2009
DOI: 10.1142/s0129167x09005261
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Orbital Approach to Microstate Free Entropy

Abstract: Motivated by Voiculescu's liberation theory, we introduce the orbital free entropy χ orb for non-commutative self-adjoint random variables (also for "hyperfinite random multivariables"). Besides its basic properties, the relation of χ orb with the usual free entropy χ is shown. Moreover, the dimension counterpart δ 0,orb of χ orb is discussed, and we obtain the relation between δ 0,orb and the original free entropy dimension δ 0 together with applications to δ 0 itself. Throughout this section, let (M, τ) be a… Show more

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Cited by 19 publications
(56 citation statements)
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“…Arguing as in Lemma 4.2 of [20], we may find a m ′ ∈ N, γ ′ > 0 and a finite G 0 ⊆ Y so that Γ RX ∨RY (F : G 0 ; m ′ , γ ′′ , k) is contained in the unitary conjugation orbit of Ξ (A k ),RX ∨RY (F : G; m, γ, k).…”
Section: Appendix a Properties Of 1-bounded Entropymentioning
confidence: 99%
“…Arguing as in Lemma 4.2 of [20], we may find a m ′ ∈ N, γ ′ > 0 and a finite G 0 ⊆ Y so that Γ RX ∨RY (F : G 0 ; m ′ , γ ′′ , k) is contained in the unitary conjugation orbit of Ξ (A k ),RX ∨RY (F : G; m, γ, k).…”
Section: Appendix a Properties Of 1-bounded Entropymentioning
confidence: 99%
“…However, we will give more 'exact' proofs to them later for the sake of completeness. In fact, (8) and (10) imply that lim N →∞…”
Section: Convergence Of Conditional Expectationmentioning
confidence: 99%
“…Thus, t 0 s∂ s [H(s, φ s (z))]ds is a continuous function of z on V t as consequence of the theorem of continuity under integral sign. It follows from (4.2) that H(t, φ t (z)) extends continuously 6 to V t ∩ T. Now, the identity K(t, φ t (z)) = K(0, z), implies that H(t, φ t (z)) rewrites as…”
Section: Proof Of the Main Resultsmentioning
confidence: 98%