2016
DOI: 10.1134/s1560354716030072
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Multi-particle dynamical systems and polynomials

Abstract: Polynomial dynamical systems describing interacting particles in the plane are studied. A method replacing integration of a polynomial multi-particle dynamical system by finding polynomial solutions of a partial differential equations is described. The method enables one to integrate a wide class of polynomial multi-particle dynamical systems. The general solutions of certain dynamical systems related to linear second-order partial differential equations are found. As a by-product of our results, new families … Show more

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Cited by 8 publications
(6 citation statements)
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References 44 publications
(85 reference statements)
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“…Exceptional polynomials appear in a number of applications in mathematical physics, mostly as solutions to exactly solvable quantum mechanical problems describing bound states [25,45,49]. They appear also in connection with super-integrable systems [38,48], exact solutions to Dirac's equation [50], diffusion equations and random processes [32], finite-gap potentials [31] and point vortex models [34].…”
Section: Application To Exceptional Hermite Polynomialsmentioning
confidence: 99%
“…Exceptional polynomials appear in a number of applications in mathematical physics, mostly as solutions to exactly solvable quantum mechanical problems describing bound states [25,45,49]. They appear also in connection with super-integrable systems [38,48], exact solutions to Dirac's equation [50], diffusion equations and random processes [32], finite-gap potentials [31] and point vortex models [34].…”
Section: Application To Exceptional Hermite Polynomialsmentioning
confidence: 99%
“…Moreover, comparing (2.17) with (2.5) and (2.16) we conclude that the zeros of consecutive Adler-Moser polynomials are stationary configurations (or equivalently, μ = (μ 1 , μ 2 ) defined in (2.13) is a critical vector measure) for the vector energy E ϕ,a ( μ) defined in (2.14), with ϕ ≡ (0, 0) and a = − 1 2 , fact that was already observed in [17]. Further generalizations of these ideas, and in particular, their relation to rational solutions of Painlevé equations, can be found in [15,16,30,34,35,37,38,57,62,78], to cite a few.…”
Section: Definition 22mentioning
confidence: 73%
“…Note that if r = 0 then the partition λ(0) = ∅ which has only 0 parts, and when r = m the last multi-index in the lexicographic order, λ(m) = λ. Note that the index sets (03) and ( 12) are incomparable although both (03) ( 13), (12) (13). The partitions λ(r) corresponding to r = (r 1 r 2 ) are given by λ((01)) = (0, 0) = ∅, λ((02)) = (0, 1), λ((03)) = (0, 2), λ(( 12)) = (1, 1), λ(( 13)) = (1, 2), and λ(( 23)) = (2, 2).…”
Section: Definition 31 (Partition)mentioning
confidence: 99%