English

Poisson boundary on full Fock space

Operator Algebras 2022-02-17 v2 Functional Analysis

Abstract

This article is devoted to studying the non-commutative Poisson boundary associated with (B(F(H)),Pω)\Big(B\big(\mathcal{F}(\mathcal{H})\big), P_{\omega}\Big) where H\mathcal{H} is a separable Hilbert space (finite or infinite-dimensional), dimH>1\dim \mathcal{H} > 1, with an orthonormal basis E\mathcal{E}, B(F(H))B\big(\mathcal{F}(\mathcal{H})\big) is the algebra of bounded linear operators on the full Fock space F(H)\mathcal{F}(\mathcal{H}) defined over H\mathcal{H}, ω={ωe:eE}\omega = \{\omega_e : e \in \mathcal{E} \} is a sequence of positive real numbers such that eωe=1\sum_e \omega_e = 1 and PωP_{\omega} is the Markov operator on B(F(H))B\big(\mathcal{F}(\mathcal{H})\big) defined by \begin{align*} P_{\omega}(x) = \sum_{e \in \mathcal{E}} \omega_e l_e^* x l_e, \ x \in B\big(\mathcal{F}(\mathcal{H})\big), \end{align*} where, for eEe \in \mathcal{E}, lel_e denotes the left creation operator associated with ee. The non-commutative Poisson boundary associated with (B(F(H)),Pω)\Big(B\big(\mathcal{F}(\mathcal{H})\big), P_{\omega}\Big) turns out to be an injective factor of type IIIIII for any choice of ω\omega. Moreover, if H\mathcal{H} is finite-dimensional, we completely classify the Poisson boundary in terms of its Connes SS-invarinat and curiously they are type IIIλIII _{\lambda } factors with λ\lambda belonging to a certain small class of algebraic numbers.

Cite

@article{arxiv.2109.02010,
  title  = {Poisson boundary on full Fock space},
  author = {B. V. Rajarama Bhat and Panchugopal Bikram and Sandipan De and Narayan Rakshit},
  journal= {arXiv preprint arXiv:2109.02010},
  year   = {2022}
}

Comments

Substantial revision has been made, proofs of some results are rewritten, one section is removed. To appear in Trans. Amer. Math. Soc

R2 v1 2026-06-24T05:41:25.624Z