Log-Sobolev inequality for the 42 and 43 measuresThe continuum 42 and 43 measures are shown to satisfy a log-Sobolev inequality uniformly in the lattice regularisation under the optimal assumption that their susceptibility is…Roland Bauerschmidt, Benoit Dagallier·Feb 4, 2022SaveLearn
Quantum number towers for the Hubbard and Holstein modelsIn 1989, Elliott Lieb published a Physical Review Letter proving two theorems about the Hubbard model. This paper used the concept of spin-reflection positivity to prove that the ground state of the…Janes K. Freericks·Feb 4, 2022SaveLearn
A Markov Chain Surrogate Model for a Two-Dimensional Interacting Particle System with Internal CollisionsA probabilistic Markov Chain (MC) surrogate model for a two-dimensional system of interacting particles within a square domain having inherent symmetries is developed. Particles are assumed to be…Tricity Andrew, James D. Nance, Mansoor A. Haider·Feb 4, 2022SaveLearn
Heat coefficients for magnetic Laplacians on the complex projective space Pn(C)Denoting by Δν the Fubini-Study Laplacian perturbed by a uniform magnetic field strength proportional to ν, this operator has a discrete spectrum consisting on eigenvalues $βm, \…K. Ahbli, A. Hafoud, Z. Mouayn·Feb 4, 2022SaveLearn
The new simplest proof of Ceyley's formula and connections with Kirkwood-Salzburg equationsA new very simple proof of the number of labeled rooted forest-graphs with a given number of vertices is given. As a partial case of this formula we have Cayley's formula.Alexei L. Rebenko·Feb 4, 2022SaveLearn
Conjugation Matters. Bioctonionic Veronese Vectors and Cayley-Rosenfeld PlanesMotivated by the recent interest in Lie algebraic and geometric structures arising from tensor products of division algebras and their relevance to high energy theoretical physics, we analyze…Daniele Corradetti, Alessio Marrani, David Chester et al.·Feb 4, 2022SaveLearn
Shape Dynamics of N Point Vortices on the SphereWe give a geometric account of the relative motion or the shape dynamics of N point vortices on the sphere exploiting the SO(3)-symmetry of the system. The main idea is to bypass the…Tomoki Ohsawa·Feb 3, 2022SaveLearn
Bose-Einstein condensation on hyperbolic spacesA well-known conjecture in mathematical physics asserts that the interacting Bose gas exhibits Bose-Einstein condensation (BEC) in the thermodynamic limit. We consider the Bose gas on certain…Marius Lemm, Oliver Siebert·Feb 3, 2022SaveLearn
Statistical mechanics of Coulomb systems: From electrons and nuclei to atoms and moleculesThis article is dedicated to Elliott Lieb in celebration of his 90th birthday. I recount briefly some history of our joint work on the existence of the thermodynamic limit for Coulomb systems and…Joel L. Lebowitz·Feb 3, 2022SaveLearn
Eyring-Kramers type formulas for some piecewise deterministic Markov processesIn this work, we give sharp asymptotic equivalents in the small temperature regime of the smallest eigenvalues of the generator of some piecewise deterministic Markov processes (including the ZigZag…Dorian Le Peutrec, Laurent Michel, Boris Nectoux·Feb 3, 2022SaveLearn
The Madelung Constant in N DimensionsWe introduce two convergent series expansions (direct and recursive) in terms of Bessel functions and representations of sums rN(m) of squares for N-dimensional Madelung constants, MN(s),…Antony Burrows, Shaun Cooper, Peter Schwerdtfeger·Feb 3, 2022SaveLearn
Elliptic generalization of integrable q-deformed anisotropic Haldane-Shastry long-range spin chainWe describe integrable elliptic q-deformed anisotropic long-range spin chain. The derivation is based on our recent construction for commuting anisotropic elliptic spin Ruijsenaars-Macdonald…M. Matushko, A. Zotov·Feb 2, 2022SaveLearn
Winding number and homotopy for quaternionic curvesFollowing a recent approach to quaternionic curves, we defined the quaternionic polar angle that enabled us to define global properties of quaternionic curves, namely the winding number and the…Sergio Giardino·Feb 2, 2022SaveLearn
