Renormalizations in holomorphic field theories on Kähler manifoldsThe divergence of Feynman graph integrals is one of the central issues in the study of perturbative quantum field theories. A rigorous formulation of these integrals usually requires renormalization.…Minghao Wang, Junrong Yan·Aug 6, 2026SaveLearn
Hyperbolic Completion of Newton's Off-Center Orbit Problem: SO(2,1) Symmetry, Inversion Duality, and Magnetic ClassificationWhich central forces produce circular trajectories whose geometric center differs from the force center? We solve the hyperbolic version of this problem for V(r)=-α(R2-r2)2, α>0,…Dipesh Bhandari·Aug 6, 2026SaveLearn
Time-marching representation based quantum algorithms for the Lattice Boltzmann model of the advection-diffusion equationThis article introduces a novel framework for developing quantum algorithms for the Lattice Boltzmann Method (LBM) applied to the advection-diffusion equation. We formulate the collision-streaming…Yuan He, Yuan Yu, Yue Yu·Aug 6, 2026SaveLearn
Boundary structure of gauge fields on asymptotically AdS spacesWe study the boundary structure of asymptotically AdS gravity and (gauge) fields defined on this background by employing the gauge PDE approach. The essential step of the construction is the…Maxim Grigoriev, Mikhail Markov·Aug 6, 2026SaveLearn
The index of a pair of pure states and the interacting integer quantum Hall effectWe introduce the index N(ω1,ω2) of a pair of pure states on a unital C*-algebra, which is a generalization of the notion of the index of a pair of projections on a Hilbert space. We…Sven Bachmann, Jacob Shapiro, Clément Tauber·Aug 6, 2026SaveLearn
Transparent boundary conditions for the spatially discrete Schrödinger equation: Reflectionless quantum transport in 1D latticesWe construct exact transparent boundary conditions (TBCs) for a time-continuous, spatially discrete Schrödinger equation that models a one-dimensional quantum lattice. Using a recently developed…Mashrab E. Akramov, Jambul R. Yusupov, Matthias Ehrhardt et al.·Aug 5, 2026SaveLearn
Phase transitions in generalized XY modelsWe associate height function models to a range of generalized two-dimensional XY models and prove that delocalisation of the height function model rules out exponential decay of the nematic order…Fabio Plaga·Aug 5, 2026SaveLearn
Multi-frequency far-field data enrichment for electromagnetic source reconstructionReconstructing unknown electromagnetic sources from far-field radiation patterns is a fundamental inverse problem with broad applications in biomedical imaging, non-destructive testing, and…Atyab Khalifa Al-Shaqsi, Heba Mohammed Al-Subhi, Xianchao Wang et al.·Aug 5, 2026SaveLearn
Lee-Yang Zeros And Particle FluctuationsWe consider classical particles in the continuum in the grand canonical ensemble, with a stable, tempered and lower-regular pair potential and boundary conditions of uniformly bounded density. We…Mohamed El Hedi Bahri, Ian Jauslin, Joel L. Lebowitz·Aug 5, 2026SaveLearn
Jordan-Twist Bethe Ansatz and Many-Body Exceptional-Point Amplification in the Finite-U Anderson ImpurityWe construct an interacting integrable realization of many-body exceptional-point amplification in the static equal-velocity linearized finite-U Anderson impurity. Two spin-orbit branches are…Vinayak M. Kulkarni·Aug 5, 2026SaveLearn
Local measurements and the entanglement transition in quantum spin chainsWe consider the transition between short-range entangled (SRE) and long-range entangled states of infinite quantum spin chains which is induced by local measurements. Specifically, we assume that the…Sven Bachmann, Mahsa Rahnama, Gabrielle Tournaire·Aug 5, 2026SaveLearn
Irreversible dynamics on Poisson manifoldsWe present a geometric construction of irreversible dynamics on Poisson manifolds that satisfies the axioms of metriplectic mechanics and the GENERIC framework. Our approach relies solely on the…Erwin Luesink·Aug 5, 2026SaveLearn
