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math-ph

Mathematical Physics

Articles in this category focus on areas of research that illustrate the application of mathematics to problems in physics, develop mathematical methods for such applications, or provide mathematically rigorous formulations of existing physical theories. Submissions to math-ph should be of interest to both physically oriented mathematicians and mathematically oriented physicists; submissions which are primarily of interest to theoretical physicists or to mathematicians should probably be directed to the respective physics/math categories

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math-ph 2026-05-13 2 theorems

Tree-like pairings guarantee factorization of tensor invariants at large N

Large N factorization of families of tensor trace-invariants

The criterion identifies families whose moments factorize, allowing explicit computation of typical multipartite Renyi entropies in random量子

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It was recently proven that, in contrast to their matrix analogues, the moments of a real Gaussian tensor of size N do not in general factorize over their connected components in the asymptotic large N limit. While the original proof of this rather surprising result was not constructive, explicit examples of non-factorizing moments, which are expectation values of trace-invariants, have since then been discovered. We explore further aspects of this problem, with a focus on Haar-distributed (or Gaussian) complex random tensors, which are more directly relevant to quantum information. We start out by exhibiting an explicit example of non-factorizing trace-invariant, thereby filling a gap in the recent literature. We then turn to the opposite question: that of finding interesting families of trace-invariants that do in fact factorize at large N. We establish three main theorems in this regard. The first one provides a sufficient combinatorial bound ensuring large N factorization, that is also simple enough to be applicable to various cases of practical relevance. Our second main result shows that the expectation value of any compatible trace-invariant is dominated by certain tree-like combinatorial structures at large N, which we refer to as tree-like dominant pairings. Our third main theorem establishes that any trace-invariant admitting tree-like dominant pairings does actually factorize at large N. In this way, we are able to prove that various families of trace-invariants that have been previously studied in the literature do factorize at large N. We apply our findings to the theory of multipartite quantum entanglement: to any trace-invariant is associated a multipartite generalization of R\'enyi entanglement entropy, whose typical expectation value in the uniform random quantum state can be explicitly computed assuming large N factorization.
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math-ph 2026-05-13 2 theorems

Exact stationary PDF for reflected random walks derived analytically

An analytical approach to calculating stationary PDFs for reflected random walks with an application to BESS-based ramp-rate control

Neumann series solves the integral equation to give precise BESS inverter sizing for renewable ramp control.

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A Wiener-Hopf-type integral equation for the stationary PDF of a reflected random walk is derived rigorously based on modern probability theory, and an application to battery energy storage systems (BESS), specifically the sizing of the inverter, is discussed in depth. The methodological steps include the construction of a Markov kernel, the derivation of a Fredholm integral equation of the second kind for the PDF of the BESS power, and an analytical solution of the equation based on a Neumann series. The analytical results were compared against numerical solutions obtained with the Nystrom method, as well as against the results of an algorithmic simulation using simulated input time series. The use of truncated versions of the analytic solution allows for the construction of simplified design rules for the power systems practitioner. General insights into inverter sizing criteria of storage systems for ramp-rate control of variable renewable energy (VRE) sources such as wind and solar are provided.
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math-ph 2026-05-13 2 theorems

Fractal supports follow Takagi functions for uniform seabed load

Quasi-Sierpinski Structure for Uniform Load Distribution

Quasi-Sierpinski structure rests directly on the seabed by displacing supports vertically according to Takagi-class functions, linking to a

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Land reclamation methods, indispensable for the proper development of modern coastal cities, are ecologically destructive. We present a fractal structure, similar to a Sierpinski triangle, which solves this problem by resting directly on the seabed thanks to the uniform load distribution we achieve on its base. To obtain this uniform distribution, we show that the supports of the structure must displace vertically following any function of the Takagi class. This causes the vertical deformations of the structure to follow this same class and the horizontal deformations to be related to the Cantor function. The structure works with an unlimited number of combinations of areas of its elements and materials, which gives designers a high degree of constructive flexibility.
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math-ph 2026-05-13 1 theorem

AKLT ground states match across finite and infinite volumes on two lattices

Local Topological Quantum Order and Spectral Gap Stability for the AKLT Models on the Hexagonal and Lieb Lattices

This equivalence with uniform exponential accuracy implies the spectral gap stays open under small perturbations.

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We prove that the ground state of the AKLT models on the hexagonal lattice and the Lieb lattice satisfy the local topological quantum order (LTQO) condition. This will be a consequence of proving that the finite volume ground states are indistinguishable from a unique infinite volume ground state. Concretely, we identify a sequence of increasing and absorbing finite volumes for which any finite volume ground state expectation is well approximated by the infinite volume state with error decaying at a uniform exponential rate in the distance between the support of the observable and boundary of the finite volume. As a corollary to the LTQO property, we obtain that the spectral gap above the ground state in these models is stable under general small perturbations of sufficient decay. We prove these results by a detailed analysis of the polymer representation of the ground states state derived by Kennedy, Lieb and Tasaki (1988) with the necessary modifications required for proving the strong form of ground state indistinguishability needed for LTQO.
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math-ph 2026-05-13 2 theorems

iQuad sensor's linear operator equals its own adjoint

A self-adjoint Fourier-type model for the iQuad wavefront sensor

Link to the 2D finite Hilbert transform makes it self-adjoint, unlike other Fourier-type sensors, and enables simpler reconstruction.

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Advanced adaptive optics (AO) systems can use Fourier-type wavefront sensing to correct optical distortions encountered in ground-based telescopes, AO-assisted retinal imaging, and free-space optical communications (FSOC). Recently, a novel Fourier-type wavefront sensor (WFS) known as the iQuad WFS has been introduced. Its design features a focal plane tessellation with a four-quadrant phase mask (FQPM) that incorporates a $\pm \pi/2$ phase shift between adjacent quadrants. In this work, we establish a comprehensive mathematical framework for the iQuad WFS, including its forward models and linearizations based on the Fr\'echet derivative. We reveal a connection between the iQuad WFS and the 2d finite Hilbert transform and demonstrate that the linear iQuad WFS operator is self-adjoint - a unique property among Fourier-type WFSs. Additionally, we introduce the double iQuad WFS, a two-path configuration that combines two rotated iQuad WFSs. This design addresses the limitations of the single iQuad WFS by suppressing poorly-seen phase components. Moreover, the double setup simplifies the mathematical modeling. We also highlight iQuad similarities to the widely used pyramid wavefront sensor (PWFS). Finally, we extend the concept of modulation to the iQuad WFS, further enhancing its versatility. The theoretical analysis presented here lays the groundwork for the development of fast and robust model-based wavefront reconstruction algorithms for the iQuad WFS, paving the way for future applications in AO instruments.
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math-ph 2026-05-13 2 theorems

Feynman-Kac formula holds for renormalized spin-boson model

A Feynman-Kac Formula for the Subcritical Ultraviolet-Renormalized Spin Boson Model

Ground states of infrared-regular models survive removal of the ultraviolet cutoff

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We prove a Feynman-Kac formula (FKF) for the self-energy renormalized spin boson Hamiltonian, describing a two-state quantum system linearly coupled to a bosonic quantum field. Similar to recent FKFs for the Fr\"ohlich polaron and the non- and semi-relativistic Nelson models, it yields a probabilistic treatment of the spin as a jump process, but treats the field on the usual bosonic Fock space. As an application, we prove that the existence of ground states for infrared-regular models persists the removal of an ultraviolet cutoff.
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math-ph 2026-05-13 Recognition

Deterministic motion emerges exactly as contact-flow attractor

When Stochasticity Resolves into Certainty: Hidden Structure of Deterministic Motion

In dissipative systems stochasticity resolves into certainty when gradient amplification is balanced by stiffness decay on a Jacobian-sett

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We prove that deterministic motion in dissipative systems emerges as a strict geometric attractor of contact flow, not a statistical approximation. Building on the contact geometry of stochastic vector bundles, we develop time-dependent contact potentials with an exact closure theorem ensuring exact satisfaction of the master equation at any finite order. The Contact Locking Theorem shows that exponential gradient amplification of the probability field is precisely counterbalanced by synchronous stiffness decay, forcing the effective macroscopic-microscopic coupling to vanish exponentially. Deterministic dynamics therefore emerges through deterministic focusing with a universal timescale governed by the drift-field Jacobian spectrum. Validation of the damped-driven Duffing oscillator confirms the predicted rate and exponential convergence.
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math-ph 2026-05-12 2 theorems

Casimir forces between point obstacles always attract

Vacuum and thermal fluctuations of a scalar field with point interactions

A convergent Born series decomposes them into non-local pairwise terms acting along lines that connect the obstacles.

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We investigate the vacuum and thermal fluctuations of a neutral massless scalar field living in Minkowski spacetime and interacting with a finite number of point-like obstacles, modelled by zero-range potentials. The system is described rigorously in terms of self-adjoint realizations of the Laplacian, under assumptions ensuring the absence of instabilities. Using the relative zeta-function technique, we determine the renormalized connected partition function and derive explicit expressions for the thermodynamic observables, characterizing both their low- and high-temperature behaviours. Furthermore, we derive of a convergent Born series expansion for the Casimir energy, which identifies multiple-scattering processes as the mechanism underlying vacuum forces. The latter decompose into pairwise contributions directed along the lines joining the obstacles, with intensities depending non-locally on the full configuration. We also present some numerical results for identical obstacles, indicating that the Casimir forces are always attractive in this context.
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math-ph 2026-05-12 2 theorems

Observables on n-plectic manifolds form a Kan-complex n-groupoid

A Simplicial Approach to Higher Geometric Quantization

Recursive gluing via a codimension-tracking Grassmann variable produces the simplicial model and a matching polarization quantization.

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This paper develops a unified framework for observables in n-plectic geometry, extending the L_infty-algebra of Hamiltonian (n-1)-forms to Hamiltonian forms of all degrees via a degree-shifting Grassmann variable u that encodes submanifold codimension. Interpreting k-form observables as k-dimensional topological defects yields a recursive gluing construction that assembles into a semi-simplicial set sOb_bullet(M), which we prove satisfies the Kan filling property, thereby providing an n-groupoid model for observables. From this semi-simplicial perspective we extract cohomological invariants and construct a recursive inner product leading to a categorified pre-n-Hilbert space. The hierarchical structure of polarizations yields a natural quantization scheme matching the 1-polarization classification of multisymplectic geometry. The resulting framework bridges higher algebraic structures with higher categorical geometry and establishes a systematic foundation for the geometric quantization of extended objects.
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math-ph 2026-05-12 2 theorems

New axiom secures Haag duality for cones in topological order

Local topological order, Haag duality, and reflection positivity

It holds for every known commuting-projector model and supplies an independent proof for string-net constructions

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In our previous article [arXiv:2307.12552], we introduced local topological order (LTO) axioms for abstract quantum spin systems which allow one to access topological order via a boundary algebra construction. Using the LTO axioms, we produced a canonical pure state on the quasi-local algebra, which gives a net of von Neumann algebras associated to a poset of cones in $\mathbb{R}^n$. In this article, motivated by [arXiv:2509.23734], we introduce an axiom for LTOs which ensures Haag duality for cone-like regions using Tomita-Takesaki theory. We prove this axiom is satisfied for all known topologically ordered commuting projector models. We thus get an independent proof of Haag duality for the Levin-Wen string net models originally proved in [arXiv:2509.23734]. We also give a reflection positivity axiom for LTOs, connecting to the recent article [arXiv:2510.20662]. We again prove this axiom is satisfied for all known topologically ordered commuting projector models about some $\mathbb{Z}/2$-reflection symmetry.
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math-ph 2026-05-12 Recognition

Cutoff spectral triples converge to minimally coupled Dirac operator

From Noncommutative Kinematics to \(U(1)_{star}\) Gauge Theory: A Family of Spectral Triples with Localized Gauge-induced Perturbations

Localized U(1) star perturbations on noncommutative planes approach the full gauge-coupled limit as the cutoff radius tends to infinity.

