Discrete honeycombs, rational edges and edge statesConsider the tight binding model of graphene, sharply terminated along an edge l parallel to a direction of translational symmetry of the underlying period lattice. We classify such edges…C. L. Fefferman, S. Fliss, M. I. Weinstein·Mar 7, 2022SaveLearn
Hamilton-Jacobi approach to thermodynamic transformationsIn this note, we formulate and study a Hamilton-Jacobi approach for describing thermodynamic transformations. The thermodynamic phase space assumes the structure of a contact manifold with the points…Aritra Ghosh·Mar 7, 2022SaveLearn
Bogoliubov Theory in the Gross-Pitaevskii Limit: a Simplified ApproachWe show that Bogoliubov theory correctly predicts the low-energy spectral properties of Bose gases in the Gross-Pitaevskii regime. We recover recent results from BBCS,BBCS4. While our main…Christian Hainzl, Benjamin Schlein, Arnaud Triay·Mar 7, 2022SaveLearn
Characterizing Schwarz maps by tracial inequalitiesLet ϕ be a linear map from the n× n matrices Mn to the m× m matrices Mm. It is known that ϕ is 2-positive if and only if for all K∈ Mn…Eric A. Carlen, Alexander Müller-Hermes·Mar 7, 2022SaveLearn
Shape of eigenvectors for the decaying potential modelWe consider the 1d Schrödinger operator with decaying random potential, and study the joint scaling limit of the eigenvalues and the measures associated with the corresponding eigenfunctions which is…Fumihiko Nakano·Mar 7, 2022SaveLearn
Pizzetti formulae and the Radon Transform on the SphereIn this paper, we obtain Pizzetti-type formulae on regions of the the unit sphere Sm-1 of Rm, and study their applications to the problem of inverting the spherical Radon…Alí Guzmán Adán, Mihaela B. Vajiac·Mar 7, 2022SaveLearn
A generalised time-evolution model for contact problems with wear and its analysisIn this paper, we revisit some classical and recent works on modelling slide-contact with wear and propose their generalisation. Namely, we upgrade the relation between the pressure and the wear rate…Dmitry Ponomarev·Mar 6, 2022SaveLearn
Landau-Ginzburg mirror, quantum differential equations and qKZ difference equations for a partial flag varietyWe consider the system of quantum differential equations for a partial flag variety and construct a basis of solutions in the form of multidimensional hypergeometric functions, that is, we construct…Vitaly Tarasov, Alexander Varchenko·Mar 6, 2022SaveLearn
Propagation of moments for large data and semiclassical limit to the relativistic Vlasov equationWe investigate the semiclassical limit from the semi-relativistic Hartree-Fock equation describing the time evolution of a system of fermions in the mean-field regime with a relativistic dispersion…Nikolai Leopold, Chiara Saffirio·Mar 6, 2022SaveLearn
Laplace and Dirac Operators on GraphsDiscrete versions of the Laplace and Dirac operators haven been studied in the context of combinatorial models of statistical mechanics and quantum field theory. In this paper we introduce several…Beata Casiday, Ivan Contreras, Thomas Meyer et al.·Mar 5, 2022SaveLearn
The generalized Marchenko method in the inverse scattering problem for a first-order linear systemThe Marchenko method is developed in the inverse scattering problem for a linear system of first-order differential equations containing potentials proportional to the spectral parameter. The…T. Aktosun, R. Ercan·Mar 5, 2022SaveLearn
The Fragmentation Kernel in Multinary/Multicomponent FragmentationThe fragmentation equation is commonly expressed in terms of two functions, the rate of fragmentation and the mean number of fragments. In the case of binary fragmentation an alternative description…Themis Matsoukas·Mar 5, 2022SaveLearn
Optimal parabolic upper bound for the energy-momentum relation of a strongly coupled polaronWe consider the large polaron described by the Fr\"ohlich Hamiltonian and study its energy-momentum relation defined as the lowest possible energy as a function of the total momentum. Using a…David Mitrouskas, Krzysztof Myśliwy, Robert Seiringer·Mar 4, 2022SaveLearn
