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Finite-index extremal II1 subfactor data

Definition

Assume AC. A II1 factor is a von Neumann algebra A with center C1, no nonzero minimal projections, and a faithful normal normalized trace τA, with the operator and trace conventions of Von Neumann algebras and commutants and States, tracial states and faithful normal traces on a von Neumann algebra. A II1 subfactor inclusion is a unital inclusion N⊆M of II1 factors, with τN=τM∣N. Its trace-preserving normal faithful conditional expectation EN:M→N is the unique expectation constructed in Tracial standard form, normal functional vectors, and expectation; it is positive, unital, N-bimodular, and the restriction of the orthogonal projection eN:L2(M)→L2(N).

A normal right Hilbert-space N-module is a Hilbert space with a unital star representation of Nop that is WOT-continuous on the operator-norm unit ball. This is the topological normality convention of the trace definition above. Right multiplication is Ra(x)=xa, so RaRb=Rba. The amplification theorem Ordinary Hilbert-module dimension and finite projection models constructs a right-module unitary H≅P(ℓ2(I)⊗L2(N)) and its model-independent canonical semifinite trace on End⁡N(H), given in that model by Tr⁡H(T)=∑i∈IτN(Tii) for positive T. Define dim⁡NH=Tr⁡H(1); in particular dim⁡NL2(N)=1. The ordinary Jones index of the inclusion is [M:N]=dim⁡NL2(M,τM)=:λ. The inclusion has finite index when λ<∞. No finite bounded frame or complete N-valued module model is part of this hypothesis.

For finite index, put B=End⁡NL2(M) and τB=λ−1Tr⁡L2(M). Let J(x)=x∗ on L2(M), so Ra=JLa∗J. The inclusion is extremal when τB(Ra)=τM(a)(a∈N′∩M). Here N′∩M={a∈M:an=na for every n∈N}, and Ra belongs to B for these a. Equivalently, the normalized trace on the commutant of the left N action and τM agree on N′∩M, transported by J. This specifies the right-action trace: the normalized trace of B on the left action of M agrees automatically with τM and does not define extremality.

For later calculations write X=M with N-valued inner product ⟨x,y⟩N=EN(x∗y) and norm ∥x∥X=∥EN(x∗x)∥1/2. Its completeness, finite projection model X≅pNk, and bounded coordinate frame are consequences proved below from ordinary finite index; they are not additional assumptions. No separability or irreducibility hypothesis is imposed.

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