Canonical formulation for the thermodynamics of sln-invariant integrable spin chainsIntegrable quantum spin chains display distinctive physical properties making them a laboratory to test and assess different states of matter. The study of the finite temperature properties is…T. S. Tavares, I. R. Passos, A. Klümper·Nov 3, 2023SaveLearn
Interface fluctuations associated with split Fermi seasWe consider the asymptotic behaviour of a family of unidimensional lattice fermion models, which are in exact correspondence with certain probability laws on partitions and on unitary matrices. These…Harriet Walsh·Nov 3, 2023SaveLearn
Computer-assisted proofs of existence of KAM tori in planetary dynamical models of -And bWe reconsider the problem of the orbital dynamics of the innermost exoplanet of the -Andromedae system (i.e., -And b) into the framework of a Secular Quasi-Periodic…Rita Mastroianni, Ugo Locatelli·Nov 3, 2023SaveLearn
Optimal Control of Incompressible Ideal Flows with Obstacle AvoidanceIt was shown in bloch2000optimal that an optimal control formulation for incompressible ideal fluid flow yields Euler's equations. In this paper, we consider a variational obstacle-avoidance…Alexandre Anahory Simoes, Anthony Bloch, Leonardo Colombo·Nov 3, 2023SaveLearn
A functional model of a class of symmetric semi-bounded operatorsLet L0 be a closed symmetric positive definite operator with nonzero defect indices n(L0) in a separable Hilbert space H. It determines a family of dynamical systems…M. I. Belishev, S. A. Simonov·Nov 2, 2023SaveLearn
Pseudorandomness of the Schr\"odinger map equationWe present the random behaviour of the Schr\"odinger map equation, a geometric partial differential equation, by considering its evolution for regular polygonal curves in both Euclidean and…Sandeep Kumar·Nov 2, 2023SaveLearn
On the stochastic Sine-Gordon model: an interacting field theory approachWe investigate the massive Sine-Gordon model in the finite ultraviolet regime on the two-dimensional Minkowski spacetime (R2,η) with an additive Gaussian white noise. In particular we…Alberto Bonicelli, Claudio Dappiaggi, Paolo Rinaldi·Nov 2, 2023SaveLearn
Topological edge spectrum along curved interfacesWe prove that that if the boundary of a topological insulator divides the plane in two regions containing arbitrarily large balls, then it acts as a conductor. Conversely, we show that topological…Alexis Drouot, Xiaowen Zhu·Nov 2, 2023SaveLearn
Characteristics of rogue waves in the scalar and vector nonlocal nonlinear Schrödinger equationsIn this paper, general higher-order rogue wave solutions of the parity-time ( P T) symmetric scalar and coupled nonlocal nonlinear Schrödinger equations (NLSEs) are calculated…Xiu-Bin Wang, Shou-Fu Tian·Nov 2, 2023SaveLearn
Singularities and asymptotic distribution of resonances for Schr\"odinger operators in one dimensionWe obtain new results about the high-energy distribution of resonances for the one-dimensional Schr\"odinger operator. Our primary result is an upper bound on the density of resonances above any…T. J. Christiansen, T. Cunningham·Nov 1, 2023SaveLearn
Weyl Group Representation of Billiard Trajectories for One-dimensional Hard Sphere DynamicsWe present an exact formula for the dynamics of N hard spheres of radius r>0 on an infinite line which evolve under the assumption that total linear momentum and kinetic energy of the system is…Mark Wilkinson·Nov 1, 2023SaveLearn
Gauge equivalence and transdimensional perturbation: point vorticesThere is an explicit resolution of the Poisson reduction of four planar point vortices, in the case that three of the vortex strengths are equal and the total vorticity is zero. The resolution, a…George W. Patrick·Oct 31, 2023SaveLearn
Variational principle for a damped, quadratically interacting particle chain with nonconservative forcingA method for designing variational principles for the dynamics of a possibly dissipative and non-conservatively forced chain of particles is demonstrated. Some qualitative features of the formulation…Amit Acharya, Ambar N. Sengupta·Oct 31, 2023SaveLearn
