Unifying spherical convolutions through liftingWe develop a unified description of convolution on the sphere by lifting to the rotation group. A number of definitions of spherical convolution have been proposed, differing in whether the kernel is…J. D. McEwen·Oct 9, 2026SaveLearn
Perturbed isotropic oscillators with inversion symmetryWe consider the normal form of a 1:1 detuned resonance that can be related, via a double averaging process, to the three body problem of celestial mechanics. In view of the symmetry in the…Antonella Marchesiello, Rita Mastroianni, Giuseppe Pucacco·Oct 9, 2026SaveLearn
Critical Ising model as the M(4,3) minimal model of conformal field theoryWe construct a linear map from the space of spin polynomials in the critical Ising model on a lattice to the state space of the M(4,3) minimal model of conformal field theory. The kernel of the map…Dmitry Chelkak, Konstantin Izyurov, Kalle Kytölä·Oct 9, 2026SaveLearn
A Sklar-Type Decomposition for Positive Binary Distributions and a Gibbs InterpretationWe study strictly positive multivariate binary distributions by separating one-body marginals from dependence. Local positive reweighting defines a dependence nucleus, completely characterized by the…Yi-Yu Lin·Oct 8, 2026SaveLearn
Lieb-Robinson bounds for irreversible dynamics via adaptive Dyson expansionIn this note, we study a broad class of time-dependent and irreversible dynamics for quantum spin systems in both finite and infinite volume. We develop a simple and flexible strategy for expanding…Carla Rubiliani, Marius Wesle, Tom Wessel·Oct 8, 2026SaveLearn
An elementary approach to the Szegő theoremsThe strong Szegő theorem and the Fisher-Hartwig formula describe the asymptotic behavior of determinants obtained by restricting translationally invariant operators to large finite regions. In…Israel Klich, Ravisankar Rajagopal·Oct 8, 2026SaveLearn
Wave packets asymptotics in κ-minkowski spaceIn this paper, we study the nature of wave packets and their decay behavior in the κ-Minkowski space. We employ techniques from singularity theory throughout our analysis. Specifically, we use…Adith A, A. Bhagwat·Oct 8, 2026SaveLearn
Multipartite entanglement spreadsThe entanglement structure of a bipartite pure state is characterized by its entanglement spectrum, or equivalently, by the family of Rényi-k entanglement entropies with integer k. Taking the…Sylvain Carrozza, Johann Chevrier, Luca Lionni·Oct 8, 2026SaveLearn
Wrinkling of a bilayered cylinder under tensionWe study near-surface tension instabilities in bilayered cylinders composed of an incompressible core coated with a thin compressible film. In theory, circumferential wrinkles with axial wavefronts…Chiara Lonati, Sairam Pamulaparthi Venkata, Kevin Moerman et al.·Oct 8, 2026SaveLearn
Extended States on the Bethe Lattice RevisitedWe give a short proof of the classical weak-disorder result that the Anderson model on the Bethe lattice has purely absolutely continuous spectrum on compact intervals in the interior of the free…Vojkan Jaksic, Yoram Last·Oct 8, 2026SaveLearn
Uniformity theory of weighted compositesBy including spatially varying volume fractions of the constituents, composites are obtained that are akin to functionally graded media. An extension of the mathematical apparatus of double groupoids…Marcelo Epstein, Mohammadjavad Javadi·Oct 8, 2026SaveLearn
Finite- and long-range spin-wave free-energy asymptotics for the two-dimensional quantum Heisenberg ferromagnetFor the two-dimensional quantum Heisenberg ferromagnet with asymptotically radial power-law exchange, we prove the leading low-temperature free energy at every fixed spin, uniformly on the weak-field…Andreas Klippel·Oct 7, 2026SaveLearn
Iterated Graph Systems (II): Bernoulli percolation and critical-exponent universality classes on hierarchical latticesWe study Bernoulli percolation and its universality classes on hierarchical lattices generated by edge iterated graph systems (EIGS). By examining eight critical exponents, we prove that no finite…Ziyu Neroli·Oct 7, 2026SaveLearn
