Abstract

Tulczyjew's triples are constructed for the Schmidt-Legendre transformations of both second and third-order Lagrangians. Symplectic diffeomorphisms relating the Ostrogradsky-Legendre and the Schmidt-Legendre transformations are derived. Several examples are presented.

Highlights

  • A geometrization of Schmidt-Legendre transformation of the higher order Lagrangians is proposed by building a proper Tulczyjew’s triplet

  • The dynamics of a system can either be formulated by a Lagrangian function on the tangent bundle of a configuration space or by a Hamiltonian function on the cotangent bundle [1, 4]

  • At the late 70’s, Tulczyjew showed that the dynamics can be represented as a Lagrangian submanifold of certain symplectic manifold on higher order bundles [7, 56, 57, 61, 62]

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Summary

Introduction

The dynamics of a system can either be formulated by a Lagrangian function on the tangent bundle of a configuration space or by a Hamiltonian function on the cotangent bundle [1, 4]. In classical mechanics a Lagrangian density is a function of positions and velocities, it is possible to find theories involving Lagrangian densities depending on the higher order derivatives as well. In such cases, to pass the Hamiltonian picture, it is a tradition to employ the Ostrogradsky-Legendre transformation [44]. The last section, will be reserved for several examples including Pais-Uhlenberg, Sarıoglu-Tekin and Clement Lagrangians

Special symplectic structures
Morse Families
The Legendre transformation
Higher order tangent bundles
Higher order Euler-Lagrange equations
Ostrogradsky-Legendre transformation
Acceleration bundle
Higher order acceleration bundles
Gauge symmetry of second order Lagrangian formalisms
Schmidt-Legendre transformation for even orders
Schmidt-Legendre transformation for odd orders
For even order formalisms
For the odd order formalisms
Example 1
Example 2
Example 3
Example 4
Example 5
Full Text
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