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We construct a spectral-triple framework for a noncommutative planar system associated with a fixed nondegenerate irreducible unitary sector of the kinematical symmetry group $G_{\mathrm{NC}}$, labelled by central parameters $(\hbar_0,\vartheta_0, B_0)$ with $\hbar_0,\vartheta_0, B_0\neq 0$ and $\hbar_0 - \vartheta_0 B_0\neq 0$. For the corresponding two-parameter family $(r,s)$ of unitarily equivalent concrete realizations, we construct even spectral triples whose Dirac operators are isospectral and have compact resolvent despite the non-unital and noncompact setting. Passing to the Moyal-side description, a linear Darboux normalization and the Stone-von Neumann theorem identify the represented smooth operator algebra with the effective Moyal-side Frechet *-algebra at $\vartheta_{\mathrm{eff}} =\vartheta_0/(1 -\vartheta_0 B_0/\hbar_0)$. For each $\varrho$, this yields locally compact non-unital base spectral triples over the involutive Moyal algebra $\mathcal{A}_{\vartheta_{\mathrm{eff}},\varrho}$, with $(r,s)$ as kinematical presentation parameters and $\varrho$ as an independent star-gauge parameter. To incorporate an external $U(1)_\star$ gauge field, we replace the linear gauge potentials by smooth cutoff localizations; the resulting bounded self-adjoint perturbations define, for every $R > 0$, locally compact non-unital spectral triples. Finally, as $R\rightarrow\infty$, we prove strong resolvent convergence to a self-adjoint limiting operator, the closure of the formal minimally coupled operator. Thus the finite-cutoff spectral triples approximate, at the level of spectral triples, the limiting minimally coupled Dirac operator over a fixed nondegenerate $G_{\mathrm{NC}}$-background.
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math-ph 2026-05-12 2 theorems

Boson scalar product yields BUC plane partition count

Generalized i-boson model and boxed BUC plane partitions

The generating function factors as a product of Schur Q-functions and is also recorded in the double scaling limit.

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This paper is devoted to investigating the relation between the generalized i-boson model and boxed BUC plane partitions. The representation of the generalized i-boson algebra and the actions of the monodromy matrix operators on basis vectors have been studied. We also consider the actions of neutral fermion vertex operators on state vectors in terms of the neutral fermionic Fock space. With the help of the scalar product of the generalized i-boson model, the generating function for boxed BUC plane partitions is derived which can be represented as the products of Schur Q-functions. Moreover, the generating function for BUC plane partitions with the double scaling limit is presented.
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math-ph 2026-05-11 Recognition

Two parameters in a recursion induce bound states in free-particle systems

Two-parameter classes of exactly solvable quantum systems

Orthogonal polynomials with tunable initial values determine spectra and allow numerical construction of new solvable quantum potentials.

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We introduce two-parameter classes of exactly-solvable novel systems whose Hamiltonian operators could be represented by tridiagonal symmetric matrices in some orthonormal basis set. The associated wavefunction is written as point-wise convergent series in the basis elements. The expansion coefficients of the series are orthogonal polynomials in the energy that satisfy the resulting three-term recursion relation starting with two-parameter initial values. These polynomials contain all physical information about the system and they depend on the values of the two parameters. However, we could not write down the associated two-parameter potential function analytically but could realize them numerically for a given set of physical parameters. We give several illustrative examples of these systems with continuous and/or discrete energy spectra. Moreover, a curious phenomenon is observed where bound states and/or resonances are induced in a system with pure continuous spectrum (e.g., a free particle) if the two parameters in the initial values exceed certain critical limits.
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math-ph 2026-05-11 2 theorems

2-cocycles classify symmetry actions in hidden quantum Markov models

Cocycle Actions on Hidden Quantum Markov Models: Symmetry Protection and Topological Order

Projective hidden actions yield G-invariant states that encode SPT order, as shown for the AKLT chain with a Markovian virtual description.

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We develop a symmetry action framework for hidden quantum Markov models (HQMMs) tailored to one-dimensional quantum spin systems and symmetry-protected topological (SPT) phases. In our setting, a symmetry group $G$ acts projectively on the hidden (virtual) degrees of freedom and linearly on the physical observation space, yielding a global HQMM state that is invariant under the combined action of $G$ for both conventional and causal (input--output) structures. We show that such symmetry actions are naturally classified by a group-cohomology $2$-cocycle $[\omega] \in H^{2}(G,\mathrm{U}(1))$, in direct analogy with the standard cohomological classification of one-dimensional bosonic SPT phases via projective edge representations. As an explicit example, we apply this construction to the Affleck--Kennedy--Lieb--Tasaki (AKLT) chain, where the hidden layer carries a nontrivial class $[\omega] \in H^{2}(\mathrm{SO}(3),\mathrm{U}(1))$ encoding its SPT order. In this case the HQMM formalism reproduces the known SPT properties of the AKLT state while providing a stochastic, Markovian description of the underlying virtual dynamics. Our results establish HQMMs as a natural bridge between quantum stochastic processes, tensor-network descriptions of many-body systems, and symmetry-protected topological order.
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math-ph 2026-05-11 Recognition

Global bundle replaces local displacement gradient for phonons

A Bundle-Theoretic Formulation of Phonons in Crystalline Phases

After fixing orientations via frame reduction, translations live on a torus bundle whose flat connection yields a covariant differential equ

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Phonons are usually introduced by choosing a local displacement field. This paper keeps that local description, but identifies the global geometric object represented by it. The aim is not to change the local acoustic equations, but to describe the global configuration space of the translational order parameter on a fixed crystallographic background and to give a globally defined replacement for the displacement gradient. After the orientational part of the crystalline order has been fixed by a reduction of the orthonormal frame bundle to a discrete point group, the translational order parameter is described as a section of an associated torus bundle. In a symmorphic crystal the point group acts on the translation torus linearly, whereas in a nonsymmorphic crystal the action is affine and records the extension class of the crystallographic group. Relative to the fixed point-group bundle, the discreteness of the structure group gives a canonical flat Ehresmann connection on the associated torus bundle. The corresponding covariant differential of the translational field is a globally defined object which locally coincides with the ordinary displacement gradient. This covariant differential is then used to formulate the phonon sector as a first-order Lagrangian field theory. When the flat torus holonomy fixes an equilibrium point, linearization about the corresponding covariantly constant section gives the usual local displacement field. For derivative-only quadratic elastic Lagrangians satisfying the standard objectivity condition, the theory reduces locally to linear elasticity and to the standard acoustic phonon spectrum. If such a global equilibrium section does not exist, the same linear theory is understood locally on defect-free simply connected patches.
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math-ph 2026-05-11 2 theorems

Stats on surfaces parameterized by Abelian and cubic differentials

On Conservative Statistical Riemann Surfaces

The moduli space of normalized conservative statistical structures is a vector bundle over Teichmüller space for genus at least 2.

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We establish a correspondence between information geometry and gauge theory. First, we define an important class of statistical manifolds, that is normalized and satisfies a conservation field equation. Second, we prove that for a conservative statistical structure on an orientable surface, the Chebyshev 1-form is constrained to be harmonic, and the traceless part of the Amari--Chentsov tensor descends to a holomorphic cubic differential. Then, we demonstrate that normalized conservative statistical structures are geometrically generated by solutions to the scalar Tzitz\'eica equation on Higgs bundles with general linear holonomy, generalizing the Labourie-Loftin correspondence. Finally, we prove that the moduli space of normalized conservative statistical structures on a closed orientable surface of genus at least 2 is completely parameterized by a holomorphic vector bundle over the Teichm\"uller space, consisting of Abelian differentials and cubic differentials.
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math-ph 2026-05-11 2 theorems

Low-activity polymer bound tames finite-temperature homological codes

An exact spacetime polymer gas for finite-temperature mathbb Z_N homological quantum code

Exact mapping to electric and magnetic defect polymers gives uniform partition control and exponential suppression of nontrivial cycles.

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We study finite-temperature $P$-form $\mathbb Z_N$ homological codes via an exact finite-Trotter quantum-to-classical map to a $(d+1)$-dimensional spacetime model with electric and magnetic topological background charges. The resulting background-resolved partition functions admit an exact reformulation in terms of closed magnetic and electric defect polymers, with opposite-species interactions governed by linking phases. By bounding this complex polymer gas by positive same-species hard-core majorant gases, we obtain an explicit low-activity criterion under which all background-dependent partition functions are uniformly controlled and homologically nontrivial polymers are exponentially suppressed on the scale of the spacetime systole. We also derive an exact higher-form Kramers-Wannier duality exchanging electric and magnetic backgrounds, Wilson and 't Hooft operators, and $P$-form and $(d-P)$-form theories. Finally, for prime $N$, we identify an exact source-free gauge-theory specialization coupled to the plaquette random-cluster model, which imports sharp phase-transition results on special geometries into the spacetime framework.
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math-ph 2026-05-11 2 theorems

Hyperbolic elements decide conformal relative equilibria

Scaling Symmetries and Conformal Relative Equilibria on Poisson Manifolds, with Applications to Lie--Poisson Systems

This algebraic test classifies every three-dimensional case and shows why the equilibria appear on so(2,1)* but are blocked for the free-rig

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We investigate conformal relative equilibria for Hamiltonian systems on exact Poisson manifolds equipped with scaling symmetries. By introducing conformally Poisson actions and conformal momentum maps, we characterize these equilibria through an augmented Hamiltonian formulation; in the nondegenerate case, this recovers the conditions recently developed for the exact symplectic case. Specializing to Lie--Poisson manifolds, where the natural scaling action canonically provides an exact Poisson structure on the dual of any finite-dimensional Lie algebra, we establish a purely algebraic criterion: a homogeneous Hamiltonian system admits a nontrivial conformal relative equilibrium if and only if the underlying Lie algebra contains a hyperbolic element. This yields a complete classification in dimension three via the Bianchi classification. As a prominent application, we show that nontrivial conformal relative equilibria emerge in the dynamics on $\mathfrak{so}(2,1)^*$, but are strictly obstructed for the classical free rigid body on $\mathfrak{so}(3)^*$.
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math-ph 2026-05-11 2 theorems

Thimble crossings match alien jumps in three integrals

Picard-Lefschetz theory and alien calculus: a case study

Explicit calculations for Airy, Bessel and Gamma models confirm that Picard-Lefschetz wall-crossing reproduces the Stokes data of resurgence

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We compare Picard--Lefschetz theory and resurgence in three basic one-dimensional exponential integrals: the Airy model, the Bessel model, and the Gamma model. On the Picard--Lefschetz side, we describe the Lefschetz thimbles and compute the connecting trajectories between critical points appearing at Stokes phases. On the resurgent side, we analyze the Borel singularities of the saddle expansions and use alien operators to recover the same Stokes coefficients. These examples serve as explicit finite-dimensional test cases for the dictionary between thimble wall-crossing and alien calculus.
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math-ph 2026-05-11 Recognition

Relative entropy bounds N-body states to Hartree mean field

Quantum Relative Entropy and the Mean-Field Limit

A stability estimate controls the distance to tensorized Hartree solutions uniformly in Planck constant and extends to open Lindblad systems

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We develop a quantum relative entropy method for the mean-field limit of quantum many-body systems. For closed systems governed by the von Neumann equation, we prove a quantitative stability estimate between the $N$-body density matrix and the tensorized solution of the Hartree equation. The argument is based on an entropy production identity, a cancellation mechanism for the centered two-body fluctuation, and a combinatorial estimate controlling the remaining mixed moments. As a consequence, we obtain propagation of chaos in trace norm for fixed marginals. We further combine the entropy estimate with known semiclassical Wasserstein bounds to derive a convergence estimate that is uniform in the Planck constant in an appropriate joint mean-field and semiclassical regime. Finally, we extend the method to finite-dimensional open quantum systems governed by Lindblad dynamics. In this setting, we establish an analogous relative entropy estimate for general bounded two-body interactions, where the mean-field potential is defined through partial trace. This shows that the entropy method does not rely on any special tensor-product decomposition of the interaction.
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math-ph 2026-05-11 1 theorem

Strong-coupling limit produces effective model for periodic band inversion

A mathematical study of periodic band inversion

Cosine-potential analysis yields gap closings, persistent Dirac cones, and Chern numbers for photon-coupled electrons.

