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We make use of the Maupertuis – Jacobi correspondence, well known in Classical Mechanics, to simplify 2-D asymptotic formulas based on Maslov’s canonical operator, when constructing Lagrangian manifolds invariant with respect to phase flows for Hamiltonians of the form . As examples we consider Hamiltonians coming from the Schr"odinger equation, the 2-D Dirac equation for graphene and linear water wave theory.

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