The Role of Second Law of Thermodynamics in Continuum Physics: A Muschik and Ehrentraut Theorem RevisitedSecond law of thermodynamics imposes that in any thermodynamic process the entropy production must be nonnegative. In continuum physics such a requirement is fulfilled by postulating the constitutive…V. A. Cimmelli, P. Rogolino·Feb 2, 2022SaveLearn
Inverse problems for locally perturbed lattices -- Discrete Hamiltonian and quantum graphWe consider the inverse scattering problems for two types of Schrödinger operators on locally perturbed periodic lattices. For the discrete Hamiltonian, the knowledge of the S-matrix for all energies…Emilia Blåsten, Pavel Exner, Hiroshi Isozaki et al.·Feb 2, 2022SaveLearn
Ballistic transport in periodic and random mediaWe prove ballistic transport of all orders, that is, xme-itHψ tm, for the following models: the adjacency matrix on Zd, the Laplace operator on…Anne Boutet de Monvel, Mostafa Sabri·Feb 2, 2022SaveLearn
Discrete Dirac reduction of implicit Lagrangian systems with abelian symmetry groupsThis paper develops the theory of discrete Dirac reduction of discrete Lagrange-Dirac systems with an abelian symmetry group acting on the configuration space. We begin with the linear theory and,…Álvaro Rodríguez Abella, Melvin Leok·Feb 1, 2022SaveLearn
On Products of Random MatricesWe introduce a family of models, which we name matrix models associated with children's drawings -- the so-called dessin d'enfant. Dessins d'enfant are graphs of a special kind drawn on a…Natalia Amburg, Aleksandr Yu. Orlov, Dmitry Vasiliev·Feb 1, 2022SaveLearn
On the Pernici-Wanless Expansion for the Entropy ( and Virial Coefficients ) of a Dimer Gas on an Infinite Regular LatticeWe work with the following expression for the entropy (density) of a dimer gas on an infinite r-regular lattice lambda(p) = 1/2 [ pln(r)-ln(p)-2(1-p)ln(1-p)-p ]+sumk=2(dk)(pk) where the…Paul Federbush·Feb 1, 2022SaveLearn
Generalized forms, metrics and Ricci flat four-metricsGeneralized differential forms are used in discussions of metric geometries and Einstein's vacuum field equations. Cartan's structure equations are generalized and applied. In particular flat…D C Robinson·Feb 1, 2022SaveLearn
Spectral Analysis of the Quantum Random Energy ModelThe Quantum Random Energy Model (QREM) is a random matrix of Anderson-type which describes effects of a transversal magnetic field on Derrida's spin glass. The model exhibits a glass phase as…Chokri Manai, Simone Warzel·Feb 1, 2022SaveLearn
Trajectories of charged particles in knotted electromagnetic fieldsWe investigate the trajectories of point charges in the background of finite-action vacuum solutions of Maxwell's equations known as knot solutions. More specifically, we work with a basis of…Kaushlendra Kumar, Olaf Lechtenfeld, Gabriel Picanço Costa·Feb 1, 2022SaveLearn
Ground state energy of the low density Bose gas with three-body interactionsWe consider the low density Bose gas in the thermodynamic limit with a three-body interaction potential. We prove that the leading order of the ground state energy of the system is determined…Phan Thành Nam, Julien Ricaud, Arnaud Triay·Jan 31, 2022SaveLearn
Nambu-Goldstone Modes for Superconducting Lattice FermionsWe present a lattice model for superconducting fermions whose nearest-neighbour two-body interactions are a Bardeen-Cooper-Schrieffer-type pairing on the hypercubic lattice Zd with the…Tohru Koma·Jan 31, 2022SaveLearn
Current correlations, Drude weights and large deviations in a box-ball systemWe explore several aspects of the current fluctuations and correlations in the box-ball system (BBS), an integrable cellular automaton in one space dimension. The state we consider is an ensemble of…Atsuo Kuniba, Grégoire Misguich, Vincent Pasquier·Jan 31, 2022SaveLearn