On the dependence of the zero-free region of a partition function on the external fieldLet \0, 1\n be the Boolean cube, endowed with the probability product measure, where P(1)=p and P(0)=q with 0 < p ≤ q and p+q=1. For i=1, …, m, let $ϕi: \0,…Alexander Barvinok·Aug 4, 2026SaveLearn
A Tau function for q-Painlevé VI as a Fredholm determinantWe give an analytic construction of a tau function for the q-difference sixth Painlevé equation (qPVI) as a Fredholm determinant through the general Riemann-Hilbert problem associated with it. We…Harini Desiraju, Pieter Roffelsen·Aug 4, 2026SaveLearn
The co-directional overtaking collision problem between a dispersive shock wave and a rarefaction wave for the Hirota equationIn this paper, we mainly investigate the overtaking collision problem between a dispersive shock wave (DSW) and a rarefaction wave (RW) propagating in the same direction in the defocusing Hirota…Yuan Xiang, Rui Guo·Aug 4, 2026SaveLearn
From Convex to Non-convex: Evolution of Rarefaction-dispersive shock interactions and the Influence of Non-convexityIn this paper, we focus on the analytical description of the interaction between a rarefaction and dispersive shock wave across both convex and non-convex cases, with particular attention to the…Jia-Xue Niu, Rui Guo, Hua-Ying Ren et al.·Aug 4, 2026SaveLearn
Quantum Turing PatternsWe construct quantum Turing patterns in Lindblad lattice dynamics and establish a rigorous theory of their nonlinear order and quantum fluctuations. For an explicit family of completely positive…Kazuki Ikeda·Aug 4, 2026SaveLearn
Quantum estimates for classical polynomial optimizationThe problem of finding lower and upper bounds on multivariate homogeneous polynomials is both difficult and important given its applications to questions ranging from dynamical stability in complex…Oleg Evnin·Aug 4, 2026SaveLearn
A maximal Hohenberg-Kohn theorem for non-interacting systems via potential theoryWe show that for Schrödinger operators in a connected domain, the Hohenberg-Kohn theorem holds within the class of Laplace form-bounded external potentials if and only if the single-particle density…Thiago Carvalho Corso·Aug 4, 2026SaveLearn
The bosonic Hubbard model on a three dimensional flat band latticeThe lowest eigenstates of the hopping matrix on the line graph of a cubic lattice with periodic boundary conditions are highly degenerate, they form a lowest flat band. Further, these states are…Leon Haag-Fank, Andreas Mielke·Aug 4, 2026SaveLearn
Fold of a bifurcation solution from the figure-eight choreography in the three body problemIn the figure-eight choreography in the classical three-body problem, both-side bifurcation solutions sometimes fold on one side of the bifurcation point with cusp of action. Three numerical examples…Hiroshi Fukuda, Hiroshi Ozaki·Aug 4, 2026SaveLearn
Irreversibility and randomnessWe make the idea of "molecular chaos" precise through algorithmic randomness of microscopic trajectories. Apart from making this idea concrete, this has three advantages. First, it sharpens…Nino Dekkers, Klaas Landsman·Aug 4, 2026SaveLearn
Subalgebras of Lie algebras. Example of sl(3,R) revisitedRevisiting the results by Winternitz [Symmetry in physics, CRM Proc. Lecture Notes 34, American Mathematical Society, Providence, RI, 2004, pp. 215-227], we thoroughly refine his classification of…Yevhenii Yu. Chapovskyi, Serhii D. Koval, Olha Zhur·Aug 4, 2026SaveLearn
Selection criteria for the compressible Euler equations: numerical studyWe numerically investigate selection criteria for dissipative weak solutions of the compressible Euler equations. Using the Kelvin-Helmholtz problem as a benchmark, we compare four standard numerical…Megala Anandan, Bahulayan Chalil Aravind, Mária Lukáčová-Medvid'ová et al.·Aug 3, 2026SaveLearn
Topological Recursion and Quantum Path SignaturesWe introduce a non-commutative Laplace transform between functionals on path space and formal series in a tensor algebra, under which a natural convolution of path functionals becomes an algebraic…Inês Aniceto, Thomas Cass, Samuel Crew·Aug 3, 2026SaveLearn