16c. Basic examples
Let us discuss now some basic examples of subfactors, with concrete illustrations for all the above notions, constructions, and general theory. These examples will all come from group actions [math]G\curvearrowright Q[/math], which are assumed to be minimal, in the sense that:
As a starting point, we have the following result, due to Jones [1]:
Assuming that [math]G[/math] is a compact group, acting minimally on a [math]{\rm II}_1[/math] factor [math]Q[/math], and that [math]H\subset G[/math] is a subgroup of finite index, we have a subfactor
This is something standard, the idea being that the factoriality of [math]Q^G,Q^H[/math] comes from the minimality of the action, and that the index formula is clear.
Along the same lines, we have the following result, due to Ocneanu [2]:
Assuming that [math]G[/math] is a finite group, acting minimally on a [math]{\rm II}_1[/math] factor [math]Q[/math], we have a subfactor as follows,
This is standard as well, the idea being that the factoriality of [math]Q\rtimes G[/math] comes from the minimality of the action, and that the index formula is clear.
We have as well a third result of the same type, due to Wassermann [3], namely:
Assuming that [math]G[/math] is a compact group, acting minimally on a [math]{\rm II}_1[/math] factor [math]Q[/math], and that [math]G\to PU_n[/math] is a projective representation, we have a subfactor
As before, the idea is that the factoriality of [math]Q^G,(M_n(\mathbb C)\otimes Q)^G[/math] comes from the minimality of the action, and the index formula is clear.
The above subfactors look quite related, and indeed they are, due to:
The Jones, Ocneanu and Wassermann subfactors are all of the same nature, and can be written as follows,
This is something standard, from [4], modulo several standard identifications. We will explain all this more in detail later, after unifying these subfactors.
In order to unify now the above constructions of subfactors, following [4], [3], the idea is quite clear. Given a compact group [math]G[/math], acting minimally on a [math]{\rm II}_1[/math] factor [math]Q[/math], and an inclusion of finite dimensional algebras [math]B_0\subset B_1[/math], endowed as well with an action of [math]G[/math], we would like to construct a kind of generalized Wassermann subfactor, as follows:
In order to do this, we must talk first about the finite dimensional algebras [math]B[/math], and about inclusions of such algebras [math]B_0\subset B_1[/math]. Let us start with the following definition:
Associated to any finite dimensional algebra [math]B[/math] is its canonical trace, obtained by composing the left regular representation with the trace of [math]\mathcal L(B)[/math]:
As a basic illustration for this, any inclusion of type [math]\mathbb C\subset B[/math] is Markov. In general, if we write [math]B_0=C(X_0)[/math] and [math]B_1=C(X_1)[/math], then the inclusion [math]B_0\subset B_1[/math] must come from a certain fibration [math]X_1\to X_0[/math], and the inclusion [math]B_0\subset B_1[/math] is Markov precisely when the fibration [math]X_1\to X_0[/math] commutes with the respective counting measures.
We will be back to Markov inclusions and their various properties on several occasions, in what follows. For our next purposes here, we just need the following result:
Given a Markov inclusion of finite dimensional algebras [math]B_0\subset B_1[/math] we can perform to it the basic construction, as to obtain a Jones tower
This is something standard, from [1], by following the computations in the above, from the case of the [math]{\rm II}_1[/math] factors, and with everything extending well. It is of course possible to do something more general here, unifying the constructions for the inclusions of [math]{\rm II}_1[/math] factors [math]A_0\subset A_1[/math], and for the inclusions of Markov inclusions of finite dimensional algebras [math]B_0\subset B_1[/math], but we will not need this degree of generality, in what follows.
With these ingredients in hand, getting back now to the Jones, Ocneanu and Wassermann subfactors, from Theorem 16.26, the point is that these constructions can be unified, and then further studied, the final result on the subject being as follows:
Let [math]G[/math] be a compact group, and [math]G\to Aut(Q)[/math] be a minimal action on a [math]{\rm II}_1[/math] factor. Consider a Markov inclusion of finite dimensional algebras
In addition to the Jones, Ocneanu and Wassermann subfactors, discussed and unified in the above, we have the Popa subfactors, which are constructed as follows:
Given a discrete group [math]\Gamma= \lt g_1,\ldots,g_n \gt [/math], acting faithfully via outer automorphisms on a [math]{\rm II}_1[/math] factor [math]P[/math], we have the following “diagonal” subfactor
In order to unify now Theorem 16.29 and Proposition 16.30, observe that the diagonal subfactors can be written in the following way, by using a group dual:
Here the group dual [math]\widehat{\Gamma}[/math] acts on [math]Q=P\rtimes\Gamma[/math] via the dual of the action [math]\Gamma\subset Aut (P)[/math], and on [math]M_n(\mathbb C)[/math] via the adjoint action of the following formal representation:
Summarizing, we are led into quantum groups. So, let us start with:
A coaction of a Woronowicz algebra [math]A[/math] on a finite von Neumann algebra [math]Q[/math] is an injective morphism [math]\Phi:Q\to Q\otimes A''[/math] satisfying the following conditions:
- Coassociativity: [math](\Phi\otimes id)\Phi=(id\otimes\Delta)\Phi[/math].
