Weak KAM for commuting Hamiltonians
arXiv:0911.3739 · doi:10.1088/0951-7715/23/4/002
Abstract
For two commuting Tonelli Hamiltonians, we recover the commutation of the Lax-Oleinik semi-groups, a result of Barles and Tourin ([BT01]), using a direct geometrical method (Stoke's theorem). We also obtain a "generalization" of a theorem of Maderna ([Mad02]). More precisely, we prove that if the phase space is the cotangent of a compact manifold then the weak KAM solutions (or viscosity solutions of the critical stationary Hamilton-Jacobi equation) for G and for H are the same. As a corrolary we obtain the equality of the Aubry sets, of the Peierls barrier and of flat parts of Mather's functions. This is also related to works of Sorrentino ([Sor09]) and Bernard ([Ber07b]).
23 pages, accepted for publication in NonLinearity (january 29th 2010). Minor corrections, fifth part added on Mather's function (or effective Hamiltonian)
References in corpus (3)
Cited by in corpus (5)
- Aubry sets for weakly coupled systems of Hamilton--Jacobi equations
- On the (non) existence of viscosity solutions of multi-time Hamilton-Jacobi equations
- On commuting Tonelli Hamiltonians: Time-periodic case
- Weak KAM theoretic aspects for nonregular commuting Hamiltonians
- On commuting Tonelli Hamiltonians: Autonomous case