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We give a mathematical analysis of the periodic band inversion phenomenon observed by Tan--Devakul for an electron in a two-dimensional periodic potential coupled to a circularly polarized photon cavity mode. In the strong-coupling limit, we derive an effective Bloch Hamiltonian and prove convergence of the low-lying bands. For a cosine potential, we explain the periodic closing and reopening of the first spectral gap, prove the existence and generic persistence of Dirac cones at the gap-closing points, and compute the Chern numbers associated to isolated band clusters. We also show that higher isolated band clusters cannot persist in the small-coupling regime. Finally, we resolve an apparent sign discrepancy between Berry curvature computations and Chern numbers by tracking the descent from the covering space to the Brillouin torus.
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math-ph 2026-05-11 2 theorems

Decay bounds quantify energy spread in half-line SSH model

Dispersive decay bounds for the SSH model on the half-line

Oscillatory integrals control boundary singularities and yield explicit parameter dependence in the rates.

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We study the Schr\"odinger flow for the SSH model, a class of self-adjoint discrete dimer lattice Hamiltonians on the half-line. Using oscillatory integral techniques, we prove dispersive time-decay estimates, which quantify the spreading of energy throughout the lattice for a localized initial condition. Furthermore, we determine precise dependence of the constants in the decay rates on the parameters of the Hamiltonian. The analysis is complicated by the fact that as a consequence of the boundary condition, the expression for the propagator contains oscillatory integrals with nonintegrable singularities.
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math-ph 2026-05-11 Recognition

Hamiltonian formulation derived for supersymmetric KdV equation

Hamiltonian formulation of the supersymmetric KdV equation

Dirac-Bergmann treatment of the a=2 degenerate Lagrangian produces a nonlocal density whose equations recover the component system.

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We studied the constrained Hamiltonian formulation of a supersymmetric Korteweg-de Vries (KdV) equation, which is observed to be a constrained system similar to its classical version. We found a nontrivial Lagrangian description, where we select $a=2$ for the free parameter $a$ in the supersymmetric extension. The corresponding degenerate Lagrangian requires an exclusive consideration and the utilization of the Dirac-Bergmann algorithm. We explicitly determined the full set of primary and secondary constraints and constructed the total Hamiltonian governing the dynamics of the system. In this analysis, in addition to a nontrivial constraint involving the fermionic fields, the consistency conditions give rise to a nonlocal contribution to the Hamiltonian density. This highlights a distinctive feature of this supersymmetric extension. We showed that the resulting Hamilton equations of motion reproduce the supersymmetric KdV system in the component form. Finally, we derived a compact superspace representation of the Hamiltonian and demonstrated its consistency with the component-level formulation.
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math-ph 2026-05-11 2 theorems

New superintegrable families for two spin particles classified

Superintegrability in the interaction of two particles with spin: First-order pseudo-scalar integrals of motion

First-order pseudo-scalar integrals complete the classification of rotationally invariant two-particle systems with spin.

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In recent work, we initiated a research program aimed at the systematic investigation of quantum superintegrable systems describing the interaction of two non-relativistic spin-$1/2$ particles in three-dimensional Euclidean space. In that study, we classified all such superintegrable systems admitting additional first-order scalar integrals of motion. In the present paper, we continue this program by focusing on systems that admit additional pseudo-scalar integrals of motion. Starting from the most general rotationally invariant Hamiltonian for two interacting spin-$1/2$ particles, we construct the most general first-order pseudo-scalar operator in the form of a matrix polynomial in the momenta. Imposing the commutativity of this operator with the Hamiltonian leads to a system of determining equations. By solving these equations, we obtain a complete classification of such superintegrable systems and determine the corresponding pseudo-scalar integrals of motion. The resulting classification provides new families of superintegrable systems with spin-dependent interactions. These systems enrich the class of integrable models relevant to nucleon--nucleon interactions and contribute to the broader program of classifying superintegrable quantum systems with spin. For selected cases, we further construct the associated polynomial symmetry algebras generated by the integrals of motion, providing additional insight into the algebraic structure of the systems.
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math-ph 2026-05-11 Recognition

Energy-truncated Hamiltonians stable uniformly in volume

Volume-Independent Spectral Stability of Energy-Truncated Effective Hamiltonians in Quantum Spin Systems

For finite-range quantum spins, low-energy subspaces leak only exponentially small amounts into high-energy sectors even in infinite volume.

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We prove a volume-uniform effective-Hamiltonian theorem for bounded finite-range quantum spin systems on possibly infinite lattices. For any finite target region, we construct an energy-truncated Hamiltonian and prove a volume-uniform spectral-overlap bound controlling the leakage of its low-energy spectral subspace into the high-energy spectral subspace of the original Hamiltonian. The bound may contain non-exponential spectral-window terms, but its cutoff-dependent remainder decays exponentially in the cutoff. In finite volume, this yields stability of low-lying eigenvalues, with eigenvalue errors controlled by the exponentially small cutoff-dependent remainder. In infinite volume, we prove the corresponding spectral-overlap estimate in the GNS representation of an infinite-volume ground state. Thus, for bounded finite-range interactions, we extend and strengthen the effective-Hamiltonian mechanism of Arad, Kuwahara, and Landau by replacing the finite-volume operator-norm formulation with a volume-uniform spectral-overlap formulation applicable in the thermodynamic limit.
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math-ph 2026-05-08 2 theorems

Lindblad dynamics converge with 1/N relative entropy bounds

Quantitative propagation of chaos for Lindblad dynamics

N-particle open quantum states approach their nonlinear mean-field limit at explicit rate 1/N

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We consider an open quantum system governed $N$-body Lindblad equation and study mean-field limits in this setting. We prove that the $N$-particle dynamics converges, in the sense of quantum relative entropy, to the tensorized solution of the limiting nonlinear equation. More precisely, we establish explicit bounds of order $1/N$ on the relative entropy between the $N$-particle density operator and the corresponding product state, thereby providing a quantitative propagation of chaos.
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math-ph 2026-05-08 2 theorems

Local cutoff recovers Lee-Huang-Yang bound for dilute Bose gas energy

A Note on the Construction of Trial States for the Dilute Bose Gas

A restriction on local particle numbers in trial wave functions bounds the ground-state energy from above by the full Lee-Huang-Yang term.

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We review how the local particle number cutoff introduced in [11] is used to build trial states for the dilute Bose gas that capture the substantial correlation structure of the ground state in the thermodynamic limit. In particular, we provide a simplified derivation of the Lee-Huang-Yang correction as an upper bound for the ground state energy.
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math-ph 2026-05-08

Conditions fix when zero-energy states have finite moments

Eigenstates with Infinite Position Moments

Schrödinger operators possess bounded k-th position moments for their threshold eigenstates exactly when the stated criteria are met.

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We prove necessary and sufficient conditions for the Schr\"odinger operators to have zero-energy bound states at the threshold of the essential spectrum such that they have bounded $k$-th moment. This result is the extension of the results published in D. Hundertmark, M. Jex, and M. Lange [Forum Mathematics, Sigma 11(2023)].
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math-ph 2026-05-08

Self-similar fronts drive dynamical cooling in 2D nonlinear waves

Dynamical cooling driven by self-similar fronts in the 2D nonlinear Schr\"odinger model

Stretching the quasi-thermal core pushes the system toward the vanishing-temperature equilibrium, analogous to a classical wave ultraviolet

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We analyze the dynamics towards partial thermalization and subsequent cooling in the defocusing two-dimensional nonlinear Schr\"odinger model, using direct simulations and insights from the wave-kinetic equations (WKE) and a fourth-order differential approximation model (DAM). We show that the evolving WKE spectrum exhibits two distinct similarity ranges--the quasi-thermal core and the ultraviolet tail--whereas in the DAM, an additional range of infrared self-similarity appears. By stretching the quasi-thermal region, the self-similar fronts drive an effective dynamical cooling process towards the formal but ill-defined equilibrium state at vanishing temperature--analogous to an ultraviolet catastrophe in a system of classical waves.
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math-ph 2026-05-08

Relativistic Pauli operators converge to non-relativistic limit as c to infinity

Non-relativistic limit of generalized relativistic Pauli operators by Feynman-Kac formulae

Semigroups converge strongly to a scaled Pauli Hamiltonian under a parameter constraint, via path integrals.

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The non-relativistic limit of a generalized relativistic Pauli operator\[H_c^{S,\alpha}=\left(2c^{\beta}\bigl(\sigma\cdot(-i\nabla-a)\bigr)^2+(mc^\gamma)^{2/\alpha}\right)^{\alpha/2}-mc^\gamma+V\]on $L^2(\mathbb{R}^3;\mathbb{C}^2)$ is investigated under the constraint$2\alpha=\gamma\beta+\gamma^2$.This operator generalizes the relativistic Pauli operator within the framework of Bernstein functions.The associated heat semigroup $e^{-tH_c^{S,\alpha}}$ admits a Feynman--Kac representation involving Brownian motion, a subordinator, and a Poisson process.Using this representation, we prove that the semigroup $e^{-tH_c^{S,\alpha}}$ converges strongly to $e^{-tH^{S,\alpha}}$ as $c\to\infty$, where the limiting generator is given by\[H^{S,\alpha}=\frac{\alpha}{2m^{\frac{2}{\alpha}-1}}\bigl(\sigma\cdot(-i\nabla-a)\bigr)^2+V.\]The non-relativistic limit of a generalized relativistic Schr\"odinger operator is also investigated.
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math-ph 2026-05-08

Voros periods expand Heun accessory parameters to match conformal blocks

Accessory Parameter of Confluent Heun Equations, Voros Periods and classical irregular conformal blocks

A cycle selection rule on the spectral curve ensures the series match classical blocks for both regular and irregular singularities.

