Continuing past the inner horizon using WKBFeatures of the black hole interior can be extracted from the analytic structure of boundary correlation functions. Working in the geodesic approximation, we find analytic continuations that probe…Shadi Ali Ahmad, Ahmed Almheiri, Simon Lin·Jan 5, 2026SaveLearn
On the temperature of the quantum black holeA nontrivial peculiarity of general relativity is that when the horizon region of black holes is rendered harmless, the exterior doubles, resulting in a causally disconnected parallel universe. This…Abram Akal·Jan 5, 2026SaveLearn
More on Pre-Inflationary Non GaussianitiesI generalize the three-point amplitude of curvature perturbations in the climbing scenario inspired by ten-dimensional non-supersymmetric strings to a broader class of exponential potentials, under…M. Meo·Jan 5, 2026SaveLearn
Entanglement Viscosity: from Unitarity to Irreversibility in Accelerated FramesWe demonstrate that the unitarity of quantum field theory, through the positivity of spectral functions, underlies thermodynamic irreversibility for a subsystem separated by a horizon, in direct…G. Yu. Prokhorov·Jan 5, 2026SaveLearn
Wilson-'t Hooft classification and the perimeter law for dyonic loops in 3d monopole semiclassicsWe investigate the long-distance behavior of dyonic loop operators in 4d SU(N) gauge theories on R3 × S1 using the 3d monopole semiclassics. If we employ the naive definition of…Yui Hayashi, Yuya Tanizaki·Jan 5, 2026SaveLearn
Critical Phenomena on the Bethe LatticeWe investigate the critical behavior of a family of Z2-symmetric scalar field theories on the Bethe lattice (the tree limit of regular hyperbolic tessellations) using both the…Rudrajit Banerjee, Nicolas Delporte, Saswato Sen et al.·Jan 5, 2026SaveLearn
Quark confinement due to unified magnetic monopoles and vortices reduced from symmetric instantons with holographyWe develop a geometric framework to analyze quark confinement in four-dimensional Euclidean SU(2) Yang--Mills theory in terms of finite-action topological defects. Starting from self-dual…Kei-Ichi Kondo·Jan 5, 2026SaveLearn
Machine learning modularityBased on a transformer based sequence-to-sequence architecture combined with a dynamic batching algorithm, this work introduces a machine learning framework for automatically simplifying complex…Yi Fan, Vishnu Jejjala, Yang Lei·Jan 5, 2026SaveLearn
Tripartite Correlation Signal from Multipartite Entanglement of PurificationWe propose a signal Δ(3)p for genuine tripartite entanglement in finite-dimensional quantum systems and Δ(3)w for holographic systems. We prove that Δ(3)p is non-negative for any…Ning Bao, Keiichiro Furuya, Joydeep Naskar·Jan 5, 2026SaveLearn
More About the Spontaneous Breaking of Time Reversal in de Sitter SpaceIt is widely thought that the quantum theory of de Sitter space requires the existence of a physical observer in the static patch. What exactly is meant by an observer is unclear; it could be…Leonard Susskind·Jan 4, 2026SaveLearn
Gaussian fluctuating Generally covariant diffusionWe extend the previously developed [1] generally covariant formalism to include diffusion of conserved charges, and comment on the seming difference between the chemica potential term and the…David Montenegro, Giorgio Torrieri·Jan 4, 2026SaveLearn
Duality and Axion WormholesThe prototype of a Euclidean wormhole solution of Einstein gravity coupled to matter is the axion wormhole in four spacetime dimensions. In this primarily expository article, we spell out some…Edward Witten·Jan 4, 2026SaveLearn
On stability of baryonic black membranesNear-extremal black membranes with topological (baryonic) U(1)B charge of M-theory compactified on the coset space M1,1,0 are stable. M1,1,0 coset is a Z2-invariant…Alex Buchel·Jan 4, 2026SaveLearn
