A symplectic extension map and a new Shubin class of pseudo-differential operators

preprint2014arXivOpen access

Abstract

For an arbitrary pseudo-differential operator A:S(RA:\mathcal{S}(\mathbb{R}% ^{n})\longrightarrow\mathcal{S}^{\prime}(\mathbb{R}^{n}) with Weyl symbol a∈S′(R2n)a\in\mathcal{S}^{\prime}(\mathbb{R}^{2n}), we consider the pseudo-differential operators A~:S(R\widetilde{A}:\mathcal{S}(\mathbb{R}% ^{n+k})\longrightarrow\mathcal{S}^{\prime}(\mathbb{R}^{n+k}) associated with the Weyl symbols a~=(a⊗12k)∘s\widetilde{a}=(a\otimes1_{2k})\circ{s}, where 12k(x)=11_{2k}(x)=1 for all x∈R2kx\in\mathbb{R}^{2k} and s{s} is a linear symplectomorphism of R2(n+k)\mathbb{R}^{2(n+k)}. We call the operators A~\widetilde{A} symplectic dimensional extensions of AA. In this paper we study the relation between AA and A~\widetilde{A} in detail, in particular their regularity, invertibility and spectral properties. We obtain an explicit formula allowing to express the eigenfunctions of A~\widetilde{A} in terms of those of AA. We use this formalism to construct new classes of pseudo-differential operators, which are extensions of the Shubin classes HGρm1,m0HG_ρ^{m_{1},m_{0}} of globally hypoelliptic operators. We show that the operators in the new classes share the invertibility and spectral properties of the operators in HGρm1,m0HG_{ρ}^{m_{1},m_{0}} but not the global hypoellipticity property. Finally, we study a few examples of operators that belong to the new classes and which are important in mathematical physics.

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