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For the Heun differential equation and all of its confluent equations, we derive formal series expansions of the accessory parameters using the Voros periods. We then compare these expansions with the classical conformal blocks recently obtained by Bonelli--Shchechkin--Tanzini, and examine the Zamolodchikov-type conjecture expected to hold between them, allowing for irregular singularities. In particular, as an extension of the previous works of Mironov--Morozov, Piatek--Pietrykowski and Lisovyy--Naidiuk, we provide a detailed prescription for choosing cycles on the spectral curve that yield the Voros period which corresponds to the classical (regular or irregular) conformal blocks through the accessory parameter.
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math-ph 2026-05-07 Recognition

Local vector bundles generate free Poisson 2-algebra bundles

Equivariant Poisson 2-Algebra Bundles over Configuration Spaces

Skew-symmetric maps on V induce compatible brackets on the free commutative 2-algebra S^⊠(S^⊗(V)) over configuration spaces.

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We study equivariant vector bundles over configuration spaces with diagonals included, viewed as orbifold quotients $M^n/\mathfrak{S}_n$ by permutation groups. Working in the equivalent language of equivariant vector bundles, we construct an induced-equivariance functor and prove its adjunction with restriction. We then define Hadamard and Cauchy tensor products and show that they form a symmetric $2$-monoidal structure. We construct the corresponding tensor and symmetric algebra bundles and prove that, for a local vector bundle $V \rightarrow M$, the bundle $\mathbf{S}^{\boxtimes} \big( \mathbf{S}^{\otimes}(V) \big)$ is the free commutative $2$-algebra generated by $V$. Finally, we show that any skew-symmetric bundle map $k : V \boxtimes V \rightarrow \mathbf{I}_{\otimes}$ induces a compatible Poisson bracket on this $2$-algebra bundle.
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math-ph 2026-05-07 2 theorems

Local vector bundles generate free commutative 2-algebra bundles

Equivariant Poisson 2-Algebra Bundles over Configuration Spaces

Skew-symmetric maps from pairs of sections induce compatible Poisson brackets on the resulting algebra bundle over configuration spaces.

abstract click to expand
We study equivariant vector bundles over configuration spaces with diagonals included, viewed as orbifold quotients $M^n/\mathfrak{S}_n$ by permutation groups. Working in the equivalent language of equivariant vector bundles, we construct an induced-equivariance functor and prove its adjunction with restriction. We then define Hadamard and Cauchy tensor products and show that they form a symmetric $2$-monoidal structure. We construct the corresponding tensor and symmetric algebra bundles and prove that, for a local vector bundle $V \rightarrow M$, the bundle $\mathbf{S}^{\boxtimes} \big( \mathbf{S}^{\otimes}(V) \big)$ is the free commutative $2$-algebra generated by $V$. Finally, we show that any skew-symmetric bundle map $k : V \boxtimes V \rightarrow \mathbf{I}_{\otimes}$ induces a compatible Poisson bracket on this $2$-algebra bundle.
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math-ph 2026-05-07

Equivariant bundles yield free commutative 2-algebras

Equivariant Poisson 2-Algebra Bundles over Configuration Spaces

A skew-symmetric map on the base bundle induces a compatible Poisson bracket on the resulting structure over configuration spaces.

abstract click to expand
We study equivariant vector bundles over configuration spaces with diagonals included, viewed as orbifold quotients $M^n/\mathfrak{S}_n$ by permutation groups. Working in the equivalent language of equivariant vector bundles, we construct an induced-equivariance functor and prove its adjunction with restriction. We then define Hadamard and Cauchy tensor products and show that they form a symmetric $2$-monoidal structure. We construct the corresponding tensor and symmetric algebra bundles and prove that, for a local vector bundle $V \rightarrow M$, the bundle $\mathbf{S}^{\boxtimes} \big( \mathbf{S}^{\otimes}(V) \big)$ is the free commutative $2$-algebra generated by $V$. Finally, we show that any skew-symmetric bundle map $k : V \boxtimes V \rightarrow \mathbf{I}_{\otimes}$ induces a compatible Poisson bracket on this $2$-algebra bundle.
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math-ph 2026-05-07

Time evolution mirrors RG flow in Gross-Neveu model

Time-Dependent Dynamical Dimensional Transmutation in the SU(2) Gross-Neveu Model with Time-Dependent Interaction Strength

When coupling strength follows renormalization trajectories, the driven model generates a dynamical mass gap and approaches its ultraviolet

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In this work we consider the time-dependent $SU(2)$ Gross-Neveu model, which is a quantum field theory of fermions which interact with each other through spin exchange interaction with time-dependent coupling strength $g(t)$. Using the recently formulated generalized Bethe ansatz framework, we show that the system is integrable provided the time-dependent coupling strength is such that its trajectories in time are exactly same as that of the renormalization group (RG) flow equations corresponding to the static model, where time `$t$' of the time-dependent model is identified with the logarithm of the cutoff `$\ln \Lambda$' of the static model. In the scaling regime $\Lambda\rightarrow\infty$, the above relation between time and the logarithm of the cutoff provides a characteristic time scale $t_0$. We analyze the exact time-dependent wavefunction in the case of coupling strength decreasing with time and show that in the adiabatic regime, which corresponds to $t\sim t_0$ for drive rate $\alpha_0=1$, the system exhibits a time-dependent dynamical dimensional transmutation where a time dependent mass gap is generated, which at time $t=t_0+\Delta t$ is given by $m(\Delta t)=m_0 e^{-\pi\alpha_0\Delta t}$, where $m_0=\Lambda e^{-\pi \alpha_0 t_0}$. Comparing this with the mass gap of the static model, we identify the adiabatic regime of the time-dependent model with the scaling regime of the static model. In the case of very large time scales $t\gg t_0$ for drive rate $\alpha_0$ or for very fast drive rates $\alpha$ such that $\alpha t \gg \alpha_0t_0$, for any $t<L$, we argue that the system is asymptotically free and approaches the $SU(2)_1$ Wess-Zumino-Novikov-Witten (WZNW) model, which corresponds to the UV fixed point of the $SU(2)$ Gross-Neveu model. Hence we establish that progression of time in the time-dependent model is equivalent to RG flow in the corresponding static model.
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math-ph 2026-05-07

CFT differential equations recover SLE percolation densities

Anchored random clusters and SLE excursions

Expressing observables as bulk-boundary correlations with degenerate operators produces exact formulas for passage probabilities and cluster

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We provide a pedagogical review of CFT techniques to compute certain Schramm-Loewner Evolution (SLE) observables in the upper half-plane. The approach relies on the ability to express the observables as bulk-boundary correlation functions that involve degenerate boundary operators and, therefore, obey certain differential equations. In particular, we recover Schramm's left-passage probability for SLE, the SLE Green's functions, and the generalized densities of ``anchored'' critical percolation clusters first obtained by Kleban, Simmons, and Ziff. We also obtain new formulas corresponding to the densities of pivotal points between critical Fortuin-Kasteleyn (FK) clusters.
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math-ph 2026-05-06

Padé approximants extend gravity models inside Brillouin sphere

Pade Approximants for Geodesy

Rational function approximations allow analytic continuation of potentials where spherical harmonics diverge, for smooth synthetic planets.

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In this note we analyze the use of Pad\'e approximants for downward continuation beyond the radius of convergence of spherical harmonic expansions (SHEs), and for identifying the complex singularities of the gravitational potential. SHEs are, in essence, expansions in 1/r, i.e., expansions about the point at infinity. Their domain of convergence is generically the exterior of the Brillouin sphere. However, for synthetic models with analytic topography and density the region of convergence may be larger, with the deviation decreasing as the structural complexity of the planet increases.
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math-ph 2026-05-06

Borel resummation yields closed forms for two Laplacian determinants

Two Regularized Determinants of Laplacian through Resurgence theory

The formulas recover the Poisson summation on the circle and Selberg trace formula on higher-genus surfaces via singularity contributions in

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We study two types of regularizations of the determinant of Laplacian on Riemann manifold from the viewpoint of resurgence theory. One is the formal logarithmic derivative of the determinant, and the other is its exponential deformation. Under appropriate conditions, the close formulas for both regularized determinant are established through Borel-Laplace resummation which takes into account the contribution of the singularities along the analytic continuation of Theta series $\hat{\Theta}_{D_X}$. The series resembles the trace of the heat kernel, but is defined via the spectrum of the square-root of the Laplacian. As applications, we revisit the well known formal logarithmic derivative of determinant on $S^1$ and compact Riemann surface with higher genus ($\geq2$) corresponding to the Poisson summation formula and Selberg trace formula respectively. Furthermore, the 1-Gevrey asymptotic behavior of the exponential deformation regularization at infinity is considered whose coefficients are determined by the trace of the heat kernel. In the end, we establish the relationship between the two regularized determinants. In fact, they have the same derivatives when the deformation parameter tends to $0$ in exponentially deformed regularization.
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math-ph 2026-05-05

Holomorphic functions on infinite-dimensional domains form closed algebras

On Algebras of Functions over Infinite Dimensions

Kernel from Gaussian covariance and holomorphic Lambda yields reproducing kernel Hilbert algebras with bounded twisted creation and annihil

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We introduce a family of reproducing kernel Hilbert spaces $\mathcal A_\Lambda$ of holomorphic functions defined on an infinite--dimensional domain in a separable Hilbert space, $\mathbb{H}$. The reproducing kernel of $\mathcal A_\Lambda$ is constructed using the covariance operator associated with a Gaussian measure on $\mathbb{H}$, along with a holomorphic function $\Lambda$ on the unit disk. Under certain conditions on the kernel, $\mathcal A_\Lambda$ is closed under pointwise multiplication, giving it the structure of a reproducing kernel Hilbert algebra (RKHA). We also study twisted canonical commutation relations on these RKHAs, where the creation and annihilation operators are both bounded.
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math-ph 2026-05-05 3 theorems

Kontsevich model explicitly matches r-spin geometry

Generalized Kontsevich model, topological recursion, and r-spin theory

KP integrability and string equation prove links to topological recursion and moduli space geometry for polynomial and deformed cases.

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By employing polynomial-reduced KP integrability, combined with the string equation, this work establishes explicit relationships between the generalized Kontsevich model, the topological recursion of the spectral curve, and the geometry of moduli spaces of $r$-spin curves. For the generalized Kontsevich model with a polynomial potential, we derive an explicit formulation and provide a proof of these widely expected correspondences. Furthermore, the method is extended to the cases with admissible deformed potentials, where the corresponding geometric theory is a deformed version of $r$-spin theory.
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math-ph 2026-05-05 3 theorems

Fifth-order KP equations have no independent second-order multipliers

Low-Order Conservation Law Multipliers for a Generalized Fifth-Order KP Family

All multipliers of order two or less reduce to first order or below in generic regimes of the generalized family.

