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The Liouville theorem for a class of Fourier multipliers and its connection to coupling

David Berger, René L. Schilling, Eugene Shargorodsky

Abstract

The classical Liouville property says that all bounded harmonic functions in $\mathbb{R}^n$, i.e.\ all bounded functions satisfying $Δf = 0$, are constant. In this paper we obtain necessary and sufficient conditions on the symbol of a Fourier multiplier operator $m(D)$, such that the solutions $f$ to $m(D)f=0$ are Lebesgue a.e.\ constant (if $f$ is bounded) or coincide Lebesgue a.e.\ with a polynomial (if $f$ grows like a polynomial). The class of Fourier multipliers includes the (in general non-local) generators of Lévy processes. For generators of Lévy processes we obtain necessary and sufficient conditions for a strong Liouville theorem where $f$ is positive and grows at most exponentially fast. As an application of our results above we prove a coupling result for space-time Lévy processes.

The Liouville theorem for a class of Fourier multipliers and its connection to coupling

Abstract

The classical Liouville property says that all bounded harmonic functions in , i.e.\ all bounded functions satisfying , are constant. In this paper we obtain necessary and sufficient conditions on the symbol of a Fourier multiplier operator , such that the solutions to are Lebesgue a.e.\ constant (if is bounded) or coincide Lebesgue a.e.\ with a polynomial (if grows like a polynomial). The class of Fourier multipliers includes the (in general non-local) generators of Lévy processes. For generators of Lévy processes we obtain necessary and sufficient conditions for a strong Liouville theorem where is positive and grows at most exponentially fast. As an application of our results above we prove a coupling result for space-time Lévy processes.
Paper Structure (5 sections, 14 theorems, 71 equations)

This paper contains 5 sections, 14 theorems, 71 equations.

Key Result

Theorem 1

Let $\psi$ be the characteristic exponent of a Lévy process and denote by $\psi(D)$ the corresponding Fourier multiplier operator. Suppose $f \in L^\infty(\mathds{R}^n)$ is such that $\psi(D)f=0$ as a distribution, i.e. If $\left\{\eta \in \mathds{R}^n \mid \psi(\eta) = 0\right\} = \{0\}$, then $f \equiv \textrm{const}$ Lebesgue almost everywhere. Conversely, if $f \equiv \textrm{const}$ Lebesgu

Theorems & Definitions (33)

  • Theorem 1: Liouville; Ali-et-al20, BS21
  • Theorem 2
  • proof : Proof of Liouville's Theorem \ref{['th:1.1']}
  • Remark 3
  • Theorem 4
  • Remark 5
  • Example 6
  • Theorem 7
  • proof
  • Theorem 8: Liouville property for polynomially bounded functions
  • ...and 23 more