Infinitesimal Rigidity of Strain Tensors for Shells with Mixed Type and its ApplicationsWe derive an infinitesimal rigidity lemma for the strain tensor of surfaces with their curvatures changing sign. As an application, we obtain the optimal constant in the first Korn inequality scales…Liang-Biao Chen, Peng-Fei Yao·Jun 24, 2022SaveLearn
Trace distance ergodicity for quantum Markov semigroupsWe discuss the quantitative ergodicity of quantum Markov semigroups in terms of the trace distance from the stationary state, providing a general criterion based on the spectral decomposition of the…Lorenzo Bertini, Alberto De Sole, Gustavo Posta·Jun 23, 2022SaveLearn
Hofstadter butterflies and metal/insulator transitions for moir\'e heterostructuresWe consider a tight-binding model recently introduced by Timmel and Mele for strained moir\'e heterostructures. We consider two honeycomb lattices to which layer antisymmetric shear strain is applied…Simon Becker, Lingrui Ge, Jens Wittsten·Jun 23, 2022SaveLearn
Contact Lagrangian systems subject to impulsive constraintsWe describe geometrically contact Lagrangian systems under impulsive forces and constraints, as well as instantaneous nonholonomic constraints which are not uniform along the configuration space. In…Leonardo J. Colombo, Manuel de León, Asier López-Gordón·Jun 23, 2022SaveLearn
Geometry of the discrete time Euler top and related 3-dimensional birational mapsIn this thesis we consider a discretization of the Euler top given by Hirota und Kimura. Using the geometric description of the conserved quantities as quadrics in real 3-space, we find that there…Nina Smeenk·Jun 23, 2022SaveLearn
The finite gap method and the periodic Cauchy problem of 2+1 dimensional anomalous waves for the focusing Davey-Stewartson 2 equationThe focusing Nonlinear Schrödinger (NLS) equation is the simplest universal model describing the modulation instability (MI) of 1+1 dimensional quasi monochromatic waves in weakly nonlinear media,…P. G. Grinevich, P. M. Santini·Jun 23, 2022SaveLearn
Some useful operators on differential forms in Galilean and Carrollian spacetimesDifferential forms on Lorentzian spacetimes is a well-established subject. On Galilean and Carrollian spacetimes it does not seem to be quite so. This may be due to the absence of Hodge star…Marián Fecko·Jun 22, 2022SaveLearn
The Ground State Energy of a Two-Dimensional Bose GasWe prove the following formula for the ground state energy density of a dilute Bose gas with density ρ in 2 dimensions in the thermodynamic limit align* e2D(ρ) = 4πρ2 Y(1 -…S. Fournais, T. Girardot, L. Junge et al.·Jun 22, 2022SaveLearn
Dirac reductions and Classical W-algebrasIn the first part of this paper, we generalize Dirac reduction to the extent of non-local Poisson vertex superalgebra and non-local SUSY Poisson vertex algebra cases. Next, we modify this reduction…Gahng Sahn Lee, Arim Song, Uhi Rinn Suh·Jun 21, 2022SaveLearn
On Generalized WKB Expansion of Monodromy Generating FunctionWe study symplectic properties of the monodromy map of the Schr\"odinger equation on a Riemann surface with a meromorphic potential having second-order poles. At first, we discuss the conditions for…Roman Klimov·Jun 21, 2022SaveLearn
Connes spectral distances, quantum discord and coherence of qubitsWe construct spectral triples of one- and two-qubit states using the Hilbert-Schmidt operatorial formulation, and study the Connes spectral distances. We also construct the Dirac operator…Bing-Sheng Lin, Zi-Hao Xu, Ji-Hong Wang et al.·Jun 21, 2022SaveLearn
Spectra of generators of Markovian evolution in the thermodynamic limit: From non-Hermitian to full evolution via tridiagonal Laurent matricesIt is shown that generators of single-particle, translation-invariant Lindblad operators on the infinite line are unitarily equivalent to direct integrals of finite-range bi-infinite Laurent operator…Frederik Ravn Klausen·Jun 20, 2022SaveLearn