Asymptotic Neutrality for the Ionization Conjecture in the Two-Center Thomas-Fermi-Dirac-von Weizsäcker TheoryThe ionization conjecture for the Thomas-Fermi-Dirac-von Weizsäcker model asks how many electrons a given nuclear configuration can bind. So far, only the single-center case has been settled by…Lu Chen, Yong Wu·Oct 7, 2026SaveLearn
Operator Schmidt Rank and the Geometry of Schmidt ProfilesThe main result of the paper states that if 0≠ v∈ Cm Cn, d=\m,n\, and p=SR(v), then for every 1 q d, equation* \OSR( U):…Mohsen Kian, Mohammad Sal Moslehian·Oct 7, 2026SaveLearn
Absence of Absolutely Continuous Spectrum for One-Dimensional Capacitance Operators with Critical Long-Range InteractionsIn this paper, we establish the absence of absolutely continuous spectrum for scalar one-dimensional Laurent operators with multiplicative disorder and critical long-range hoppings. In particular,…Habib Ammari, Jiayu Qiu·Oct 7, 2026SaveLearn
Matrix Product State Representatives of Symmetry-Protected PhasesWe provide a simple ansatz for finding integer spin SO(3)×2T×2R-invariant matrix product states representing a phase for each triple of 2 topological indices studied in the…Thomas Jackson·Oct 7, 2026SaveLearn
Nematic order in monomer-dimer models of Heilmann and Lieb with lateral attraction in dimensions d 2We study the d-dimensional generalization of Models II (d=2) and V (d=3) for liquid crystals introduced by Heilmann--Lieb (1979), which consists of dimers on the hypercubic lattice at chemical…Qidong He·Oct 6, 2026SaveLearn
Conformal invariance of the planar four-state Potts model and its random-cluster representationFor the critical random-cluster model on Z2 with cluster-weight q=4, we prove the convergence of loops to CLE(4) in the scaling limit. Conformal invariance of the four-state Potts model…Emile Averous, Hugo Duminil-Copin, Tiancheng He et al.·Oct 6, 2026SaveLearn
An unified approach for the (inverted) quantum harmonic oscillator and the Berry-Keating hamiltonianWe propose an unified view to three well known quadratic Hamiltonians widely considered in quantum mechanics, i.e. those of the harmonic oscillator, of the inverted harmonic oscillator, and the…Fabio Bagarello, Emanuele Balistreri, Sergey Kuzhel·Oct 6, 2026SaveLearn
Stability of Matter Interacting with Classical Non-Abelian Gauge FieldsStability of matter is the property that the ground state energy of N charged quantum particles is bounded below by -CN, with C independent of N. We ask whether this holds for colour-charged…Robin Reuvers, Jan Philip Solovej, David Stuart·Oct 6, 2026SaveLearn
Localization Dichotomy for Hall Insulators on the LatticeWe prove the localization dichotomy conjecture for non-periodic Hall insulators on the lattice. That is, we show that the Fermi projector P of a gapped exponentially local Hamiltonian on…Alex Bols·Oct 6, 2026SaveLearn
Convergence Without Finite Exactness in the Eigenstate Quantum BootstrapThe eigenstate quantum-mechanical bootstrap can converge to the physical moment set while remaining nonexact at every finite order. We prove this for a one-dimensional quasi-exactly solvable sextic…Ye Zhou, Daniel Keren·Oct 6, 2026SaveLearn
Pulsation of quantum walk on finite graphWe study discrete-time quantum walks on weighted graphs, where every edge in an edge cut set is assigned a small weight ε>0. The parameter ε represents the strength of the connections through the…Taisuke Hosaka, Etsuo Segawa·Oct 6, 2026SaveLearn
A mathematical analogy between certain hollow vortex and bubble flows - existence, uniqueness, and identical boundary shapesWe study two physically distinct steady free-boundary problems in a two-dimensional inviscid fluid: a hollow vortex in a constant-vorticity flow subject to simple shear, third order and linear strain…Valentin D. Kunz, Saleh Tanveer, Darren G. Crowdy·Oct 6, 2026SaveLearn