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Related papers: On the four-body lima\c{c}on choreography: maximal…

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For one 3-body and two 5-body planar choreographies on the same algebraic Lemniscate by Bernoulli we found explicitly a maximal possible set of (particular) Liouville integrals, 7 and 15, respectively, (including the total angular…

Classical Physics · Physics 2021-10-14 Alexander V. Turbiner , Juan Carlos Lopez Vieyra

In a remarkable paper of 2003 by Fujiwara et al. \cite{Fujiwara2003}, a figure-eight three-body choreography on the algebraic lemniscate by Bernoulli was discovered. Such a choreography was found to be driven by the action of a pairwise…

Mathematical Physics · Physics 2019-05-22 Juan Carlos Lopez Vieyra

We analyze planar $n$-body Hamiltonian systems with quadratic $D_n$-invariant interactions and identify the symmetry obstruction to choreographic motion. Choreographies are taken throughout to be collision-free solutions of the equations of…

Mathematical Physics · Physics 2026-05-01 A M Escobar-Ruiz , M Fernandez-Guasti

The Lie-Poisson algebra so(N+1) and some of its contractions are used to construct a family of superintegrable Hamiltonians on the ND spherical, Euclidean, hyperbolic, Minkowskian and (anti-)de Sitter spaces. We firstly present a…

Mathematical Physics · Physics 2008-11-26 Francisco J. Herranz , Angel Ballesteros

It is found explicitly 5 Liouville integrals in addition to total angular momentum which Poisson commute with Hamiltonian of 3-body Newtonian Gravity in ${\mathbb R}^3$ along the Remarkable Figure-8-shape trajectory discovered by…

Classical Physics · Physics 2020-05-27 Alexander V Turbiner , Juan Carlos Lopez Vieyra

We identify a new superintegrable Hamiltonian in 3 degrees of freedom, obtained as a reduction of pure Keplerian motion in 6 dimensions. The new Hamiltonian is a generalization of the Keplerian one, and has the familiar 1/r potential with…

Exactly Solvable and Integrable Systems · Physics 2009-11-13 P. E. Verrier , N. W. Evans

A family of classical superintegrable Hamiltonians, depending on an arbitrary radial function, which are defined on the 3D spherical, Euclidean and hyperbolic spaces as well as on the (2+1)D anti-de Sitter, Minkowskian and de Sitter…

Mathematical Physics · Physics 2008-04-24 Francisco J. Herranz , Angel Ballesteros

In this work we introduce a planar restricted four-body problem where a massless particle moves under the gravitational influence due to three bodies following the eight figure choreography, and we explore some symmetric periodic orbits of…

Dynamical Systems · Mathematics 2019-10-29 Ricardo Lara , Abimael Bengochea

The superintegrability of four Hamiltonians $\tilde{H_r} = \lambda\, H_r$, $r=a,b,c,d$, where $H_r$ are known Hamiltonians and $\lambda$ is a certain function defined on the configuration space and depending of a parameter $\kappa$, is…

Mathematical Physics · Physics 2020-02-14 Manuel F. Ranada

In general relativity, the motion of an extended body moving in a given spacetime can be described by a particle on a (generally non-geodesic) worldline. In first approximation, this worldline is a geodesic of the underlying spacetime, and…

General Relativity and Quantum Cosmology · Physics 2024-02-05 Paul Ramond

The motion of a rigid body in a quadratic potential is an important example of an integrable Hamiltonian system on a dual to a semidirect product Lie algebra so(n) x Symm(n). We give a Lagrangian derivation of the corresponding equations of…

solv-int · Physics 2007-05-23 Yuri B. Suris

We study four particular 3-dimensional natural Hamiltonian systems defined in conformally Euclidean spaces. We prove their superintegrability and we obtain, in the four cases, the maximal number of functionally independent integrals of…

Mathematical Physics · Physics 2021-09-13 Jose F. Carinena , Manuel F. Ranada , Mariano Santander

The two-dimensional n-body problem of classical mechanics is a non-integrable Hamiltonian system for n > 2. Traditional numerical integration algorithms, which are polynomials in the time step, typically lead to systematic drifts in the…

Computational Physics · Physics 2009-11-07 Oksana Kotovych , John C. Bowman

The superposition of the Kepler-Coulomb potential on the 3D Euclidean space with three centrifugal terms has recently been shown to be maximally superintegrable [Verrier P E and Evans N W 2008 J. Math. Phys. 49 022902] by finding an…

Mathematical Physics · Physics 2015-05-13 Angel Ballesteros , Francisco J. Herranz

We give a construction of completely integrable 4-dimensional Hamiltonian systems with cubic Hamilton functions. Applying to the corresponding pairs of commuting quadratic Hamiltonian vector fields the so called Kahan-Hirota-Kimura…

Exactly Solvable and Integrable Systems · Physics 2017-04-12 Matteo Petrera , Yuri B. Suris

A Hamiltonian with two degrees of freedom is said to be superintegrable if it admits three functionally independent integrals of the motion. This property has been extensively studied in the case of two-dimensional spaces of constant…

Mathematical Physics · Physics 2007-05-23 E. G. Kalnins , J. M. Kress , P. Winternitz

Families of three-body Hamiltonian systems in one dimension have been recently proved to be maximally superintegrable by interpreting them as one-body systems in the three-dimensional Euclidean space, examples are the Calogero, Wolfes and…

Mathematical Physics · Physics 2013-09-03 C. Chanu , L. Degiovanni , G. Rastelli

This paper analyzes the optimal control problem of cubic polynomials on compact Lie groups from a Hamiltonian point of view and its symmetries. The dynamics of the problem is described by a presymplectic formalism associated with the…

Optimization and Control · Mathematics 2015-05-27 L. Abrunheiro , M. Camarinha , J. Clemente-Gallardo

A Hamiltonian system is completely integrable (in the sense of Liouville) if there exist as many independent integrals of motion in involution as the dimension of the configuration space. Under certain regularity conditions,…

Symplectic Geometry · Mathematics 2025-05-26 Leonardo Colombo , Manuel de León , Manuel Lainz , Asier López-Gordón

We use the maximally permutation symmetric set of three-body coordinates, that consist of the "hyper-radius" $R = \sqrt{\rho^{2} + \lambda^{2}}$, the "rescaled area of the triangle" $\frac{\sqrt 3}{2 R^2} |{\bm \rho} \times {\bm \lambda}|$)…

Mathematical Physics · Physics 2015-03-19 Milovan Suvakov , V. Dmitrasinovic
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