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Related papers: Exact operator solution of the Calogero-Sutherland…

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The three-particle Hamiltonian obtained by replacing the two-body trigonometric potential of the Sutherland problem by a three-body one of a similar form is shown to be exactly solvable. When written in appropriate variables, its…

High Energy Physics - Theory · Physics 2008-02-03 C. Quesne

Exact analytical, closed-form solutions, expressed in terms of special functions, are presented for the case of a three-dimensional nonlinear quantum oscillator with a position dependent mass. This system is the generalization of the…

Mathematical Physics · Physics 2015-06-15 Axel Schulze-Halberg , John R. Morris

Much work has been devoted to the study of nonstrange baryons belonging to the $[\textbf{70},1^-]$ multiplet in the framework of the $1/N_c$ expansion. Using group theoretical arguments here we examine the relation between the exact wave…

High Energy Physics - Phenomenology · Physics 2008-11-26 N. Matagne , Fl. Stancu

We propose the integrable N-dimensional Calogero-Coulomb-Stark and two-center Calogero-Coulomb systems and construct their constants of motion via the Dunkl operators. Their Schr\"odinger equations decouple in parabolic and elliptic…

Mathematical Physics · Physics 2016-02-26 Tigran Hakobyan , Armen Nersessian

It is shown that the Calogero-Moser models based on all root systems of the finite reflection groups (both the crystallographic and non-crystallographic cases) with the rational (with/without a harmonic confining potential), trigonometric…

High Energy Physics - Theory · Physics 2009-10-31 A. J. Bordner , N. S. Manton , R. Sasaki

We calculate the Wigner distribution function for the Calogero-Sutherland system which consists of harmonic and inverse-square interactions. The Wigner distribution function is separated out into two parts corresponding to the relative and…

Quantum Physics · Physics 2007-05-23 A. Tegmen , T. Altanhan , B. S. Kandemir

We demonstrate that the exact form-factors of the Calogero-Sutherland model which were recently found in Ref.[10] in confirmation of the congectures earlier made by Haldane (Ref.[9]) can be reproduced in the framework of some bosonization…

Condensed Matter · Physics 2009-10-22 D. V. Khveshchenko

We introduce two-parameter classes of exactly-solvable novel systems whose Hamiltonian operators could be represented by tridiagonal symmetric matrices in some orthogonal bases. The associated wavefunction is written as point-wise…

Mathematical Physics · Physics 2026-05-28 A. D. Alhaidari

We construct a discrete version of the plane wave solution to a discrete Dirac-K\"{a}hler equation in the Joyce form. A geometric discretisation scheme based on both forward and backward difference operators is used. The conditions under…

Mathematical Physics · Physics 2020-07-02 Volodymyr Sushch

We derive an exact expression for the single particle Green function in the Calogero-Sutherland model for all rational values of the coupling $\beta$. The calculation is based on Jack polynomial techniques and the results are given in the…

High Energy Physics - Theory · Physics 2009-10-28 D. Serban , F. Lesage , V. Pasquier

The angular wave functions for a hydrogen atom are well known to be spherical harmonics, and are obtained as the solutions of a partial differential equation. However, the differential operator is given by the Casimir operator of the…

Quantum Physics · Physics 2017-01-09 Naohisa Ogawa

Exceptional orthogonal polynomials constitute the main part of the bound-state wavefunctions of some solvable quantum potentials, which are rational extensions of well-known shape-invariant ones. The former potentials are most easily built…

Mathematical Physics · Physics 2015-06-23 C. Quesne

A class of exact solutions of the Skyrme model are obtained. They are described by the Weierstrass $\wp$-function or the Jacobi elliptic function. They are not solitonic but of wave character. They supply us with examples of the…

High Energy Physics - Theory · Physics 2009-11-10 M. Hirayama , C. -G. Shi , J. Yamashita

For the models of $N$-body identical harmonic oscillators interacting through potentials of homogeneous degree -2, the unitary operator that transforms a system of time-dependent parameters into that of unit spring constant and unit mass of…

Quantum Physics · Physics 2007-05-23 Dae-Yup Song

Multivariable generalizations of the classical Hermite, Laguerre and Jacobi polynomials occur as the polynomial part of the eigenfunctions of certain Schr\"odinger operators for Calogero-Sutherland-type quantum systems. For the generalized…

solv-int · Physics 2009-10-30 T. H. Baker , P. J. Forrester

Approximation on the spherical cap is different from that on the sphere which requires us to construct new operators. This paper discusses the approximation on the spherical cap. That is, so called Jackson-type operator…

Classical Analysis and ODEs · Mathematics 2014-09-15 Yuguang Wang , Feilong Cao

We define a new multispecies model of Calogero type in D dimensions with harmonic, two-body and three-body interactions. Using the underlying conformal SU(1,1) algebra, we indicate how to find the complete set of the states in Bargmann-Fock…

High Energy Physics - Theory · Physics 2009-11-10 S. Meljanac , M. Milekovic , A. Samsarov

A recent novel derivation of the representation of Virasoro singular vectors in terms of Jack polynomials is extended to the supersymmetric case. The resulting expression of a generic super-Virasoro singular vector is given in terms of a…

Mathematical Physics · Physics 2016-10-12 O. Blondeau-Fournier , P. Mathieu , D. Ridout , S. Wood

We construct the dynamical symmetry of the quantum Calogero model with particle exchange in a confining Coulomb field. This symmetry is governed by the algebra $so(N+1,2)$, deformed by exchange (Dunkl) operators, with its invariant sector…

High Energy Physics - Theory · Physics 2026-05-26 Tigran Hakobyan

Starting from Rodrigues formula we present a general construction of raising and lowering operators for orthogonal polynomials of continuous and discrete variable on uniform lattice. In order to have these operators mutually adjoint we…

Mathematical Physics · Physics 2009-11-10 M. Lorente