On the topology of the space of coordination geometriesCoordination geometries describe how the neighbours of a central particle are arranged around it. Such geometries can be thought to lie in an abstract topological space; a model of this space could…John Çamkıran, Fabian Parsch, Glenn D. Hibbard·Jul 25, 2022SaveLearn
Graphene Dirac fermions in symmetric electric and magnetic fields: the case of an electric square wellIn this paper, a simple method is proposed to get analytical solutions (or with the help of a finite numerical calculations) of the Dirac-Weyl equation for low energy electrons in graphene in the…İsmail Burak Ateş, Şengül Kuru, Javier Negro·Jul 25, 2022SaveLearn
Conversations with Flaschka: Kac-Moody groups and Verblunsky coefficientsIn this paper we discuss two items which in one way or another originated from conversations with Hermann Flaschka and his students. The first is an application of the Toda lattice to the question of…Mohammad Javad Latifi, Doug Pickrell·Jul 23, 2022SaveLearn
Towards a mathematical Theory of the Madelung EquationsEven though the Madelung equations are central to many 'classical' approaches to the foundations of quantum mechanics such as Bohmian and stochastic mechanics, no coherent mathematical theory has…Maik Reddiger, Bill Poirier·Jul 22, 2022SaveLearn
Exponential moments for disk counting statistics at the hard edge of random normal matricesWe consider the multivariate moment generating function of the disk counting statistics of a model Mittag-Leffler ensemble in the presence of a hard wall. Let n be the number of points. We focus on…Yacin Ameur, Christophe Charlier, Joakim Cronvall et al.·Jul 22, 2022SaveLearn
A Szego Limit Theorem Related to the Hilbert MatrixThe Szego limit theorem by Fedele and Gebert for matrices of the type identity minus Hankel matrix is proved for the special case 1-βπHN,α where HN,α is the…Peter Otte·Jul 22, 2022SaveLearn
Toward fixed point and pulsation quantum search on graphs driven by quantum walks with in- and out-flows: a trial to the complete graphWe treat a quantum walk model with in- and out- flows at every time step from the outside. We show that this quantum walk can find the marked vertex of the complete graph with a high probability in…Yusuke Higuchi, Mohamed Sabri, Etsuo Segawa·Jul 21, 2022SaveLearn
Existence of the transfer matrix for a class of nonlocal potentials in two dimensionsEvanescent waves are waves that decay or grow exponentially in regions of the space void of interaction. In potential scattering defined by the Schr\"odinger equation, (-∇2+v)=k2 for…Farhang Loran, Ali Mostafazadeh·Jul 20, 2022SaveLearn
Determining the volume fraction in 2-phase composites and bodies using time varying applied fieldsA body containing two phases, which may form a periodic composite with microstructure much smaller that the body, or which may have structure on a length scale comparable to the body, is…Ornella Mattei, Graeme W. Milton, Mihai Putinar·Jul 20, 2022SaveLearn
Dirac cones for a mean-field model of grapheneIn this article, we show that, in the dissociation regime and under a non-degeneracy assumption, the reduced Hartree-Fock theory of graphene presents Dirac points at the vertices of the first…Jean Cazalis·Jul 20, 2022SaveLearn
Self-avoiding walks contained within a squareWe have studied self-avoiding walks contained within an L × L square whose end-points can lie anywhere within, or on, the boundaries of the square. We prove that such walks behave,…Anthony J Guttmann, Iwan Jensen, Aleksander L Owczarek·Jul 20, 2022SaveLearn
A Novel Potential Featuring Off-Center Circular OrbitsIn Book 1, Proposition 7, Problem 2 of his 1687 Philosophiae Naturalis Principia Mathematica, Isaac Newton poses and answers the following question: Let the orbit of a particle moving in a central…Maxim Olshanii·Jul 20, 2022SaveLearn