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We study local conservation law multipliers for a generalized fifth-order Kadomtsev--Petviashvili family whose one-dimensional reductions include the Lax, Sawada--Kotera, and Kaup--Kupershmidt equations. Using the direct multiplier method, we classify zeroth-order multipliers that are independent of the dependent variable within a natural polynomial subclass and construct representative conserved vectors. We then prove that every multiplier of differential order at most two is necessarily of differential order at most one. An unrestricted first-order classification is obtained when the coefficient of the cubic derivative nonlinearity is nonzero, and the same reduction is established on a generic algebraic sub-branch of the complementary case. In these regimes, all first-order multipliers reduce to the zeroth-order family. A finite list of exceptional branches remains open. The results identify the structural sources responsible for the low-order rigidity of the multiplier problem in the generic regimes treated here.
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math-ph 2026-05-05 3 theorems

Pauli-Fierz energy at zero momentum scales as Λ^{3/2}

On the Ultraviolet Problem for the Ground State Energy of the Translation-Invariant Pauli--Fierz Model at Zero Total Momentum

A convexified variational functional yields an asymptotic upper bound showing the ultraviolet divergence grows like the cutoff to the three-

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We study the ground state energy of the Pauli--Fierz model in the absence of external potentials. We consider the fiber decomposition of the Pauli--Fierz operator with respect to the spectral values, $p$, of the total momentum operator and focus on the case $p = 0$. The corresponding variational problem is analyzed to estimate the dependence of the ground state energy on the ultraviolet cutoff $\Lambda$. We employ a Bogoliubov--Hartree--Fock approximation using pure, quasifree states generated by Bogolubov transformations (parametrized by a positive Hilbert--Schmidt operator $z$) and Weyl transformations (parametrized by a vector $\eta$) applied to the vacuum. We prove that the resulting energy functional is not a convex function of $\eta$ and $z$. We identify the non-convex term and remove it from the energy functional. The modified functional retains the full interaction term and is shown to be strictly convex. We study the ground state of the modified functional and prove the existence of a unique minimizer. Furthermore, we construct an explicit partial minimizer (with respect to $\eta$, for fixed $z$), which allows us to eliminate $z$ and reduce the minimization problem to a single variable, $\eta$. Finally, we estimate the minimum of the modified energy functional in terms of the ultraviolet cutoff $\Lambda$ and demonstrate that, up to a constant factor, it grows asymptotically as $\Lambda^{3/2}$, as $\Lambda \to \infty$.
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math-ph 2026-05-04 3 theorems

Lie group fiber bundles are generalized principal bundles

A constructive approach to generalized principal connections

Connections on them associate only to Lie group fiber bundle connections and reduce to standard principal connections.

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We address the recently introduced notions of generalized principal bundle and generalized principal connection by keeping track of global geometric properties through local coordinate transformation laws. This approach leads us to introduce generalized principal bundle coordinates and to find their transformation laws. Besides, we show that any Lie group fiber bundle (and hence, in particular, any vector bundle) is a generalized principal bundle and we give a proof of the fact that any Lie group fiber bundle with connected typical fiber is an associated bundle to a suitable principal bundle. Moreover, we present a direct way to characterize Lie group fiber bundle connections and generalized principal connections in terms of horizontal lifts and of local conditions. Finally, we recover in our setting some already known results, including that generalized principal connections are associated only to Lie group fiber bundle connections and that they reduce to usual principal connections on standard principal bundles. Our results are needed in order to understand how generalized principal connections might fit in the fiber bundle treatment of classical field theories, aiming towards a notion of generalized gauge theory.
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math-ph 2026-05-04

Tensorial free cumulants defined for all orders via group averages

Properties of tensorial free cumulants

Linking two approaches yields formulas for products and explicit non-trivial examples from Gaussians with non-trivial covariances.

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In the past two years, several points of view have been proposed to address the question of the generalization of the theory of free probability to random tensors with different invariances, and it is unclear at this point whether they lead to the same notions of tensorial free cumulants and freeness. One way to approach this problem, developed by Collins, Gurau and the second named author for local unitary invariant random tensors, relies on finite size quantities involving averages over the invariance group, and whose asymptotics naturally possess the properties expected for tensorial generalizations of free cumulants of arbitrary orders. At this point, this approach has only been carried out for certain distributions, and for a subset of the moments that define such theories, and a more systematic and exhaustive study is lacking. This is the program initiated in this paper: we link this approach to the one proposed by Nechita and Park; extend a number of their results as well as those of the aforementioned paper to arbitrary orders of fluctuations, thereby generalizing higher order free cumulants; push further the study of distributions with larger invariance groups; detail the link with the asymptotics of the free-energies of the tensor HCIZ and BGW integrals; and provide formulae for tensorial free cumulants of products of tensors. Another important question is that of the definition of concrete distributions whose tensorial free-cumulants take non-trivial values. We compute the tensorial free cumulants for Gaussian random tensors with non-trivial covariances, and show that they provide such examples.
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math-ph 2026-05-04 3 theorems

Ladder operators solve variable-mass quantum Hamiltonians

A position dependent mass Hamiltonian and abstract ladder operators

Factorizable cases yield eigenvalues and bi-coherent states via pseudo-bosons without requiring self-adjointness

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We consider the Hamiltonian $H$ of a particle in one dimension with a position dependent mass for which we apply the recent strategy of the so-called {\em abstract ladder operators}, in the attempt to find its eigenvalues and eigenvectors. We don't assume that $H$ is self-adjoint, while we focus on the case of a factorizable operator. We show then that pseudo-bosonic operators play a relevant role in this analysis, and we construct bi-coherent states attached to these operators. Explicit examples are discussed.
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math-ph 2026-05-04 2 theorems

p-adic SO(3) Haar measure factors across three nautical angles

The Haar measure of the p-adic rotation group textrm{SO}(3)_p via nautical angles

Transporting the quaternion group measure through the isomorphism and p-adic Jacobian produces an explicit product density for the invariant

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We study the explicit construction of the Haar measure on the compact $p$-adic rotation group $\textrm{SO}(3)_p$ by nautical (Cardano) parametrization. Exploiting its topological group isomorphism with $\mathbb{H}_p^\times/\mathbb{Q}_p^\times$ of $p$-adic quaternions modulo scalars, we derive the corresponding change of variables formulas and compute the associated Jacobian in the $p$-adic setting, which we combine with the known Haar measure on the multiplicative group of $p$-adic quaternions $\mathbb{H}_p^\times$. This yields an explicit formula for the normalized Haar measure on $\textrm{SO}(3)_p$ in nautical coordinates, with a factorized density in the three angles. Our construction provides a concrete tool suited for applications of non-Archimedean models where an explicit angular description of invariant integration is required.
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math-ph 2026-05-04

Reflection symmetry on twisted Dirac requires 2A integer

Reflection Symmetry, APS Boundary Conditions, and Equivariant Spectral Flow on a Warped Cylinder

The condition enables mode pairing and reduces varying-holonomy spectral flow to mod-two parity of crossings.

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We study reflection symmetry and Atiyah-Patodi-Singer (APS) boundary conditions for twisted Dirac operators on a finite warped cylinder. For a complex line twist with holonomy parameter $A$, we show that the reflection lifts to a unitary symmetry of the twisted Dirac setting if and only if $2A\in\mathbb Z$. In the resulting reflection-compatible fixed-holonomy case, reflection pairs opposite shifted angular modes, and the paired APS blocks are unitarily equivalent. The reflection trace on the APS harmonic space localizes to the unique self-paired zero-mode sector. We then turn to parameter-dependent versions of the model. For fixed gauge-trivial holonomy, the family remains pointwise \(O(2)\)-equivariant, and its spectral flow admits an \(RO(O(2))\)-valued decomposition. For genuinely varying holonomy, pointwise \(O(2)\)-equivariance is lost along the path. The representation-ring-valued invariant is then replaced by a residual sign-level invariant: the mod-two parity of the APS crossing events.
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math-ph 2026-05-04

Anderson model on Bethe lattice has analytic DOS at strong disorder

Strong-disorder expansion of the root-averaged density of states for the Anderson model on the Bethe lattice

Root-averaged density becomes absolutely continuous with a power series in inverse disorder strength inside a scaled energy interval.

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We study the root-averaged density of states for the Anderson model on the Bethe lattice in the strong-disorder regime. Here the density of states means the root-averaged spectral measure, not a finite-volume eigenvalue counting limit. We assume that the single-site distribution has compact support and has a locally analytic density on an interval $I^\sharp$ containing a given interval $I$. Combining the random-walk expansion on the tree with a complex-analytic argument for the single-site Stieltjes transforms, we prove that the scaled averaged diagonal resolvent has a holomorphic continuation to a complex neighborhood of $I$ for all sufficiently large $\lambda$. By the Stieltjes inversion formula, the root-averaged density of states measure is absolutely continuous on the scaled energy window $\lambda I$, and its density is real analytic and has a finite-order strong-disorder expansion there. In the scaled form $E=\lambda\xi$, the leading coefficient is the local density of the single-site distribution. All odd coefficients vanish, and the higher coefficients are finite sums determined by occupation profiles of short closed walks on the tree. For the uniform single-site distribution, we compute the first nonzero correction term explicitly.
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math-ph 2026-05-04

Generalized Fourier transform defined on any Riemannian manifold

Generalized Fourier Transforms for Momentum-Space Construction on Riemannian Manifolds

The transform is an isometric isomorphism diagonalizing the Laplace-Beltrami operator and satisfies a generalized Parseval-Plancherel result

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We extend Fourier analysis to curved spaces by defining a Generalized Fourier Transform (GFT) on any Riemannian manifold $\Sigma$ via spectral decomposition. Under minimal requirements that the transform is an isometric isomorphism and has a kernel diagonalizing the Laplace-Beltrami operator, we prove that the GFT satisfies a generalized Parseval-Plancherel theorem. To resolve the spectral degeneracy that obscures "momentum space" in such settings, we require the degenerate sector to be resolved by a local, symmetry-adapted maximal Abelian commuting set (a fiberwise MASA), constructed from geometric differential operators, most notably from Killing data when such symmetries are available. We provide a constructive algorithm for generating these commuting operators and show that the resulting momentum label spaces $\mathcal{F}$ (discrete, continuous, or mixed) reflect geometric symmetry constraints. We introduce a dual classification: (i) by MASA completeness and Stackel separability, and (ii) by the topology of $\mathcal{F}$. Finally, we distinguish unitary changes induced by true isometries (which preserve the GFT structure) from changes of coordinate-adapted degeneracy resolution/separation schemes, which may induce inequivalent $k$-space labelings (e.g. Cartesian vs spherical constructions in $\mathbb{R}^{3}$) while remaining unitarily equivalent on $\mathcal{L}^{2}\left[\Sigma\right]$. This symmetry-adapted harmonic analysis is intended as a foundation for curved-space mode decompositions; dynamical applications are developed in the subsequent work.
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math-ph 2026-05-04 2 theorems

Generalized Fourier transform defined on any Riemannian manifold

Generalized Fourier Transforms for Momentum-Space Construction on Riemannian Manifolds

Spectral decomposition with symmetry-adapted operators resolves degeneracy and yields a Parseval-Plancherel theorem for curved spaces.