Obstructions to the existence of Mller mapsMller maps are identifications between the observables of a perturbatively interacting physical system and the observables of its underlying free (i.e. non-interacting) system. This work studies…Marco Benini, Alastair Grant-Stuart, Giorgio Musante et al.·Oct 31, 2023SaveLearn
Schur function expansion in non-Hermitian ensembles and averages of characteristic polynomialsWe study k-point correlators of characteristic polynomials in non-Hermitian ensembles of random matrices, focusing on the real, complex and quaternion N × N Ginibre ensembles. Our approach…Alexander Serebryakov, Nick Simm·Oct 31, 2023SaveLearn
Local solutions of RG flow equations from the Nash-Moser theoremWe prove local existence of solutions of a functional Renormalisation Group equation for the effective action of an interacting quantum field theory, when a suitable Local Potential Approximation is…Edoardo D'Angelo, Nicola Pinamonti·Oct 31, 2023SaveLearn
Undressing the electronThe extended algebra of the free electromagnetic fields, including infrared singular fields, and the almost radial gauge, both introduced earlier, are postulated for the construction of the quantum…Andrzej Herdegen·Oct 31, 2023SaveLearn
Wolfes model aka G2/I6-rational integrable model: g(2), g(3) hidden algebras and quartic polynomial algebra of integralsOne-dimensional 3-body Wolfes model with 2- and 3-body interactions also known as G2/I6-rational integrable model of the Hamiltonian reduction is exactly-solvable and superintegrable. Its…J C Lopez Vieyra, A V Turbiner·Oct 31, 2023SaveLearn
Beliaev damping in Bose gasAccording to the Bogoliubov theory the low energy behaviour of the Bose gas at zero temperature can be described by non-interacting bosonic quasiparticles called phonons. In this work the damping…Jan Dereziński, Ben Li, Marcin Napiórkowski·Oct 30, 2023SaveLearn
Kerner equation for motion in a non-Abelian gauge fieldThe equations of motion of an isospin-carrying particle in a Yang-Mills and gravitational field were first proposed in 1968 by Kerner, who considered geodesics in a Kaluza-Klein-type framework. Two…Peter A Horvathy, Peng-Ming Zhang·Oct 30, 2023SaveLearn
Kinetic description and macroscopic limit of swarming dynamics with continuous leader-follower transitionsIn this paper, we derive a kinetic description of swarming particle dynamics in an interacting multi-agent system featuring emerging leaders and followers. Agents are classically characterized by…Emiliano Cristiani, Nadia Loy, Marta Menci et al.·Oct 30, 2023SaveLearn
An operational point of view to the theory of multi-variable/multi-index Hermite polynomialsThe use of algebraic tools of operational and umbral nature is exploited to develop a new point of view and to extend the theory of Hermite polynomials, with more than one variable also of complex…Giuseppe Dattoli, Silvia Licciardi, Elio Sabia·Oct 30, 2023SaveLearn
Classification of the anyon sectors of Kitaev's quantum double modelWe give a complete classification of the anyon sectors of Kitaev's quantum double model on the infinite triangular lattice and for finite gauge group G, including the non-abelian case. As…Alex Bols, Siddharth Vadnerkar·Oct 30, 2023SaveLearn
The Application of Homotopy Perturbation Method to the Solution of Non-Linear Partial Differential EquationsIn this study, a thorough investigation was conducted into the Homotopy Perturbation Method (HPM) and its application to solve the Burger and Blasius equations. The HPM is a mathematical technique…Gbenga Onifade Ebenezer·Oct 30, 2023SaveLearn
From O-operators of 3-Dimensional 3-Lie algebras to 3-Pre-Lie algebrasIn this paper, we explicitly determine all O-operators with respect to the adjoint representation of 3-dimensional complex 3-Lie algebras. Furthermore, we provide the induced 3-Pre-Lie…Cheng Ziying, Kang Chuangchuang, Lü Jiafeng·Oct 30, 2023SaveLearn