0000000000395537

AUTHOR

Thierry Combot

showing 7 related works from this author

Integrability of the one dimensional Schrödinger equation

2018

We present a definition of integrability for the one dimensional Schroedinger equation, which encompasses all known integrable systems, i.e. systems for which the spectrum can be explicitly computed. For this, we introduce the class of rigid functions, built as Liouvillian functions, but containing all solutions of rigid differential operators in the sense of Katz, and a notion of natural boundary conditions. We then make a complete classification of rational integrable potentials. Many new integrable cases are found, some of them physically interesting.

Class (set theory)Integrable systemFOS: Physical sciencesComplex analysisAlgebras01 natural sciencesSchrödinger equationsymbols.namesake[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]0103 physical sciencesBoundary value problem0101 mathematics010306 general physicsGauge field theoryMathematical PhysicsMathematical physicsMathematicsMSC: 34M46 34M50 37J30Liouville equation010102 general mathematicsSpectrum (functional analysis)Operator theory[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]Statistical and Nonlinear PhysicsMathematical Physics (math-ph)Differential operatorHamiltonian mechanicssymbols34M46 34M50 37J30
researchProduct

Integrability and Non Integrability of Some n Body Problems

2016

International audience; We prove the non integrability of the colinear 3 and 4 body problem, for any positive masses. To deal with resistant cases, we present strong integrability criterions for 3 dimensional homogeneous potentials of degree −1, and prove that such cases cannot appear in the 4 body problem. Following the same strategy, we present a simple proof of non integrability for the planar n body problem. Eventually, we present some integrable cases of the n body problem restricted to some invariant vector spaces.

[ MATH ] Mathematics [math]Pure mathematicsDegree (graph theory)Integrable systemCentral configurationsn-body problem[ PHYS.ASTR ] Physics [physics]/Astrophysics [astro-ph]010102 general mathematicsMathematical analysisDifferential Galois theory01 natural sciences010101 applied mathematicsDifferential Galois theoryHomogeneousSimple (abstract algebra)Integrable systems0101 mathematicsInvariant (mathematics)[MATH]Mathematics [math]Homogeneous potentialMorales-Ramis theory[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]MathematicsVector space
researchProduct

Bi-homogeneity and integrability of rational potentials

2020

Abstract In this paper we consider natural Hamiltonian systems with two degrees of freedom for which Hamiltonian function has the form H = 1 2 ( p 1 2 + p 2 2 ) + V ( q 1 , q 2 ) and potential V ( q 1 , q 2 ) is a rational function. Necessary conditions for the integrability of such systems are deduced from integrability of dominate term of the potential which usually is appropriately chosen homogeneous term of V. We show that introducing weights compatible with the canonical structure one can find new dominant terms which can give new necessary conditions for integrability. To deduce them we investigate integrability of a family of bi-homogeneous potentials which depend on two integer para…

Hamiltonian mechanicsPure mathematicsPolynomialDegree (graph theory)Integrable system010308 nuclear & particles physicsApplied MathematicsHomogeneous potentialsRational functionDifferential Galois theoryIntegrability01 natural sciencesHamiltonian systemsymbols.namesakeQuadratic equationIntegerSpecial functions0103 physical sciencessymbolsMSC 37J30[MATH]Mathematics [math]010306 general physicsAnalysisMathematicsJournal of Differential Equations
researchProduct

Elementary Integration of Superelliptic Integrals

2021

Consider a superelliptic integral $I=\int P/(Q S^{1/k}) dx$ with $\mathbb{K}=\mathbb{Q}(\xi)$, $\xi$ a primitive $k$th root of unity, $P,Q,S\in\mathbb{K}[x]$ and $S$ has simple roots and degree coprime with $k$. Note $d$ the maximum of the degree of $P,Q,S$, $h$ the logarithmic height of the coefficients and $g$ the genus of $y^k-S(x)$. We present an algorithm which solves the elementary integration problem of $I$ generically in $O((kd)^{\omega+2g+1} h^{g+1})$ operations.