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We extend Fourier analysis to curved spaces by defining a Generalized Fourier Transform (GFT) on any Riemannian manifold $\Sigma$ via spectral decomposition. Under minimal requirements that the transform is an isometric isomorphism and has a kernel diagonalizing the Laplace-Beltrami operator, we prove that the GFT satisfies a generalized Parseval-Plancherel theorem. To resolve the spectral degeneracy that obscures "momentum space" in such settings, we require the degenerate sector to be resolved by a local, symmetry-adapted maximal Abelian commuting set (a fiberwise MASA), constructed from geometric differential operators, most notably from Killing data when such symmetries are available. We provide a constructive algorithm for generating these commuting operators and show that the resulting momentum label spaces $\mathcal{F}$ (discrete, continuous, or mixed) reflect geometric symmetry constraints. We introduce a dual classification: (i) by MASA completeness and Stackel separability, and (ii) by the topology of $\mathcal{F}$. Finally, we distinguish unitary changes induced by true isometries (which preserve the GFT structure) from changes of coordinate-adapted degeneracy resolution/separation schemes, which may induce inequivalent $k$-space labelings (e.g. Cartesian vs spherical constructions in $\mathbb{R}^{3}$) while remaining unitarily equivalent on $\mathcal{L}^{2}\left[\Sigma\right]$. This symmetry-adapted harmonic analysis is intended as a foundation for curved-space mode decompositions; dynamical applications are developed in the subsequent work.
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math-ph 2026-05-04

Twisted orientation maps free phases into the interacting Bott spiral

Unraveling the Bott spiral

The model computes how symmetry-protected phases reduce in dimension on the interacting side and shows why Altland-Zirnbauer classes are not

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We construct and compute a homotopy-theoretic model for the Bott spiral of symmetry-protected topological phases (SPTs) studied by Queiroz--Khalaf--Stern. We model free and interacting fermionic SPTs using K-theory and reflection-positive invertible field theories (IFTs), resp., and define a twisted generalization of the Atiyah--Bott--Shapiro orientation to produce a free-to-interacting map. We also define and compute spiral maps of IFTs to model dimensional reduction in this context, answering a question of Hason--Komargodski--Thorngren. Our analysis highlights two general aspects of homotopical free-to-interacting maps. First, IFTs are more sensitive than K-theory is to the input symmetry data; in particular, the specification of an Altland--Zirnbauer class is insufficient information to define symmetry type for an IFT. Second, the remnant of Bott periodicity on the interacting side relies on an isomorphism of two extraspecial groups of order 32. Our computations use a novel 4-periodic description of a sector of the twisted ko-homology of elementary abelian 2-groups.
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math-ph 2026-05-01

Quantum evolution approximates classical electrodynamics as ħ vanishes

Classical limit of the Pauli-Fierz dynamics

Explicit rates of convergence are derived for the Pauli-Fierz model under the classical limit for select initial states.

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We study the Schr\"odinger evolution generated by the Pauli-Fierz Hamiltonian, a model for nonrelativistic quantum electrodynamics, in the classical limit $\hbar \rightarrow 0$. In this regime, we rigorously derive the Newton-Maxwell equations of classical electrodynamics as effective dynamics approximating the time evolution. Our result complements prior work by an alternative derivation that provides explicit estimates on the rate of convergence, justifying the validity of the approximation for a special class of initial data.
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math-ph 2026-05-01

Dilation models open quantum dynamics via unitary evolution on enlarged space

Quantum Dynamics: A Dilation-Based Approach

Channel curves dilate exactly for analytic cases and approximately for Lipschitz-continuous ones in finite dimensions.

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In the study of open quantum systems, one commonly describes the evolution of a system of interest through reduced dynamics, obtained by treating the environment indirectly rather than as a part of the full model. This thesis presents an expository account of an alternative, dilation-based viewpoint in the finite-dimensional setting, where a family of reduced dynamics is represented through unitary evolution on a larger system consisting of the original system together with an ancillary environment. After reviewing the reduced-dynamics perspective and the language of quantum channels, we formulate finite-dimensional quantum dynamics as channel-valued dynamical curves and use this framework to discuss Stinespring dilations of such curves. We then present exact dilation results for analytic dynamical curves, explain the singular behavior that can arise at t=0, and describe approximation results showing that Lipschitz-continuous dynamical curves admit approximate finite-dimensional Stinespring dilations. The thesis therefore provides a mathematically focused introduction to dilation-based modeling of quantum dynamics and argues that a change of perspective can lead to new ways of formulating problems in the theory of open quantum systems.
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math-ph 2026-05-01

Constraint algorithms reduce singular systems to consistent submanifolds

Constrained Symplectic and Contact Hamiltonian Systems: A Review

Pre-symplectic and pre-contact structures locate the admissible phase-space subsets for well-defined Hamiltonian evolution.

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Singular theories, characterised by the presence of degeneracies in their Lagrangian or Hamiltonian descriptions, require the systematic implementation of constraints in order to obtain well-defined dynamics. While the symplectic framework provides the standard geometrical setting for conservative mechanical systems, those theories which exhibit dissipative effects are most appropriately discussed within the context of contact geometry. In this review, we present the geometrical structure underlying pre-symplectic and pre-contact manifolds, and develop the corresponding constraint algorithms that determine the admissible subset of phase space upon which consistent Hamiltonian evolution exists. We then close the discussion of each of the constraint algorithms with an example.
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math-ph 2026-05-01

Spin-boson model blocks quasiparticle condensation

No-Go Theorem for Quasiparticle BEC in the Spin-Boson Model

A zero-mode term formally suggests BEC but moderate equilibrium states forbid it at finite temperature.

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We analyze the possibility of Bose-Einstein condensation (BEC) at finite temperature in the spin-boson model within the frameworks of functional integral representations and the resolvent algebra. Because a sesquilinear form arising from the zero mode appears, analogous to the case of the free Bose gas, a BEC-type component is also formally present in the spin-boson model. However, according to arxiv:1207.4621, quasiparticles do not undergo BEC, so an argument is needed to exclude this possibility. In particular, for moderate equilibrium states defined by following the formulation of that paper, a no-go theorem for BEC is obtained.
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math-ph 2026-05-01

No-go theorem blocks quasiparticle BEC in spin-boson model

No-Go Theorem for Quasiparticle BEC in the Spin-Boson Model

A formal zero-mode contribution does not produce condensation for moderate equilibrium states.

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We analyze the possibility of Bose-Einstein condensation (BEC) at finite temperature in the spin-boson model within the frameworks of functional integral representations and the resolvent algebra. Because a sesquilinear form arising from the zero mode appears, analogous to the case of the free Bose gas, a BEC-type component is also formally present in the spin-boson model. However, according to arxiv:1207.4621, quasiparticles do not undergo BEC, so an argument is needed to exclude this possibility. In particular, for moderate equilibrium states defined by following the formulation of that paper, a no-go theorem for BEC is obtained.
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math-ph 2026-05-01

Nilpotents collapse hypergeometric functions to polynomials

Hypergeometric Functions of Nilpotent Operators: Functional Collapse and Structural Depth at Exceptional Points

Analytic functions shrink Jordan depths at exceptional points to at most ceil((m+1)/r) where r is the contact order

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We study hypergeometric functions of nilpotent operators in finite-dimensional settings, motivated by the algebraic structure of exceptional points in non-Hermitian quantum mechanics. Our starting point is the following exact result: if N is a nilpotent operator of index m+1 in an associative algebra over C, then every generalized hypergeometric function pFq evaluated at N reduces to a finite polynomial in N of degree at most m, without any analytic convergence requirement. This "functional collapse" is distinct from the classical parameter-termination mechanism and arises purely from the nilpotent structure of the argument. The main result is a "nilpotent depth criterion" (Theorem 2): if the first non-constant coefficient of a formal series F appears in degree r >= 1, then the nilpotent part F(N) - F(0)I has nilpotency index bounded above by ceil((m+1)/r). We apply this criterion to Hamiltonians at exceptional points, where H = lambda I + N with N^{m+1} = 0. Theorem 3 establishes that a function F analytic at lambda reduces the Jordan depth of the exceptional point from m+1 to at most ceil((m+1)/r), where r is the contact order of F at lambda. As consequences: the time evolution operator e^{tH} preserves the full Jordan depth for all t != 0; a function with a zero of order m+1 at lambda annihilates the entire Jordan structure; and the order of the pole of the modified resolvent is reduced from m+1 to at most m+1-r. Results are illustrated with explicit 3x3 Jordan block computations for 1F1, 2F1, and the time evolution operator, confirming sharpness of the bounds.
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math-ph 2026-05-01

Two Hamilton-Jacobi theories for dissipative field theories via k-contact geometry

Hamilton--Jacobi theory for non-conservative field theories in the k-contact framework

Dynamics reconstructed from integrable k-vector fields on base manifolds, with explicit equations for affine Hamiltonians and recovery of k=

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This article develops a Hamilton--Jacobi theory for non-conservative classical field theories, with particular emphasis on dissipative systems, in the framework of co-oriented k-contact geometry. We introduce evolution k-contact k-vector fields, extending the contact evolution formalism to field theories, and analyse the corresponding Hamilton--De Donder--Weyl equations. Moreover, we develop two distinct families of Hamilton--Jacobi theories: a z-independent approach, based on the reconstruction of the dynamics from an integrable k-vector field defined on the base manifold of $(\bigoplus^kT^*Q)\times\mathbb{R}^k\to Q$, and a z-dependent approach, where the integrable k-vector field is defined on the base manifold of $(\bigoplus^kT^*Q)\times\mathbb{R}^k\to Q\times\mathbb{R}^k$. We develop in detail the important case of Hamiltonian functions with affine dependence on the dissipative variables, show how quadratic dependence on these variables can be used structurally to enlarge the range of applications, and recover the ordinary contact Hamilton--Jacobi theory as the particular case k=1, while removing some technical assumptions appearing in previous formulations. Our theory is illustrated through several representative examples, including the telegrapher/Klein--Gordon equation, a dissipative Hunter--Saxton equation, a simple dissipative non-regular first-order field model, and a relativistic thermodynamic model.
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math-ph 2026-04-30

Chern character jumps keep states delocalized under disorder

Dynamical delocalization in disordered 2D Chern insulators

Continuity of averaged projections with energy and disorder strength makes the topological index robust, allowing transitions even after gap

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We show the existence of energies exhibiting dynamical delocalization in discrete 2D Chern insulators perturbed by a random potential in a general setting. Our proof exploits two main features of the model: jumps in the integer value of the Chern character and continuity of averaged spectral projections in both energy and disorder parameters. This allows us to show robustness of the topological index in the presence of disorder, which, combined with existing methods to prove dynamical localization, allows us to provide detailed information on the phase diagram of the model. The novelty of our approach is that we are able to show dynamical delocalization in the disorder parameter, and not only in the energy parameter, which allows to prove Anderson metal-insulator transition even when spectral gaps close due to the strength of disorder.
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math-ph 2026-04-30

Twist of quantum group generates long-range spin-chain deformations

The quantum group structure of long-range integrable deformations

The resulting non-associative algebra encodes the long-range terms while a large perturbative substructure preserves integrability to first

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Quantum integrable spin chains are known to possess a large family of long-range deformations generated by the local, boost and bilocal operators. Although these deformations are well-understood on the level of the pairwise commuting charges, the underlying quantum group structures had not yet been recognised. In this paper, we provide a quantum group-theoretical description for the family of long-range deformations of arbitrary homogeneous Yang-Baxter integrable spin chains up to first order in the deformation parameter. In particular, we show that the deformations are obtained via a twist of the algebraic structure of the underlying quantum group. This twisting results in a generally non-associative algebra that has a non-trivial Drinfeld associator. The Drinfeld associator is then shown to encode the information about the long-range interaction terms for the integrable spin chain. Moreover, the deformed quantum group is shown to contain a large perturbatively associative substructure, thus ensuring the perturbative integrability of the long-range model. The deformed quantum group provides explicit expressions for the Lax operators and R-matrices of the long-range deformed models, which manifestly satisfy the RLL relation and the Yang-Baxter equation up to first order in the deformation parameter. In order to derive the results, we introduce algebra elements that we call the algebraic charge densities. As a side result, we provide a conjecture for the explicit expressions of the undeformed charge densities in terms of these algebra elements.
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math-ph 2026-04-30

