<p>The geometric theory of pseudo-differential and Fourier integral operators relies on the symplectic structure of cotangent bundles. If one is to study calculi with some specific feature adapted to a geometric situation, the corresponding notion of cotangent bundle needs to be adapted as well, and leads to spaces with a singular symplectic structure. Analysing these singularities is a necessary step in order to construct the calculus itself.</p><p>In this article we provide some new insights into the symplectic structures arising from asymptotically Euclidean manifolds. In particular, we study the action of the Poisson brackets on <i>SG</i>-pseudo-differential operators and define a new class of singular symplectomorphisms, taking into account the geometric picture. We then consider this notion in the context of the characterisation of order-preserving isomorphisms of the <i>SG</i>-algebra, and show that these are in fact given by conjugation with a Fourier integral operator of <i>SG</i>-type.</p>

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Canonical transformations near infinity and isomorphisms of SG-pseudo-differential operators

  • Alessandro Pietro Contini

摘要

The geometric theory of pseudo-differential and Fourier integral operators relies on the symplectic structure of cotangent bundles. If one is to study calculi with some specific feature adapted to a geometric situation, the corresponding notion of cotangent bundle needs to be adapted as well, and leads to spaces with a singular symplectic structure. Analysing these singularities is a necessary step in order to construct the calculus itself.

In this article we provide some new insights into the symplectic structures arising from asymptotically Euclidean manifolds. In particular, we study the action of the Poisson brackets on SG-pseudo-differential operators and define a new class of singular symplectomorphisms, taking into account the geometric picture. We then consider this notion in the context of the characterisation of order-preserving isomorphisms of the SG-algebra, and show that these are in fact given by conjugation with a Fourier integral operator of SG-type.