Meixner class of orthogonal polynomials of a non-commutative monotone Levy noise
Abstract
Let (Xt)t0 denote a non-commutative monotone L\'evy process. Let ω=(ω(t))t0 denote the corresponding monotone L\'evy noise.. A continuous polynomial of ω is an element of the corresponding non-commutative L2-space L2(τ) that has the form Σi=0n ω i,f(i), where f(i)∈ C0( R+i). We denote by CP the space of all continuous polynomials of ω. For f(n)∈ C0( R+n), the orthogonal polynomial P(n)(ω),f(n) is defined as the orthogonal projection of the monomial ω n,f(n) onto the subspace of L2(τ) that is orthogonal to all continuous polynomials of ω of order n-1. We denote by OCP the linear span of the orthogonal polynomials. Each orthogonal polynomial P(n)(ω),f(n) depends only on the restriction of the function f(n) to the set \(t1,…,tn)∈ R+n t1 t2… tn\. The orthogonal polynomials allow us to construct a unitary operator J:L2(τ) F, where F is an extended monotone Fock space. Thus, we may think of the monotone noise ω as a distribution of linear operators acting in F. We say that the orthogonal polynomials belong to the Meixner class if CP=OCP. We prove that each system of orthogonal polynomials from the Meixner class is characterized by two parameters: λ∈ R and η0. In this case, the monotone L\'evy noise has the representation ω(t)=∂t+λ∂t∂t+∂t+η∂t∂t∂t. Here, ∂t and ∂t are the (formal) creation and annihilation operators at t∈ R+ acting in F.