Initial-data gauge fix yields Hadamard states for Maxwell on curved spacetime

On the Quantisation of Linear Gauge Theories on Lorentzian Manifolds: Maxwell's Theory via Complete Gauge Fixing

Hodge decomposition on Cauchy surfaces removes unphysical modes, enabling rigorous quantization of electromagnetic fields in general spacetm

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This thesis is devoted to the study of hyperbolic differential operators on globally hyperbolic manifolds, linear gauge theories and their quantisation. In the first part, we treat the Cauchy problem for symmetric hyperbolic systems and normally hyperbolic operators on globally hyperbolic manifolds from first principles. Although hyperbolic equations are usually studied with local interactions, there are strong motivations from several areas of mathematical physics to consider also nonlocal interactions. As an intermezzo, we therefore take a small deviation from the classical local theory and prove well-posedness of the Cauchy problem for symmetric hyperbolic systems coupled to a broad class of nonlocal potentials. The second part presents a detailed exposition of linear gauge theories in globally hyperbolic spacetimes. Linear gauge theories are yet another deviation from the concept of hyperbolicity: the corresponding equations of motion are generically non-hyperbolic; however, can always be reduced to a constrained hyperbolic dynamics once an appropriate gauge fixing procedure has been applied. We give a thorough analysis of their Cauchy problem and classical phase space, complemented by a detailed discussion of many examples of physical interest, and discuss their quantisation following the algebraic approach to quantum field theory. The final chapter is devoted to the quantisation of Maxwell's theory on globally hyperbolic spacetimes, with the goal of proving the existence of Hadamard states. The novelty of our approach lies in a new gauge-fixing procedure at the level of initial data, which allows us to suppress the unphysical degrees of freedom. This gauge is achieved by means of a new Hodge decomposition for differential k-forms in Sobolev spaces on complete Riemannian manifolds, while states are constructed using tools from pseudodifferential calculus.
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math-ph 2026-04-30

Qubit phases turn comparison defects into geometric phases

Remarks on pairwise comparisons, transition amplitudes, and qubit states

Triangular inconsistencies in the extracted U(1) structure equal normalized Bargmann invariants for non-orthogonal pure states.

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We discuss a pairwise-comparison viewpoint on finite families of qubit states. Starting from transition amplitudes between pure states, we distinguish three associated levels of comparison data: complex amplitudes, transition probabilities, and phase-valued pairwise comparisons. In the non-orthogonal case, the phase data define a \(U(1)\)-valued reciprocal pairwise comparison structure. We show that the corresponding triangular defects are naturally related to normalized Bargmann invariants and therefore to geometric phases. This gives a simple interpretation of inconsistency-type quantities in terms of quantum kinematics. We also comment on realizability constraints coming from Gram matrices of rank at most two, and on the passage from unitary phase data to more general transition data. The aim of the paper is mainly conceptual: to isolate a common language between pairwise comparisons and elementary quantum geometry.
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math-ph 2026-04-30

Toda integrability yields structures for b-angulations

On enumeration of b-angulations of surfaces from an integrability perspective

Explicit formulas for b=3 and b=4 plus a fine structure for even b follow from integrability and imply a prior conjecture.

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In this paper, we study generating series enumerating polygonal angulations of closed oriented surfaces of fixed genus, focusing on $b$-angulations with $b = 3$ or $b = 2\nu$, $\nu \geq 2$. Based on Toda integrability, we establish new structural results in the cases $b = 3$ and $b = 4$. Furthermore, via the Hodge--GUE correspondence, we derive a fine structure in the $b = 2\nu$ case, which implies a conjectural statement of Gharakhloo--Latimer.
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math-ph 2026-04-30

Pandharipande equations extended to double Hurwitz numbers

Combinatorics and asymptotic behavior for double Hurwitz numbers

The recursions from the 2-Toda hierarchy produce explicit asymptotic formulas when genus or degree grows large.

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Polynomial-in-time algorithms for computing classical Hurwitz numbers were given in [4] based on the Pandharipande equation. The paritition function of double Hurwitz numbers was proved [21] to satisfy the 2-Toda hierarchy. In this paper, similar to [21] we derive Pandharipande-type equations for double Hurwitz numbers from 2-Toda hierarchy. Based on these equations and a method from [4], we study large genus as well as large degree asymptotics of double Hurwitz numbers.
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math-ph 2026-04-30

Rigged Liouville supports super bra-ket for quasi-Hermitian operators

Rigged Liouville space formulation for quasi-Hermitian Liouville operators

Unitary equivalence of Hilbert-Schmidt operators to tensor products yields symmetric structures and dual-space spectra.

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We discuss a super bra-ket formalism for quasi-Hermitian Liouvillian operators within the framework of rigged Hilbert spaces (RHS). An RHS in terms of the Liouville space, referred to as a rigged Liouville space (RLS), is reconstructed by exploiting the mathematical fact that the space of Hilbert-Schmidt operators is unitarily equivalent to the tensor product of Hilbert spaces. The obtained RLS endows a rigorous foundation of the construction for the super bra-ket and for the spectral decompositions of both Hermitian and quasi-Hermitian Liouville operators, which are characterized by the generalized eigenvectors in the dual spaces. Furthermore, within this framework, the non-Hermitian Liouvillian operator and its adjoint can be constructed symmetrically, with their symmetric structure preserved. As an application of our RLS methodology, we examine the Liouville operators corresponding to Hermitian and non-Hermitian harmonic oscillators and elucidate the differences between their spectral decomposition forms.
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math-ph 2026-04-29

Jacobi algebra solves generic superintegrable model on sphere

The dynamical algebra of the generic superintegrable model on the two-sphere

Embedding inside su(1,1) tensor product yields algebraic spectrum and two-variable Jacobi polynomial wavefunctions.

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The rank two Jacobi algebra $\mathfrak{J}_2$ is identified as the dynamical algebra of the generic quadratic superintegrable model on the two-sphere. The physical representation of this algebra is obtained from its embedding in $\mathfrak{su}(1,1)^{\otimes 3}$. The exact solution of the model is derived algebraically from this representation. The wavefunctions are found to be expressed in terms of two-variable Jacobi polynomials whose characterization is a by-product of the algebraic treatment of the model.
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math-ph 2026-04-29

Level crossings of random pencils converge to deterministic measure

Level Crossing in Random Matrices. III. Analogs of Girko's circular and Wigner's semicircle laws

The empirical distribution settles to an explicit limit once circular law, tail bounds, and repulsion estimates hold, verified outright for

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We study the asymptotic distribution of level crossings for random matrix pencils A_n+\lambda B_n in several ensembles, including complex and real i.i.d. matrices and Gaussian/Hermitian settings. We derive a representation of the normalized log-discriminant in terms of pairwise eigenvalue interactions and formulate conditions under which its limit is governed by a deterministic potential. Under assumptions combining a uniform circular law, logarithmic tail control, and small-spacing (repulsion) estimates, we prove convergence of the empirical measure of level crossings to an explicit deterministic limit. In the complex Gaussian case these assumptions are verified (modulo a uniformity step), while in the general i.i.d. setting the results are conditional and motivated by universality theory. We further analyze the real case, showing that any limiting measure does not concentrate on the real projective line under suitable hypotheses, and discuss analogous phenomena for elliptic/Hermitian ensembles. Our results highlight the role of logarithmic energy and universality in governing spectral degeneracies of random matrix pencils.
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math-ph 2026-04-29

Refined homomorphisms induce sl2 symmetry in triplet W-algebras

Derivations on the triplet W-algebras with mathfrak{sl}₂-symmetry

The maps extend the known derivation property to general parameters and determine the automorphism group of the related superalgebra.

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We construct derivations on the triplet $W$-algebras $\mathcal{W}_{p_+,p_-}$ by refining the Frobenius homomorphisms of Tsuchiya-Wood and show that the property of the Adamovi\'{c}-Milas derivation for $\mathcal{W}_{2,p}$ extends to our derivations. As an application, we show that the $\mathfrak{sl}_2$-symmetry of $\mathcal{W}_{p_+,p_-}$ arises naturally from our construction. We further show that our method applies to the triplet $W$-superalgebra $\mathcal{SW}(m)$ and that the full automorphism group ${\rm Aut}(\mathcal{SW}(m))$ is $PSL_2(\mathbb{C})\times \mathbb{Z}_2$.
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math-ph 2026-04-29

Newell equation long-time asymptotics derived rigorously

Long-time asymptotics of the Newell equation on the line

Riemann-Hilbert analysis and steepest descent give explicit leading terms in the dispersive region for rapid-decay data

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In 1978, A. C. Newell [SIAM J. Appl. Math. 35(4) (1978) 650-664] proposed an exactly solvable model called Newell equation, which simulates the investigation of significant interaction mechanism between long and short waves. Nearly fifty years have passed, yet the long-time asymptotics of the Newell equation remains an open problem to date, with no results reported. In this work, the long-time asymptotic behaviors of the solutions to this model under Schwartz class initial conditions are studied by using the Riemann-Hilbert formulation. Through direct and inverse scattering analysis, the corresponding Riemann-Hilbert problem is formulated, and its relationship with the solution to the initial-value problem of the Newell equation is established. The existence and uniqueness of the solution to the Riemann-Hilbert problem is proved by vanishing lemma. Subsequently, the asymptotic expressions of the solution to the initial-value problem in the dispersive wave region are obtained by using the Deift-Zhou nonlinear steepest descent method. This work extends Newell's original results, providing a rigorous proof for the findings presented in Section 4 of his paper, along with explicit expressions. Furthermore, the comparison between direct numerical simulations and the theoretical results obtained in this paper demonstrates the reliability of the asymptotic expressions.
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math-ph 2026-04-29

Newell equation asymptotics derived via steepest descent

Long-time asymptotics of the Newell equation on the line

Schwartz data enable Riemann-Hilbert formulation whose long-time behavior is extracted explicitly.