Family of asymptotic solutions to the two-dimensional kinetic equation with a nonlocal cubic nonlinearityWe apply the original semiclassical approach to the kinetic ionization equation with the nonlocal cubic nonlinearity in order to construct the family of its asymptotic solutions. The approach…Alexander V. Shapovalov, Anton E. Kulagin, Sergei A. Siniukov·Mar 4, 2022SaveLearn
Galton-Watson trees with first ancestor interactionWe consider the set of random Bienaymé-Galton-Watson trees with a bounded number of offspring and bounded number of generations as a statistical mechanics model: a random tree is a rooted subtree of…Francois Dunlop, Arif Mardin·Mar 4, 2022SaveLearn
Law of Large Numbers for Random Quantum Dynamical SemigroupsWe present a Law of Large Numbers principle for uniformly continuous random quantum dynamical semigroups. Random iterates of independent copies of these semigroups are shown to be Chernoff equivalent…John E. Gough, Yurii N. Orlov, Vsevolod Zh. Sakbaev et al.·Mar 4, 2022SaveLearn
Moments dynamics and stationary states for classical diffusion-type GKSL equationsThe explicit dynamics of the moments for the GKSL equation and the approach in finding stationary Gaussian states are obtained. In our case the GKSL equation corresponds to Wiener stochastic…D. D. Ivanov, A. E. Teretenkov·Mar 3, 2022SaveLearn
Chirality in Affine Spaces and in SpacetimeAn object is chiral when its symmetry group contains no indirect isometry. It can be difficult to classify isometries as direct or indirect, except in the Euclidean case. We classify them with the…Michel Petitjean·Mar 3, 2022SaveLearn
A second order upper bound on the ground state energy of a Bose gas beyond the Gross-Pitaevskii regimeWe consider a system of N bosons in a unitary box in the grand-canonical setting interacting through a potential with scattering length scaling as N-1+κ, κ∈ (0,2/3). This regimes…Giulia Basti·Mar 3, 2022SaveLearn
Clusters of resonances for a non-selfadjoint multichannel discrete Schr\"odinger operatorWe study the distribution of resonances for discrete Hamiltonians of the form H0+V near the thresholds of the spectrum of H0. Here, the unperturbed operator H0 is a multichannel Laplace type…Marouane Assal, Olivier Bourget, Pablo Miranda et al.·Mar 2, 2022SaveLearn
Periodic striped states in Ising models with dipolar interactionsWe review the problem of determining the ground states of 2D Ising models with nearest neighbor ferromagnetic and dipolar interactions, and prove a new result supporting the conjecture that, if the…Davide Fermi, Alessandro Giuliani·Mar 2, 2022SaveLearn
Principal Eigenvalue and Landscape Function of the Anderson Model on a Large BoxWe state a precise formulation of a conjecture concerning the product of the principal eigenvalue and the sup-norm of the landscape function of the Anderson model restricted to a large box. We first…Daniel Sánchez-Mendoza·Mar 2, 2022SaveLearn
Macroscopic behaviour in a two-species exclusion process via the method of matched asymptoticsWe consider a two-species simple exclusion process on a periodic lattice. We use the method of matched asymptotics to derive evolution equations for the two population densities in the dilute regime,…James Mason, Robert L Jack, Maria Bruna·Mar 2, 2022SaveLearn
From Short-Range to Mean-Field Models in Quantum LatticesRealistic effective interparticle interactions of quantum many-body systems are widely seen as being short-range. However, the rigorous mathematical analysis of this type of model turns out to be…J. -B. Bru, W. de Siqueira Pedra, K. Rodrigues Alves·Mar 2, 2022SaveLearn
On symbol correspondences for quark systems I: CharacterizationsWe present the characterizations of symbol correspondences for mechanical systems that are symmetric by SU(3), which we refer to as quark systems. The quantum quark systems are the unitary…P. A. S. Alcântara, P. de M. Rios·Mar 1, 2022SaveLearn