The Hamiltonian structure of integrable PDEs

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speaker: Matteo Casati

 tme:  Part 1: 2025.1.15, 13:30-16:00

          Part 2: 2025.1.16, 14:00-16:00

 place: Yifu Building 1417

 Abstract

One of the several different notions of integrability for systems of PDEs is the so-called Liouville integrability, namely the existence of a suitable number of conserved quantities during the evolution of a system. Such a notion is analogue to the one of integrability for finite-dimensional systems, and it is bases on the Lie algebra defined by the Poisson bracket, which constitutes the Hamiltonian structure of the system.

I will review the notion of Poisson structures (in some contexts called Hamiltonian operators) focusing on systems of PDEs, showing their relation with the integrability of the system (bi-Hamiltonian pairs, recursion operators..) and underlying their common features

One crucial feature of Poisson brackets for integrable PDEs is that they can be regarded as differential-geometrical objects on the space of functions between two manifolds and that their existence is constrained by the structure of the so-called “target manifold”. I will review the geometry of the Poisson brackets of hydrodynamic type defined by Dubrovin and Novikov and show how to naturally extend the notion to brackets defined by higher order and/or multidimensional differential operators. The case of weakly non-local Poisson structures of first and third order will be discussed too. Finally, I will present the first results of a joint project with G. Carlet about the structure of differential-geometric Poisson brackets of arbitrary order.

 

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