The Blume-Emery-Griffiths model at the FAD and AD interfacesWe analyse the Blume-Emery-Griffiths (BEG) model on the lattice at the ferromagnetic-antiquadrupolar-disordered (FAD) and antiquadrupolar-disordered (AD) interfaces of parameters. In our…Paulo C. Lima, Riccardo Mariani, Aldo Procacci et al.·Jul 19, 2022SaveLearn
Ground States for Infrared Renormalized Translation-Invariant Non-Relativistic QEDWe consider a translation-invariant Pauli-Fierz model describing a non-relativistic charged quantum mechanical particle interacting with the quantized electromagnetic field. The charged particle may…David Hasler, Oliver Siebert·Jul 19, 2022SaveLearn
A dualization approach to the Ground State Subspace Classification of Abelian Higher Gauge Symmetry ModelsIn the literature, abelian higher gauge symmetry models are shown to be valid in all finite dimensions and exhibit the characteristic behavior of SPT phases models. While the ground state degeneracy…J. Lorca Espiro·Jul 19, 2022SaveLearn
Parametric models and information geometry on W*-algebrasWe introduce the notion of smooth parametric model of normal positive linear functionals on possibly infinite-dimensional W*-algebras generalizing the notions of parametric models used in classical…Florio M. Ciaglia, Fabio Di Nocera, Jürgen Jost et al.·Jul 19, 2022SaveLearn
On General-n Coefficients in Series Expansions for Row Spin-Spin Correlation Functions in the Two-Dimensional Ising ModelWe consider spin-spin correlation functions for spins along a row, Rn = σ0,0σn,0, in the two-dimensional Ising model. We discuss a method for calculating general-n…Robert Shrock·Jul 19, 2022SaveLearn
A characterisation of orthomodular spaces by Sasaki mapsGiven a Hilbert space H, the set P(H) of one-dimensional subspaces of H becomes an orthoset when equipped with the orthogonality relation induced by the inner product on H. Here, an…Bert Lindenhovius, Thomas Vetterlein·Jul 19, 2022SaveLearn
Notes on invariant measures for loop groupsLet K denote a simply connected compact Lie group and let G=K C, the complexification. It is known that there exists an LK bi-invariant probability measure on a natural hyperfunction…Doug Pickrell·Jul 19, 2022SaveLearn
Deformation quantization of the simplest Poisson OrbifoldWhenever a given Poisson manifold is equipped with discrete symmetries the corresponding algebra of invariant functions or the algebra of functions twisted by the symmetry group can have new…Alexey Sharapov, Evgeny Skvortsov, Arseny Sukhanov·Jul 18, 2022SaveLearn
When Poisson and Moyal Brackets are equal?In the phase space 2d, let us denote \A,B\ the Poisson bracket of two smooth classical observables and \A, B\ their Moyal bracket, defined as the Weyl symbol of $i[ A,…Didier Robert·Jul 18, 2022SaveLearn
G-dual teleparallel connections in Information GeometryGiven a real, finite-dimensional, smooth parallelizable Riemannian manifold (N,G) endowed with a teleparallel connection ∇ determined by a choice of a global basis of vector fields…Florio M. Ciaglia, Fabio Di Cosmo, Alberto Ibort et al.·Jul 18, 2022SaveLearn
Variational analysis in one and two dimensions of a frustrated spin system: chirality transitions and magnetic anisotropic transitionsWe study the energy of a ferromagnetic/antiferromagnetic frustrated spin system with values on two disjoint circumferences of the 3-dimensional unit sphere in a one-dimensional and two-dimensional…Andrea Kubin, Lorenzo Lamberti·Jul 18, 2022SaveLearn
Winding Number Statistics for Chiral Random Matrices: Averaging Ratios of Determinants with Parametric DependenceTopological invariance is a powerful concept in different branches of physics as they are particularly robust under perturbations. We generalize the ideas of computing the statistics of winding…Nico Hahn, Mario Kieburg, Omri Gat et al.·Jul 18, 2022SaveLearn
Perturbation theory for the 43 measure, revisited with Hopf algebrasWe give a relatively short, almost self-contained proof of the fact that the partition function of the suitably renormalised 43 measure admits an asymptotic expansion, the coefficients of…Nils Berglund, Tom Klose·Jul 18, 2022SaveLearn