Channel-Resolved High-Overtone Quasinormal Modes Decode Kasner Scaling inside Black HolesThe high-overtone quasinormal-mode spectrum encodes the near-singularity Kasner scaling of black-hole interiors. We show that distinct structures in this spectrum independently determine the temporal…Zi-Qing Xiao, Jun Nian, Li Li·Sep 15, 2026·Top 7%SaveLearn
Topological Modular Forms Constrain Threshold States in Extremal N=1 AdS3 GravityWe identify a topological constraint on extremal N=1 AdS3 spectra that is not implied by genus-one modular covariance of the three even spin structure partition functions. Assuming the…Yutaka Yoshida·Sep 15, 2026·Top 47%SaveLearn
Low-energy brane decoupling in AdS flux vacuaWe study the decoupling of branes sourcing AdS flux vacua from the asymptotic bulk using scalar-wave absorption probabilities. In a one-modulus truncation, the result depends only on the dimension of…Fien Apers, Noelia Sánchez González·Sep 15, 2026·Top 86%SaveLearn
Cohomological Aspects of Entanglement Entropy: From Information Theory to Noncommutative GeometryWe develop a cohomological framework for entanglement entropy that unifies perspectives from information theory, operator algebras, and noncommutative geometry. Starting from the…Radoslav C. Rashkov·Sep 15, 2026·Top 43%SaveLearn
Generalized complexity and dynamical response in holographic Vaidya spacetimesWe investigate "Complexity=Anything" for smooth Vaidya geometries, using the Weyl squared functional as the most common candidate for our study. Our numerical analysis of candidates in 4- and…Mojtaba Shahbazi, Monireh Emami·Sep 15, 2026·Top 63%SaveLearn
Supersymmetric extension of the Hull--Lambert--Sen chiral boson on the 2-TorusWe present a supersymmetric extension of the Hull-Lambert-Sen chiral boson model. The two-metric formulation developed by Hull provides a powerful and tractable framework for the quantization of…Amine El Amri, Pietro Antonio Grassi·Sep 15, 2026·Top 94%SaveLearn
Carrollian Conformal Dynamics and Flat-Space HolographyThe conformal boundary of asymptotically flat spacetime is null and therefore carries a Carrollian rather than Lorentzian geometry. This changes the relation between symmetry, variational principles…Simon Pekar·Sep 15, 2026·Top 61%SaveLearn
Constraints on Kasner Exponents from Holography and Energy ConditionsA central question in bottom-up holography is whether a given bulk effective theory admits a consistent holographic dual. In this work, we explore whether the near-singularity Kasner scaling of…Zi-Hao Li, Run-Qiu Yang·Sep 15, 2026·Top 68%SaveLearn
Positivity Bounds in N =1 SupersymmetryFor a low-energy Effective Field Theory (EFT) to admit a consistent ultraviolet (UV) completion, it must adhere to the fundamental principles of locality, unitarity, analyticity, and Lorentz…Jingxuan Bu, Jiayin Gu, Runqing Wang·Sep 15, 2026·Top 61%SaveLearn
Unitarity and the Forward Direction in Theories with Long-Range ForcesIntegrating scattering amplitudes over the forward direction, and consequently the unitarity constraints one extracts from such integrals, can appear ambiguous in theories with long-range forces.…Luke Lippstreu·Sep 15, 2026·Top 16%SaveLearn
Stringy Gauge StructuresA field theory action, able to incorporate stringy gauge symmetry enhancement-breaking effects, which occur at particular points of moduli space in a heterotic string toroidal compactification…Gerardo Aldazabal, Eduardo Andrés, Lucía M. Cabrera et al.·Sep 15, 2026·Top 79%SaveLearn
Edge observables in Maxwell theory on null boundariesWe study edge observables in three-dimensional Maxwell theory on null boundaries using a Hamiltonian formulation adapted to null foliations. We consider three backgrounds: Minkowski spacetime, the…Dušan Đorđević, Olivera Miskovic, Antonia Montecinos et al.·Sep 14, 2026·Top 60%SaveLearn
Zero- and Finite-Temperature Casimir Effect in a Fracton Gauge FieldWe investigate the zero- and finite-temperature Casimir interaction of the free trace-full scalar-charge fracton gauge field between two parallel reflecting boundaries. A variational analysis…Celio R. Muniz·Sep 14, 2026·Top 57%SaveLearn
