Lagrangian multiforms on coadjoint orbits for finite-dimensional integrable systems
arXiv:2307.07339 · doi:10.1007/s11005-023-01766-9
Abstract
Lagrangian multiforms provide a variational framework to describe integrable hierarchies. The case of Lagrangian -forms covers finite-dimensional integrable systems. We use the theory of Lie dialgebras introduced by Semenov-Tian-Shansky to construct a Lagrangian -form. Given a Lie dialgebra associated with a Lie algebra and a collection , , of invariant functions on , we give a formula for a Lagrangian multiform describing the commuting flows for on a coadjoint orbit in . We show that the Euler-Lagrange equations for our multiform produce the set of compatible equations in Lax form associated with the underlying -matrix of the Lie dialgebra. We establish a structural result which relates the closure relation for our multiform to the Poisson involutivity of the Hamiltonians and the so-called ``double zero'' on the Euler-Lagrange equations. The construction is extended to a general coadjoint orbit by using reduction from the free motion of the cotangent bundle of a Lie group. We illustrate the dialgebra construction of a Lagrangian multiform with the open Toda chain and the rational Gaudin model. The open Toda chain is built using two different Lie dialgebra structures on . The first one possesses a non-skew-symmetric -matrix and falls within the Adler-Kostant-Symes scheme. The second one possesses a skew-symmetric -matrix. In both cases, the connection with the well-known descriptions of the chain in Flaschka and canonical coordinates is provided.
arXiv commentAuthors' accepted version, to appear in Lett. Math. Phys. New section 4 added about reduction, corrected typos and references added. 42 pages
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