2014
DOI: 10.1215/21562261-2693451
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On the eigenfunctions of the complex Ornstein–Uhlenbeck operators

Abstract: Starting from the 1-dimensional complex-valued Ornstein-Uhlenbeck process, we present two natural ways to imply the associated eigenfunctions of the 2-dimensional normal Ornstein-Uhlenbeck operators in the complex Hilbert space L 2 C (µ). We call the eigenfunctions Hermite-Laguerre-Ito polynomials. In addition, the Mehler summation formula for the complex process are shown. MSC: 60H10,60H07,60G15.

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Cited by 18 publications
(21 citation statements)
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“…The following proposition gives an integration by parts formula of complex Gaussian random variables, whose proof is straight forward. Please refer to Lemma 3.2 of [5] or Lemma 2.3 of [2]. Proposition 2.2 (integration by parts formula).…”
Section: Preliminaries: Concise Complex Malliavin Calculusmentioning
confidence: 99%
See 1 more Smart Citation
“…The following proposition gives an integration by parts formula of complex Gaussian random variables, whose proof is straight forward. Please refer to Lemma 3.2 of [5] or Lemma 2.3 of [2]. Proposition 2.2 (integration by parts formula).…”
Section: Preliminaries: Concise Complex Malliavin Calculusmentioning
confidence: 99%
“…We define the divergence operators δ andδ as the adjoint of D andD respectively, with the domains Dom(δ) and Dom(δ) the subsets of L 2 (Ω, H) composed of those elements u such that there exists a constant c > 0 verifying for all F ∈ S, Proof. First, we claim that a complex Hermite polynomials J m,n (z, ρ) [7,5] satisfies that 1) partial derivatives:…”
Section: Preliminaries: Concise Complex Malliavin Calculusmentioning
confidence: 99%
“…Especially, when x is a complex Brownian motion, the right hand side of the above equality is equal to the complex multiple Wiener-Itô integral: [9] t 0 t 0 · · · t 0 dx t1 · · · dx tm dx tm+1 · · · dx tm+n .…”
Section: Complex Wiener-itô Multiple Integrals and Chaos Decompositionmentioning
confidence: 99%
“…− e iθ z ∂ ∂z − e −iθz ∂ ∂z , (1.2) where θ ∈ (− π 2 , π 2 ) is fixed and ∂f ∂z = 1 2 ( ∂f ∂x − i ∂f ∂y ), ∂f ∂z = 1 2 ( ∂f ∂x + i ∂f ∂y ) are the Wirtinger derivatives of f at point z = x + iy with x, y ∈ R. In [8], it is shown that the eigenfunctions are the complex Hermite polynomials and form an orthonormal basis of L 2 (γ) where dγ = 1 2π e − x 2 +y 2 2 dxdy (see Proposition 2.2 below). In this paper, we will firstly show thatL θ can be realized as an unbounded normal operator (see [19, p. 368]) in L 2 (γ) but nonsymmetric when θ ̸ = 0.…”
Section: Introductionmentioning
confidence: 99%