Partial quasi-morphisms and quasi-states on cotangent bundles, and symplectic homogenization
By Alexandra Monzner, Nicolas Vichery, F. Zapolsky. 2011
72 citations recorded by the source corpus.
For a closed connected manifold N, we construct a family of functions on the Hamiltonian group G of the cotangent bundle T^*N, and a family of functions on the space of smooth functions with compact support on T^*N. These satisfy properties analogous to those of partial quasi-morphisms and quasi-states of Entov and Polterovich. The families are parametrized by the first real cohomology of N. In the case N=T^n the family of functions on G coincides with Viterbo's symplectic homogenization operator. These functions have applications to the algebraic and geometric structure of G, to Aubry-Mather theory, to restrictions on Poisson brackets, and to symplectic rigidity.
Subfields: Geometry and Topology, Mathematical Physics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/32007bf2b05f369aedbae83aba2979bee2358a2f
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Citations in the corpus
- Coisotropic rigidity and $C^{0}$-symplectic geometry (2013, methodology): “otangent bundles. We briefly outline below the construction of these invariants via Lagrangian Floer homology and collect their main properties in this situation. We refer to Monzner– Vichery–Zapolsky [18] which gives a very nice exposition of the theory. Let Lbe a smooth compact manifold, L 0 denote”
- On the Homogenization of the Hamilton-Jacobi Equation (2019, methodology): “used by different communities with different meanings; in this work, we refer to our result as a “Homogenization result for the Hamilton-Jacobi equation”, in the same spirit as it is done in [9], [33], [27], etc. In the remaing part of this introduction, in order to present our main result, we need to”
- Bounds on spectral norms and barcodes (2018, background): “ology by Viterbo in [118] by means of generating functions, then in Floer theory by Schwarz [97], and Oh [84, 85], and in Lagrangian Floer theory by Leclercq [64] and Leclercq-Zapolsky [65] (see also [44, 77, 81]). We refer to [65] for a review of the literature. In terms of Lagrangian (resp. Hamilt”