Liberation, free mutual information and orbital free entropy

preprint2017arXivOpen access

Abstract

We present here some connections between the liberation process for projections (P,Q)↦(P,UtQUt∗)(P,Q)\mapsto(P,U_tQU_t^*) and its counterpart (R,S)↦(R,UtSUt∗)(R,S)\mapsto(R,U_tSU_t^*) for symmetries when the projections {P,Q}\{P,Q\} and the symmetries {R,S}\{R,S\} are associated, where UtU_t is a free unitary Brownian motion freely independent from {P,Q}\{P,Q\} (and so {R,S}\{R,S\}). We relate the moments of their actions on the operators Xt:=PUtQUt∗X_t:=PU_tQU_t^* and Yt:=UtRUt∗SY_t:=U_tRU_t^*S and use this to prove a relationship between the corresponding spectral measures (hereafter μtμ_t and νtν_t). On the other hand, we focus in the process of unitary random variables YtY_t in the case of arbitrary trace values τ(R),τ(S)τ(R),τ(S). More precisely, we use stochastic calculus to derive a partial differential equation (PDE for short) for its Herglotz transform and use it to develop subordination results in terms of Löwner equations. The paper is closed with an improved proof of i∗(CP+C(I−P);CQ+C(I−Q))=−χorb(P,Q)i^*\left( \mathbb{C}P+\mathbb{C}(I-P); \mathbb{C}Q+\mathbb{C}(I-Q) \right)=-χ_{orb}\left(P,Q\right) as an application.

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