Perturbation theory for nonlinear Schrodinger equationsTreating the nonlinear term of the Gross-Pitaevskii nonlinear Schrodinger equation as a perturbation of an isolated discrete eigenvalue of the linear problem one obtains a Rayleigh-Schrodinger power…Andrea Sacchetti·Jun 20, 2022SaveLearn
Galilean and Carrollian Hodge star operatorsThe standard Hodge star operator is naturally associated with metric tensor (and orientation). It is routinely used to concisely write down physics equations on, say, Lorentzian spacetimes. On…Marián Fecko·Jun 20, 2022SaveLearn
Spectral branch points of the Bloch-Torrey operatorWe investigate the peculiar feature of non-Hermitian operators, namely, the existence of spectral branch points (also known as exceptional or level crossing points), at which two (or many) eigenmodes…Nicolas Moutal, Denis S. Grebenkov·Jun 20, 2022SaveLearn
Scaling Symmetries, Contact Reduction and Poincaré's dreamA symplectic Hamiltonian system admitting a scaling symmetry can be reduced to an equivalent contact Hamiltonian system in which some physically-irrelevant degree of freedom has been removed. As a…Alessandro Bravetti, Connor Jackman, David Sloan·Jun 20, 2022SaveLearn
Mobility estimation for Langevin dynamics using control variatesThe scaling of the mobility of two-dimensional Langevin dynamics in a periodic potential as the friction vanishes is not well understood for non-separable potentials. Theoretical results are lacking,…G. A. Pavliotis, G. Stoltz, U. Vaes·Jun 20, 2022SaveLearn
Kolmogorov algorithm for isochronous Hamiltonian systemsWe present a Kolmogorov-like algorithm for the computation of a normal form in the neighborhood of an invariant torus in `isochronous' Hamiltonian systems, i.e., systems with Hamiltonians of the…Rita Mastroianni, Christos Efthymiopoulos·Jun 20, 2022SaveLearn
Sparse Random Block Matrices : universalityWe study ensembles of sparse random block matrices generated from the adjacency matrix of a Erdös-Renyi random graph with N vertices of average degree Z, inserting a real symmetric d × d…Giovanni M. Cicuta, Mario Pernici·Jun 19, 2022SaveLearn
Complex Generalized Integral Means Spectrum of Drifted Whole-Plane SLE and LLEWe present new results for the complex generalized integral means spectrum for two kinds of whole-plane Loewner evolutions driven by L\'evy processes: - L\'evy processes with continuous trajectories,…Bertrand Duplantier, Yong Han, Chi Nguyen et al.·Jun 18, 2022SaveLearn
(2+1)-dimensional KdV, fifth-order KdV, and Gardner equations derived from the ideal fluid model. Soliton, cnoidal and superposition solutionsWe study the problem of gravity surface waves for an ideal fluid model in the (2+1)-dimensional case. We apply a systematic procedure to derive the Boussinesq equations for a given relation between…Anna Karczewska, Piotr Rozmej·Jun 17, 2022SaveLearn
Singular cotangent models and complexity in fluids with dissipationIn this article we analyze several mathematical models with singularities where the classical cotangent model is replaced by a b-cotangent model. We provide physical interpretations of the singular…Baptiste Coquinot, Pau Mir, Eva Miranda·Jun 17, 2022SaveLearn
Asymmetric transport computations in Dirac models of topological insulatorsThis paper presents a fast algorithm for computing transport properties of two-dimensional Dirac operators with linear domain walls, which model the macroscopic behavior of the robust and asymmetric…Guillaume Bal, Jeremy G Hoskins, Zhongjian Wang·Jun 17, 2022SaveLearn
Universality of the number variance in rotational invariant two-dimensional Coulomb gasesAn exact map was established by Lacroix-A-Chez-Toine, Majumdar, and Schehr in [44] between the N complex eigenvalues of complex non-Hermitian random matrices from the Ginibre ensemble, and the…Gernot Akemann, Sung-Soo Byun, Markus Ebke·Jun 17, 2022SaveLearn
Discrete orthogonal ensemble on the exponential latticesInspired by Aomoto's q-Selberg integral, the orthogonal ensemble in the exponential lattice is considered in this paper. By introducing a skew symmetric kernel, the configuration space of this…Peter J Forrester, Shi-Hao Li, Bo-Jian Shen et al.·Jun 17, 2022SaveLearn