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Spectral theory for Lévy and Lévy-Ornstein-Uhlenbeck semigroups on step 2 Carnot groups

Maria Gordina, Rohan Sarkar

Abstract

We consider non-local perturbations $Δ^ψ_G$ of sub-Laplacians on a step $2$ Carnot group $G$. The perturbations are by translation-invariant non-local operators acting along the vertical directions in $G$. We use harmonic analysis on $G$ to obtain intertwining relationship between the semigroups generated by $Δ^ψ_G$ and some strongly continuous contraction semigroups on Euclidean spaces with purely continuous spectrum, and as a result we identify the spectrum of $Δ^ψ_G$. Further we introduce the Lévy-Ornstein-Uhlenbeck (OU) semigroup corresponding to $Δ^ψ_G$. We prove that these Markov semigroups are ergodic, though they are not normal operators on $L^2$ space with respect to the invariant distribution $\mathsf{p}_ψ$. The intertwining relationships allow us to show that all Lévy-OU generators on $G$ are isospectral, that is, they have the same eigenvalues with the same multiplicities. As a byproduct, we obtain a precise description of the eigenspaces, and also derive explicit formula for the co-eigenfunctions corresponding to some eigenvalues.

Spectral theory for Lévy and Lévy-Ornstein-Uhlenbeck semigroups on step 2 Carnot groups

Abstract

We consider non-local perturbations of sub-Laplacians on a step Carnot group . The perturbations are by translation-invariant non-local operators acting along the vertical directions in . We use harmonic analysis on to obtain intertwining relationship between the semigroups generated by and some strongly continuous contraction semigroups on Euclidean spaces with purely continuous spectrum, and as a result we identify the spectrum of . Further we introduce the Lévy-Ornstein-Uhlenbeck (OU) semigroup corresponding to . We prove that these Markov semigroups are ergodic, though they are not normal operators on space with respect to the invariant distribution . The intertwining relationships allow us to show that all Lévy-OU generators on are isospectral, that is, they have the same eigenvalues with the same multiplicities. As a byproduct, we obtain a precise description of the eigenspaces, and also derive explicit formula for the co-eigenfunctions corresponding to some eigenvalues.

Paper Structure

This paper contains 21 sections, 48 theorems, 293 equations.

Key Result

Proposition 3.2

For all $f\in L^1(G)\cap L^2(G)$ we have

Theorems & Definitions (97)

  • Proposition 3.2: Plancherel's theorem
  • Lemma 3.4
  • proof
  • Definition 3.5: Weyl transform
  • Remark 3.6
  • Proposition 3.7
  • proof
  • Lemma 3.9
  • proof
  • Proposition 3.10
  • ...and 87 more