Coprime integersDegree (graph theory)LogarithmRoot of unity010102 general mathematics68W300102 computer and information sciencesIntegration problem01 natural sciencesCombinatoricsMathematics - Algebraic Geometry010201 computation theory & mathematicsSimple (abstract algebra)Genus (mathematics)FOS: Mathematics[MATH]Mathematics [math]0101 mathematicsAlgebraic Geometry (math.AG)Symbolic integrationMathematicsProceedings of the 2021 on International Symposium on Symbolic and Algebraic Computation
researchProduct

A Symplectic Kovacic's Algorithm in Dimension 4

2018

Let $L$ be a $4$th order differential operator with coefficients in $\mathbb{K}(z)$, with $\mathbb{K}$ a computable algebraically closed field. The operator $L$ is called symplectic when up to rational gauge transformation, the fundamental matrix of solutions $X$ satisfies $X^t J X=J$ where $J$ is the standard symplectic matrix. It is called projectively symplectic when it is projectively equivalent to a symplectic operator. We design an algorithm to test if $L$ is projectively symplectic. Furthermore, based on Kovacic's algorithm, we design an algorithm that computes Liouvillian solutions of projectively symplectic operators of order $4$. Moreover, using Klein's Theorem, algebraic solution…

[MATH.MATH-DS]Mathematics [math]/Dynamical Systems [math.DS]010102 general mathematicsDynamical Systems (math.DS)Differential operator01 natural sciencesSymplectic matrixDifferential Galois theory34M15Operator (computer programming)Fundamental matrix (linear differential equation)Mathematics - Symplectic Geometry0103 physical sciencesFOS: MathematicsSymplectic Geometry (math.SG)010307 mathematical physicsMathematics - Dynamical Systems0101 mathematicsAlgebraically closed fieldAlgebraic numberMathematics::Symplectic GeometryAlgorithmMathematicsSymplectic geometryProceedings of the 2018 ACM International Symposium on Symbolic and Algebraic Computation
researchProduct

Symbolic integration of hyperexponential 1-forms

2019

Let $H$ be a hyperexponential function in $n$ variables $x=(x_1,\dots,x_n)$ with coefficients in a field $\mathbb{K}$, $[\mathbb{K}:\mathbb{Q}] <\infty$, and $\omega$ a rational differential $1$-form. Assume that $H\omega$ is closed and $H$ transcendental. We prove using Schanuel conjecture that there exist a univariate function $f$ and multivariate rational functions $F,R$ such that $\int H\omega= f(F(x))+H(x)R(x)$. We present an algorithm to compute this decomposition. This allows us to present an algorithm to construct a basis of the cohomology of differential $1$-forms with coefficients in $H\mathbb{K}[x,1/(SD)]$ for a given $H$, $D$ being the denominator of $dH/H$ and $S\in\mathbb{K}[x…

FOS: Computer and information sciencesMathematics - Differential GeometryComputer Science - Symbolic ComputationPure mathematicsMathematics::Commutative Algebra010102 general mathematics68W30Field (mathematics)010103 numerical & computational mathematicsFunction (mathematics)[MATH] Mathematics [math]Symbolic Computation (cs.SC)16. Peace & justiceFunctional decomposition01 natural sciencesDifferential Geometry (math.DG)FOS: MathematicsComputer Science::Symbolic Computation0101 mathematics[MATH]Mathematics [math]Symbolic integrationMathematics
researchProduct

Integrability and non integrability of some n body problems

2015

We prove the non integrability of the colinear $3$ and $4$ body problem, for any masses positive masses. To deal with resistant cases, we present strong integrability criterions for $3$ dimensional homogeneous potentials of degree $-1$, and prove that such cases cannot appear in the $4$ body problem. Following the same strategy, we present a simple proof of non integrability for the planar $n$ body problem. Eventually, we present some integrable cases of the $n$ body problem restricted to some invariant vector spaces.

FOS: MathematicsDynamical Systems (math.DS)Mathematics - Dynamical Systems37J30 37J35
researchProduct