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In 1978, A. C. Newell [SIAM J. Appl. Math. 35(4) (1978) 650-664] proposed an exactly solvable model called Newell equation, which simulates the investigation of significant interaction mechanism between long and short waves. Nearly fifty years have passed, yet the long-time asymptotics of the Newell equation remains an open problem to date, with no results reported. In this work, the long-time asymptotic behaviors of the solutions to this model under Schwartz class initial conditions are studied by using the Riemann-Hilbert formulation. Through direct and inverse scattering analysis, the corresponding Riemann-Hilbert problem is formulated, and its relationship with the solution to the initial-value problem of the Newell equation is established. The existence and uniqueness of the solution to the Riemann-Hilbert problem is proved by vanishing lemma. Subsequently, the asymptotic expressions of the solution to the initial-value problem in the dispersive wave region are obtained by using the Deift-Zhou nonlinear steepest descent method. This work extends Newell's original results, providing a rigorous proof for the findings presented in Section 4 of his paper, along with explicit expressions. Furthermore, the comparison between direct numerical simulations and the theoretical results obtained in this paper demonstrates the reliability of the asymptotic expressions.
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math-ph 2026-04-29

Griffiths inequalities hold for general gauge glasses on Nishimori line

Griffiths inequalities and Gibbs-Bogoliubov inequality for general gauge glasses with Gaussian disorder on Nishimori line

Monotonicity of pressure and correlations follows, and replica-symmetric mean-field approximations upper-bound the true quenched free energy

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We consider a class of gauge glass models with Gaussian disorder on the Nishimori line, including the Ising spin glass, the $XY$ gauge glass, the $Z_q$ gauge glass, and the gauge-invariant Potts model. We prove that the first and second Griffiths inequalities hold for these models on arbitrary lattice structures. As a consequence, both the pressure and the correlation functions are monotonically increasing with respect to the inverse temperature along the Nishimori line. Furthermore, we establish an analogue of the Gibbs--Bogoliubov inequality for this class of models. This result implies that, on the Nishimori line, the approximate quenched free energy obtained via the replica method with a replica-symmetric mean-field approximation is always greater than the true quenched free energy. Our results provide a broad generalization of previous results established for the Ising spin glass with Gaussian disorder on the Nishimori line.
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math-ph 2026-04-29

Curvature gradient sets rotation rate of vortex pairs on catenoid

Co-rotating Vortices on Surfaces of Variable Negative Curvature: Hamiltonian Structure and Drift Dynamics

Exact antipodal solution spins at speed fixed by how curvature changes with latitude, yielding instability and secular drift.

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Vortices in fluids and superfluids underpin phenomena ranging from Bose--Einstein condensates and superfluid films to neutron stars and hydrodynamic micro-rotors, where geometry can strongly influence their motion. Curvature can induce vortex motion with no planar analogue. We study Hamiltonian vortex motion on a catenoid, a minimal surface of variable negative curvature, and derive explicit equations of motion, conserved quantities, and reductions for co-rotating vortex pairs. For two identical vortices we find an exact antipodal solution in which the pair rotates rigidly at fixed latitude, with angular velocity $\Omega=(\Gamma/16\pi)\,K'(V)/\sqrt{-K(V)}$, where $K(V)$ is the Gaussian curvature. Thus the motion is governed by the curvature gradient rather than the curvature itself. The symmetric state is linearly unstable, with growth rate $\lambda=\sqrt{3}|\Omega|$, in agreement with numerical simulations. For generic equal-strength pairs, conservation of the Hamiltonian and rotational momentum reduces the nonlinear dynamics to a single quadrature, yielding bounded relative oscillations together with a secular azimuthal drift. Simulations of the full equations confirm the reduced theory and reveal the same curvature-induced transport mechanism in a localized many-vortex cluster, motivating a broader theory of collective vortex drift on curved surfaces.
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math-ph 2026-04-29

Finite differences create non-unique phase retrieval examples

On phase retrieval for continuous and discrete Fourier transforms

The method produces distinct sparse functions with matching Fourier intensities and resolves an open question for holography.

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We continue studies on phase retrieval for continuous and discrete Fourier transforms in multidimensions. Using finite difference operators, we give a large class of unexpected examples of non-uniqueness for this problem, including examples with the sparsity condition. A prototype of this construction in the continuous case is given in the work Novikov, Xu (JFAA, 2026), using linear differential operators. The construction of the present work also yields a large class of non-trivial Pauli partners, i.e., different functions with the same intensities in both configuration and Fourier domains. Besides, our construction yields examples that solve an old open question in phase retrieval with background information arising in many areas including Fourier holography.
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math-ph 2026-04-29

Log topological recursion defines free energies matching known partitions

Geometry of Logarithmic Topological Recursion: Dilaton Equations, Free Energies and Variational Formulas

New definition reproduces Nekrasov-Shatashvili and all-genus mirror curve energies without extra computation.

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One of the most important applications of topological recursion concerns spectral curves for which the functions $(x,y)$ defining the spectral curve are allowed to have logarithmic singularities. This occurs for instance for Seiberg-Witten curves and mirror curves computing Gromov--Witten invariants of toric Calabi--Yau threefolds. A recently introduced extension of topological recursion, the so-called logarithmic topological recursion, exhibits the correct behavior under certain limits of those spectral curves. In this article, we derive the dilaton equations in the setting of logarithmic topological recursion, as well as variational formulas, and provide a definition of the free energies in situations where standard topological recursion was known to fail. We present examples in which the new definition of the free energies \textit{directly} (without any computation) reproduces the full perturbative part of the Nekrasov--Shatashvili partition function of 4d $\mathcal{N}=2$ pure supersymmetric gauge theory, as well as the all-genus free energies of mirror curves of strip geometries, including in particular the topological vertex and the resolved conifold.
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math-ph 2026-04-29

Arbitrary-variance SK spin glass has explicit free energy at high temperature

The SK model with a sparse variance profile: free energy and AMP algorithm for TAP equations at high temperature

The asymptotic formula and convergent AMP solver for magnetizations hold for any fixed, possibly sparse profile.

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A generalization of the Sherrington-Kirkpatrick (SK) model for spin glasses is considered, in which the interaction matrix is endowed with a variance profile that has no particular structure an may be sparse. In the first part of this paper, an asymptotic equivalent of the free energy is derived at sufficiently high temperatures, regardless of the signature of the variance profile matrix. In the second part, the mean of the spin vector under the Gibbs measure is estimated using an Approximate Message Passing algorithm based on the Thouless-Anderson-Palmer equations. The dynamical approach of Adhikari et.al. (J. Stat. Phys., 2021), originally developed for the classical SK model, is adapted to the present setting to obtain these results.
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math-ph 2026-04-29

Three symmetry classes for time-fractional telegraph equations

Lie symmetry classification and invariant solutions of time-fractional telegraph systems with variable coefficients

Classification by transport-potential relation yields exact solutions in Mittag-Leffler and Fox H-functions.

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Time-fractional telegraph equations provide fundamental mathematical models for transport processes that exhibit memory and nonlocal effects in industrial and physical systems. These models arise naturally in heat transport in materials with thermal memory, wave propagation in viscoelastic media, and charge transport in spatially heterogeneous semiconductor devices. In this study, we investigate a class of time-fractional telegraph systems with spatially varying coefficients using Lie symmetry analysis and the Riemann--Liouville fractional derivative. We establish a complete Lie group classification for sufficiently differentiable coefficient functions and determine all functional forms that admit such symmetry extensions. The symmetry structure is shown to depend fundamentally on the relationship between the transport coefficient and the potential function, resulting in three distinct symmetry classes. For each case, optimal systems of one-dimensional Lie subalgebras are constructed, and the governing fractional partial differential equations are systematically reduced to fractional ordinary differential equations. Exact invariant solutions are obtained in closed form and expressed in terms of Mittag--Leffler functions, generalized Wright functions, and Fox $H$-functions. These analytical solutions provide valuable insights into fractional telegraph-type transport phenomena and serve as important benchmarks for validating numerical methods in industrial transport modeling and fractional evolution systems.
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math-ph 2026-04-29

Riesz gas covariances reduce to Gegenbauer polynomial sums

Gegenbauer polynomials and fluctuation properties of the one-dimensional Riesz gas

The formula for s in (-1,1) generalizes the cosine expansion at s=0 and collapses to gamma products for power sums.

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The Riesz gas in one-dimension consists of particles interacting via a pair potential, ${\rm sgn}(s) |x - x'|^{-s}$, $s \ne 0$ and $-\log | x - x'|$ for $s=0$. In the infinite density limit, with the particle support the interval $[-1,1]$, we apply a functional derivative method due to Beenakker to compute the covariance of two smooth linear statistics for the Riesz gas with exponent $s \in (-1,1)$, $s \ne 0$. This we give in terms of a sum over Fourier components of the linear statistics with respect to a Gegenbauer polynomial $\{C_n^{(s/2)}(x) \}$ basis, which generalises a known form in the case $s=0$ involving a cosine expansion. For the power sum linear statistic, our general formula can be reduced to a product of gamma function form, and compared against recent exact results in the literature for this case.
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math-ph 2026-04-28

Invariant measure on energy surfaces yields statistical ensembles

Invariant Measures in Hamiltonian Systems: The Analytical Foundations of Statistical Physics

The construction stays preserved under Hamiltonian flow and produces both microcanonical and canonical partition functions from dynamics.

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We construct a measure in the hamiltonian function level sets that is invariant under the hamiltonian flow for short times and flow preserving for arbitrarily long times. This allows a probabilistic approach to the study of hamiltonian systems, in the space of states with fixed energy. We prove that this measure generates the microcanonical partition function employed in physics and show that it can be transformed into the canonical partition function in an asymptotic limit, hence reproducing classical Statistical Physics. We also argue that this gives an alternative solution to Simon's second problem.
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math-ph 2026-04-28

Every AQFT has a prefactorization algebra of its superselection sectors

Prefactorization algebras of superselection sectors

Under Haag duality the sectors assemble into a locally constant C*-categorical structure over the same spacetime regions.

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This paper revisits the theory of superselection sectors in algebraic quantum field theory from the modern perspective of prefactorization algebras. Under the standard assumptions of Haag duality and a locally faithful vacuum representation, it is shown that every AQFT defined over a filtered orthogonal category of spacetime regions, satisfying some mild additional geometric hypotheses, has an associated locally constant $C^\ast$-categorical prefactorization algebra of superselection sectors over the same orthogonal category. In the case of double cones in the $(n\geq 2)$-dimensional Minkowski spacetime, our approach provides a conceptual explanation for the well-known $\mathbb{E}_n$-monoidal structure on the $C^\ast$-category of superselection sectors as the combination, through Dunn-Lurie additivity $\mathbb{E}_n\simeq \mathbb{E}_1\otimes \mathbb{E}_{n-1}$, of the familiar $\mathbb{E}_1$-monoidal structure from Haag duality and an $\mathbb{E}_{n-1}$-monoidal structure from Lorentzian geometry. A refinement of our results to equivariant contexts under a discrete group $G$ is also provided.
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math-ph 2026-04-28

Pauli stabilizer codes match Clifford QCAs one dimension higher

The Classification of Pauli Stabilizer Codes: A Lattice and Continuum Treatise

Bulk-boundary correspondence classifies lattice codes up to gapped interfaces using algebraic L-theory and reveals differences from framedTQ

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We classify mobile Pauli stabilizer codes up to gapped interfaces and coarse-graining using the framework of algebraic $\mathrm{L}$-theory. We compare this classification with that of framed TQFTs, theories that arise naturally in the continuum, highlighting a close structural relationship between the two. Our approach is formulated in the category of perfect chain complexes equipped with quadratic functor over the Laurent polynomial ring $R = \mathbb{Z}/p[x_1^{\pm 1}, \ldots, x_n^{\pm 1}]$, within which the collection of topological operators of Pauli stabilizer codes arise naturally as objects. In particular, we establish a bulk-boundary correspondence for lattice theories: the equivalence class of a Pauli stabilizer code up to gapped interface is described by a Clifford QCA in one dimension higher. This is done using the universal target category for stabilizer codes, which is the categorical spectrum whose existence and universal properties are introduced in this work. We conclude by highlighting subtle differences between the classification of Pauli stabilizer codes and TQFTs, leading to qualitative distinctions between lattice and continuum theories.
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