A dS4 maximum in M-theory from Casimir energies on Riemann-flat manifoldsWe describe a fully explicit, four-dimensional, top-down de Sitter saddle, constructed via compactification of M-theory on the Riemann-flat manifold T7/Z8. The solution has a vacuum…Miquel Aparici, Bruno Valeixo Bento, Miguel Montero·Sep 14, 2026·Top 18%SaveLearn
Instanton Interactions and the Axion Weak Gravity ConjectureThe Weak Gravity Conjecture admits a formulation in terms of long-range charged particle self-interactions being repulsive. We adopt a similar approach to the Axionic Weak Gravity Conjecture by…Jarod Hattab, Eran Palti·Sep 14, 2026·Top 46%SaveLearn
Schwinger-Keldysh effective actions for non-hydrodynamic poles and branch cutsRetarded thermal correlators, analytically continued to complex frequency, exhibit non-hydrodynamic poles and branch cuts that constrain hydrodynamics. We construct Gaussian Schwinger-Keldysh…Andrea Amoretti, Matteo Anselmi, Daniel K. Brattan·Sep 14, 2026·Top 53%SaveLearn
Persistent Spontaneous Time-Reversal BreakingWe provide an analytic realization of spontaneous parity and time-reversal breaking without thermal restoration in a local, unitary, ultraviolet-complete quantum field theory in 2+1 dimensions with…Michael Smolkin, Lev Yung·Sep 14, 2026·Top 6%SaveLearn
Making the Great Desert BloomThe absence of new physics beyond neutrino masses between the weak scale and the Planck scale is referred to as the great desert. It is often seen as a nightmare scenario for particle physics. Here…Jacques Distler, Andreas Karch·Sep 14, 2026·Top 62%SaveLearn
The Role of Completeness in Probing Symmetry BreakingCompleteness is widely recognized in quantum information as an important property of a family of monotones, because it ensures that no information relevant to state conversion is lost. We show that…Yuya Kusuki, Hiroyasu Tajima, Shion Yamashika·Sep 14, 2026·Top 9%SaveLearn
Separation of variables for non-diagonalisable models: XXX with twisted boundary conditionsWe study the Heisenberg XXX spin chain with twisted periodic boundary conditions with a defective twist matrix. Using quantum separation of variables, we show that the generalised eigenvectors of…Juan Miguel Nieto García·Sep 14, 2026·Top 81%SaveLearn
Symmetry Descent in M-theory, Part I: A Twelve-Dimensional Parent TheoryWe initiate a symmetry descent procedure for M-theory engineered quantum field theories. Starting from a higher form BF theory supplemented by a cubic bulk topological interaction, we construct a…Pinak Banerjee, Subham Roy, Xingyang Yu·Sep 14, 2026·Top 36%SaveLearn
D-term and F-term potential of non-Abelian D7-branes in IIB Calabi-Yau orientifoldsWe derive the 4d D-term and F-term potential generated by a D7-brane stack in Calabi-Yau orientifold compactifications of type IIB string theory, taking into account the effect of worldvolume and…Daniel Junghans·Sep 14, 2026·Top 2%SaveLearn
Exact group invariant scar towers in two dimensional gauge theoriesWe construct exact many-body scar towers in two dimensional gauge theories with two flavors of massless fundamental fermions. For oppositely charged fermions, the scar subspace is generated by a…João Barata, Kiryl Pakrouski, Andrey V. Sadofyev·Sep 14, 2026·Top 15%SaveLearn
Single-Instance Observables in the Sachdev-Ye-Kitaev ModelWe present a diagrammatic expansion for thermal expectation values of low-weight Majorana strings in a fixed realization of the N-fermion Sachdev--Ye--Kitaev (SYK) model. At each order in the…Brian Swingle·Sep 14, 2026·Top 57%SaveLearn
An attempt to derive the LVS from a 10d EFT perspectiveNon-perturbative scalar potentials are a central ingredient for stabilising moduli in flux compactifications. A key target in this context is the direct 10d derivation of the LVS AdS potential, i.e.,…Arthur Hebecker, Andreas Schachner, Gaetano Maria Sifo·Sep 14, 2026·Top 93%SaveLearn