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added pointer to today’s:
In this paper we construct a unitary matrix model that captures the asymptotic growth of Young diagrams under q-deformed Plancherel measure.
added statement of
limn→∞pPl({λ∈Part(n)|2√nln|sYTableauxλ|√n!−c<ε})=1.from
Added an actual definition:
From a MathOverflow answer by Vadim Alekseev:
Suppose G is a locally compact group. What one ultimately wants to study is (upon fixing a Haar measure in the noncompact case) the left regular representation λ:G→U(L2(G,Haar)). Now, general theory tells us that while it’s not always possible to decompose L2(G) as a direct sum of irreducible reprenentations (this already fails for ), it is always possible to decompose it as a direct integral of irreducible representations (which are parametrised by the unitary dual ˆG of G). Now, if G is unimodular and type I, the direct integral decomposition (with respect to both left and right actions of G) is as follows:
L2(G)≅∫ˆGHπdμ(π),where Hπ=π⊗π*, and its understanding requires, in particular, to determine the measure μ on ˆG such that the above becomes an isometric isomorphism. The unique measure with this property is called the Plancherel measure of G (associated to a given Haar measure). Equivalently, it’s the unique measure such that
‖f‖22=∫ˆG‖π(f)‖2HSdμ(π),f∈L1(G,Haar)∩L2(G,Haar).And another one:
From a MathOverflow answer by Cameron Zwarich:
If G is a unimodular second countable Type I group, then the Plancherel measure is the unique measure μ such that
‖f‖22=∫ˆG‖π(f)‖2HSdμ(π).for every f∈L1(G)∩L2(G). This appears as Theorem 18.8.2 in Dixmier’s book on C*-algebras.
When G is not unimodular, the question becomes more complicated, because the Plancherel measure needs to be twisted by a section of a line bundle; see the paper of Duflo-Moore on the subject for the gory details. When G is not second countable, I do not know of a published result; the technical details of direct integral theory are more difficult in this case and not standard. When G is not Type I, the decomposition of the left regular representation into irreducibles is no longer unique, and some of the operators on the right-hand side of the formula will fail to have finite Hilbert-Schmidt norm.
The closest analogue to the definition of a Haar measure on abelian locally compact groups as a left-invariant Radon measure is the characterization of the Plancherel measure as a unique co-invariant trace (or weight) on the von Neumann algebra ℳ generated by the left-regular representation of G. Suppose G satisfies the same hypotheses as above and Δ:ℳ→ℳˉ⊗ℳ is the comultiplication on ℳ given by λ(s)↦λ(s)⊗λ(s). Then the Plancherel trace is the unique normal semifinite trace τ on ℳ such that
τ((φ⊗id)(Δ(a)))=τ(a)for all a∈ℳ+τ and φ∈ℳ*. A similar characterization holds for the Plancherel weight of an arbitrary locally compact group, or for the Haar weight of a locally compact quantum group. For proofs, see volume 2 of Takesaki or any of the literature on von Neumann algebraic quantum groups.
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