- Trace equivariance: [math](tr\otimes id)\Phi=tr(.)1[/math].
- Smoothness: [math]\overline{\mathcal Q}^{\,w}=Q[/math], where [math]\mathcal Q=\Phi^{-1}(Q\otimes_{alg}\mathcal A)[/math].
These conditions come from what happens in the commutative case, [math]A=C(G)[/math], where they correspond to the usual associativity, trace equivariance and smoothness of the corresponding action [math]G\curvearrowright Q[/math]. Along the same lines, we have as well:
A coaction [math]\Phi:Q\to Q\otimes A''[/math] as above is called:
- Ergodic, if the algebra [math]Q^\Phi=\left\{p\in Q\big|\Phi(p)=p\otimes1\right\}[/math] reduces to [math]\mathbb C[/math].
- Faithful, if the span of [math]\left\{(f\otimes id)\Phi(Q)\big|f\in Q_*\right\}[/math] is dense in [math]A''[/math].
- Minimal, if it is faithful, and satisfies [math](Q^\Phi)'\cap Q=\mathbb C[/math].
Observe that the minimality of the action implies in particular that the fixed point algebra [math]Q^\Phi[/math] is a factor. Thus, we are getting here to the case that we are interested in, actions producing factors, via their fixed point algebras. Following [4], we have:
Consider a Woronowicz algebra [math]A=(A,\Delta,S)[/math], and denote by [math]A_\sigma[/math] the Woronowicz algebra [math](A,\sigma\Delta ,S)[/math], where [math]\sigma[/math] is the flip. Given two coactions
Our first task is to investigate the factoriality of such algebras, and we have here:
If [math]\beta:B\to B\otimes A[/math] is a coaction and [math]\pi:Q\to Q\otimes A_\sigma[/math] is a minimal coaction, then the following conditions are equivalent:
- The von Neumann algebra [math](B\otimes Q)^{\beta\odot\pi}[/math] is a factor.
- The coaction [math]\beta[/math] is centrally ergodic, [math]Z(B)\cap B^\beta=\mathbb C[/math].
This is something standard, from [4], the idea being as follows:
(1) Our first claim, which is something whose proof is a routine verification, explained in [4], is that the following diagram is a non-degenerate commuting square:
(2) In order to prove now the result, it is enough to check the following equality, between subalgebras of the von Neumann algebra [math]B\otimes Q[/math]:
But this follows from the non-degeneracy of the above commuting square. See [4].
With the above results in hand, we can now formulate our main theorem regarding the fixed point subfactors, of the most possible general type, as follows:
Let [math]G[/math] be a compact quantum group, and [math]G\to Aut(Q)[/math] be a minimal action on a [math]{\rm II}_1[/math] factor. Consider a Markov inclusion of finite dimensional algebras
The above result is important in connection with probability questions, because our usual character computations for [math]G[/math], for instance in the case where [math]G\subset U_N^+[/math] is easy, take place in the associated planar algebra [math]P_k=(B_0'\cap B_k)^G[/math]. More on this later.
This was for the basic theory of the fixed point subfactors. Many more things can be said about them, notably with an axiomatization of the planar algebras that we can obtain in this way, as being the subalgebras of Jones' bipartite graph planar algebras from [8], and also with a number of results and open questions regarding amenability. For more on all this, and for further details on the above, we refer to [4], [8], [9].
General references
Banica, Teo (2024). "Calculus and applications". arXiv:2401.00911 [math.CO].
References
- 1.0 1.1 V.F.R. Jones, Index for subfactors, Invent. Math. 72 (1983), 1--25.
- A. Ocneanu, Quantized groups, string algebras and Galois theory for algebras, London Math. Soc. Lect. Notes 136 (1988), 119--172.
- 3.0 3.1 3.2 3.3 A. Wassermann, Coactions and Yang-Baxter equations for ergodic actions and subfactors, London Math. Soc. Lect. Notes 136 (1988), 203--236.
- 4.0 4.1 4.2 4.3 4.4 4.5 4.6 4.7 4.8 4.9 T. Banica, Principles of operator algebras (2024).
- T. Banica, Introduction to quantum groups, Springer (2023).
- S. Popa, Classification of amenable subfactors of type II, Acta Math. 172 (1994), 163--255.
- S. Popa, An axiomatization of the lattice of higher relative commutants of a subfactor, Invent. Math. 120 (1995), 427--445.
- 8.0 8.1 V.F.R. Jones, The planar algebra of a bipartite graph, in “Knots in Hellas '98 (2000), 94--117.
- P. Tarrago and J. Wahl, Free wreath product quantum groups and standard invariants of subfactors, Adv. Math. 331 (2018), 1--57.