Point Particles as Spin ChainsThis work surveys a recently developed approach to the study of free point particles on Riemannian manifolds, based on the Kirillov orbit method, geometric quantization, and the geometry of…Viacheslav Krivorol·Jan 4, 2026SaveLearn
Tori, Klein Bottles, and Modulo 8 Parity/Time-reversal Anomalies of 2+1d Staggered FermionsWe study the symmetries of lattice staggered fermions in 2+1d. Using the symmetries, we can place the system on any sheared torus or Klein bottle. These different backgrounds provide diagnostics of…Nathan Seiberg, Wucheng Zhang·Jan 3, 2026SaveLearn
From the Wavefunction of the Universe to In-In-Correlators: A Perturbative Map to All OrdersBoth the Wavefunction of the Universe and the Schwinger-Keldysh in-in formalism are central tools for analyzing primordial cosmological observables, such as equal-time correlation functions. While…Gonzalo A. Palma·Jan 2, 2026SaveLearn
Spin-operator form factors of the critical Ising chain and their finite volume scaling limitsIn this work, we provide a self-contained derivation of the spin-operator matrix elements in the fermionic basis, for the critical periodic Ising chain at a generic system length N∈ 2Z 2.…Yizhuang Liu·Jan 2, 2026SaveLearn
Extended BMS representations and stringsWe construct in detail the irreducible representations of the BMS group with super rotations in three and four dimensions that have the same rest frame momenta as the massive and massless Poincare…Romain Ruzziconi, Peter West·Jan 2, 2026SaveLearn
Thermal and Casimir effects in a Lorentz-violating massive scalar fieldIn this work, a massive scalar field theory incorporating Lorentz violation is investigated. The symmetry breaking is introduced via a background traceless antisymmetric tensor. Within the framework…D. S. Cabral, L. H. A. R. Ferreira, L. A. S. Evangelista et al.·Jan 2, 2026SaveLearn
The JLMS formula in a large code with approximate error correctionGauge/gravity duality is often described as a quantum error correcting code. However, as seen in the Jafferis-Lewkowycz-Maldacena-Suh (JLMS) formula, exact quantum error correction with complementary…Xi Dong, Donald Marolf, Pratik Rath·Jan 1, 2026SaveLearn
One loop renormalization of 5D gauge-Yukawa theoriesThe common lore dictates that extra dimensional theories loose predictive power at energies just above the compatification scale, due to the power-law running of bulk coupling. We show that…Giacomo Cacciapaglia, Wanda Isnard, Roman Pasechnik et al.·Jan 1, 2026SaveLearn
Log Soft Constraints on KMOC FormalismThe KMOC formalism provides a systematic framework for extracting classical observables perturbatively from on-shell scattering amplitudes. In this work, we apply this formalism to compute…Siddhartha Paul, Adarsh Vishwakarma·Jan 1, 2026SaveLearn
Generalized 2-split for higher-derivative YM and GR amplitudes at tree-levelWe study the generalized 2-split of higher-derivative amplitudes, including Yang-Mills (YM) and Gravity (GR) amplitudes with special insertions of higher-derivative vertices, by expanding them into…Liang Zhang, Kang Zhou·Jan 1, 2026SaveLearn
Equivariant Cohomology, BRST Quantization, and Analytic Localization: A Unified FrameworkThis paper provides a detailed exposition of the two main models for equivariant cohomology -- the Cartan and Weil models -- and their explicit isomorphism via the Kalkman (Mathai--Quillen)…Lixin Xu·Jan 1, 2026SaveLearn
Soft Algebras in AdS4 from Light Ray Operators in CFT3Flat Minkowski space (M4) and AdS4 can both be conformally mapped to the Einstein cylinder. The maps may be judiciously chosen so that some null generators of the I+ boundary of…Ahmed Sheta, Andrew Strominger, Adam Tropper et al.·Dec 31, 2025SaveLearn