hsien Tai·Nov 18, 2025SaveLearn
Unitary SUSY for the chiral graviton and chiral gravitino in de Sitter spacetimeIt is commonly believed that a unitary supersymmetric quantum field theory (QFT) involving graviton and gravitino fields on fixed 4-dimensional de Sitter spacetime (dS4) cannot exist due to known…Atsushi Higuchi, Vasileios A. Letsios·Nov 18, 2025SaveLearn
Sampling Polynomial Rational Remainders with SPQR: A new Package for Polynomial Division and EliminationWe introduce SPQR, a new Mathematica package for the division and elimination of variables from polynomial systems. SPQR works by sampling and reconstructing results over finite…Vsevolod Chestnov, Giulio Crisanti·Nov 18, 2025SaveLearn
Vortex stability in pseudo-Hermitian theoriesPseudo-Hermitian (including PT-symmetric) field theories support phenomenology that cannot be replicated in standard Hermitian theories. We describe a concrete example in which the vortex…R. A. Battye, S. J. Cotterill, P. Millington·Nov 18, 2025SaveLearn
Manifest symplecticity in classical scatteringThe Liouville theorem states that classical time evolution is an incompressible flow in phase space. We investigate two formulations of classical mechanics in which this property is manifested.…Joon-Hwi Kim·Nov 18, 2025SaveLearn
Infrared Quantum Electrodynamics and the Rayleigh-Jeans PhysicsInfrared quantum electrodynamics (IR-QED) acquires a natural geometric interpretation once soft photons are described as adiabatically transported electron-photon clouds. Within this framework, the…Jorge Gamboa, Natalia Tapia Arellano·Nov 17, 2025SaveLearn
Generalized Global Symmetries of T[M] Theories: Part IIWe continue the investigation of symmetries and anomalies of T[M] theories obtained by compactifying 6d SCFTs on an internal manifold M. We extend the notion of "polarizations on a manifold…Sergei Gukov, Po-Shen Hsin, Du Pei·Nov 17, 2025SaveLearn
Geometric QCD I: The Hodge-Dual Surface and Quark ConfinementThis is the first of two papers presenting a geometric framework for Planar QCD (Nc ∞). In this part, we establish the kinematic foundation of the theory by constructing the unique stable…Alexander Migdal·Nov 17, 2025SaveLearn
Surface Observables, 2-Knot Invariants, and Nonabelian Electric FluxesThis work introduces a surface observable for nonabelian four-dimensional BF theory with a cosmological term. The surface observable yields new 2-knot invariants that may extend beyond known…Alberto S. Cattaneo·Nov 17, 2025SaveLearn
Precision tests of bulk entanglement: AdS3 vectorsWe consider single-particle excitations of the massive Chern-Simons field of mass M in AdS3 and evaluate their contribution at the first sub-leading order in GN to the entanglement entropy…Rayirth Bhat, Justin R. David, Semanti Dutta·Nov 17, 2025SaveLearn
Application of Solving Inverse Scattering Problem in Holographic Bulk ReconstructionWe investigate the problem of bulk metric reconstruction in holography by leveraging the inverse scattering framework applied to boundary two-point correlation functions. We generalize our previous…Bo-Wen Fan, Run-Qiu Yang·Nov 17, 2025SaveLearn
Subleading Color Corrections at Three Loops to the tr(ϕ2) Three-Point Form Factor in N = 4 Super Yang-Mills TheoryWe compute three-loop corrections to the three-point form factor of the operator tr(ϕ2) in N = 4 Super Yang-Mills theory. In particular, our result is valid beyond the…Xin Guan, Bernhard Mistlberger, Michael Ruf·Nov 17, 2025SaveLearn
Reconstructing the Gravitational Waveform from Its Probe LimitGravitational observables for binary systems exhibit a simple polynomial dependence on the masses m1, m2 of the two scattering objects when they are written in terms of the appropriate…Carlo Heissenberg, Rodolfo Russo·Nov 17, 2025SaveLearn
Sparse Modular Forms, Lattices, and CodesMotivated by sparseness conditions for holographic CFTs, we investigate sparseness of modular forms, lattices, and codes. For this we investigate the free energy of such objects as their weight,…Christoph A. Keller, Ashley Winter Roberts·Nov 17, 2025SaveLearn
Elementary Constituents ConjectureIn this note, we conjecture and provide evidence that quantum gravity cobordism classes are trivialized by elementary generators with tension at most order 1 in Planck units. Motivated by the…Vinicius Nevoa, Sanjay Raman, Cumrun Vafa·Nov 17, 2025SaveLearn
Bosonisation Cohomology: Spin Structure Summation in Every DimensionGauging fermion parity and summing over spin structures are subtly distinct operations. We introduce 'bosonisation cohomology' groups HBd+2(X) to capture this difference, for theories…Philip Boyle Smith, Joe Davighi·Nov 17, 2025SaveLearn
TT Deformations and Form Factor ProgramIn this proceeding contribution, we review a recently proposed method to compute the minimal form factors (MFFs) of diagonal integrable field theories perturbed by irrelevant fields of the TT…Olalla A. Castro-Alvaredo, Stefano Negro, Fabio Sailis·Nov 17, 2025SaveLearn
Global quenches and correlator dynamics in de Sitter spaceWe study non-equilibrium initial states of quantum fields in curved space-time and develop a framework for describing global quenches as unitary perturbations of the initial density matrix. Using the…Ivan A. Belkovich, Damir Sadekov, Gleb S. Zverev·Nov 17, 2025SaveLearn
Notes on Quantum Effective ActionsWe first note that, at least in perturbation theory, there is a well-defined (subject to regularization) Lorentzian definition of the quantum effective action in both flat and curved space including…S. P. de Alwis·Nov 17, 2025SaveLearn
IR/UV mixing from higher-order interactions in a Scalar FieldThe observed vacuum energy lies far below quantum-field-theoretic estimates. Weinberg's theorem shows that no field can dynamically relax the cosmological constant to zero in a local theory with…Satish Ramakrishna·Nov 16, 2025SaveLearn
Spinors and the quaternionic Poincaré groupWhen four dimensional spacetime R is considered as locally embedded on a larger manifold M, labelled by higher division algebra coordinates, a natural question to ask is how much of the symmetry…R. Vilela Mendes·Nov 16, 2025SaveLearn
Orientations of Orbi-K-Theory measuring Topological Phases and Brane ChargesTopological Chern phases of quantum materials, as well as brane charges on M-theory orbifolds, have famously been argued to be classified by (orbi) topological K-theory, or possibly by other stable…Hisham Sati, Urs Schreiber·Nov 16, 2025SaveLearn
E-Strings and Four-ManifoldsWe investigate the physics of the E-string theory and its compactifications as well as their applications to four-dimensional topology. In particular, we compute the partition function of the…Du Pei, David H. Wu·Nov 14, 2025SaveLearn
Analyticity of the Black Hole S-MatrixWe establish the analytic structure of the S-matrix in the complex-frequency plane for classical wave scattering on a Schwarzschild background in four space-time dimensions. Our argument relies on…Miguel Correia, Tushar Gopalka, Giulia Isabella et al.·Nov 14, 2025SaveLearn
Integrability for the spectrum of Jordanian AdS/CFTJordanian deformations offer rare integrable realisations of non-AdS holography, whose solvability methods differ from conventional AdS/CFT examples. Here we study the sl(2,R) sector of…Sibylle Driezen, Fedor Levkovich-Maslyuk, Adrien Molines·Nov 14, 2025SaveLearn