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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: | |||
<math display="block"> | |||
(Q^G)'\cap Q=\mathbb C | |||
</math> | |||
As a starting point, we have the following result, due to Jones <ref name="jo1">V.F.R. Jones, Index for subfactors, ''Invent. Math.'' '''72''' (1983), 1--25.</ref>: | |||
{{proofcard|Proposition|proposition-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 | |||
<math display="block"> | |||
Q^G\subset Q^H | |||
</math> | |||
having index <math>N=[G:H]</math>, called Jones 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 <ref name="ocn">A. Ocneanu, Quantized groups, string algebras and Galois theory for algebras, ''London Math. Soc. Lect. Notes'' '''136''' (1988), 119--172.</ref>: | |||
{{proofcard|Proposition|proposition-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, | |||
<math display="block"> | |||
Q\subset Q\rtimes G | |||
</math> | |||
having index <math>N=|G|</math>, called Ocneanu subfactor. | |||
|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 <ref name="was">A. Wassermann, Coactions and Yang-Baxter equations for ergodic actions and subfactors, ''London Math. Soc. Lect. Notes'' '''136''' (1988), 203--236.</ref>, namely: | |||
{{proofcard|Proposition|proposition-3|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 | |||
<math display="block"> | |||
Q^G\subset (M_n(\mathbb C)\otimes Q)^G | |||
</math> | |||
having index <math>N=n^2</math>, called Wassermann 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: | |||
{{proofcard|Theorem|theorem-1|The Jones, Ocneanu and Wassermann subfactors are all of the same nature, and can be written as follows, | |||
<math display="block"> | |||
\left( Q^G\subset Q^H\right)\,\simeq\, \left( ({\mathbb C}\otimes Q)^G\subset (l^\infty(G/H)\otimes Q)^G\right) | |||
</math> | |||
<math display="block"> | |||
\left( Q\subset Q\rtimes G\right)\,\simeq\, \left( (l^\infty (G)\otimes Q)^G\subset ({\mathcal L} (l^2(G))\otimes Q)^G\right) | |||
</math> | |||
<math display="block"> | |||
\left( Q^G\subset (M_n(\mathbb C) \otimes Q)^G\right)\,\simeq\, \left( ({\mathbb C}\otimes Q)^G\subset (M_n(\mathbb C)\otimes Q)^G\right) | |||
</math> | |||
with standard identifications for the various tensor products and fixed point algebras. | |||
|This is something standard, from <ref name="ba2">T. Banica, Principles of operator algebras (2024).</ref>, 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 <ref name="ba2">T. Banica, Principles of operator algebras (2024).</ref>, <ref name="was">A. Wassermann, Coactions and Yang-Baxter equations for ergodic actions and subfactors, ''London Math. Soc. Lect. Notes'' '''136''' (1988), 203--236.</ref>, 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: | |||
<math display="block"> | |||
(B_0\otimes Q)^G\subset (B_1\otimes Q)^G | |||
</math> | |||
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: | |||
{{defncard|label=|id=|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>: | |||
<math display="block"> | |||
tr:B\subset\mathcal L(B)\to\mathbb C | |||
</math> | |||
We say that an inclusion of finite dimensional algebras <math>B_0\subset B_1</math> is Markov if it commmutes with the canonical traces of <math>B_0,B_1</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: | |||
{{proofcard|Proposition|proposition-4|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 | |||
<math display="block"> | |||
B_0\subset_{e_1}B_1\subset_{e_2}B_2\subset_{e_3}B_3\subset\ldots\ldots | |||
</math> | |||
exactly as we did in the above for the inclusions of <math>{\rm II}_1</math> factors. | |||
|This is something standard, from <ref name="jo1">V.F.R. Jones, Index for subfactors, ''Invent. Math.'' '''72''' (1983), 1--25.</ref>, 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: | |||
{{proofcard|Theorem|theorem-2|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 | |||
<math display="block"> | |||
B_0\subset B_1 | |||
</math> | |||
and let <math>G\to Aut(B_1)</math> be an action which leaves invariant <math>B_0</math>, and which is such that its restrictions to the centers of <math>B_0</math> and <math>B_1</math> are ergodic. We have then a subfactor | |||
<math display="block"> | |||
(B_0\otimes Q)^G\subset (B_1\otimes Q)^G | |||
</math> | |||
of index <math>N=[B_1:B_0]</math>, called generalized Wassermann subfactor, whose Jones tower is | |||
<math display="block"> | |||
(B_1\otimes Q)^G\subset(B_2\otimes Q)^G\subset(B_3\otimes Q)^G\subset\ldots | |||
</math> | |||
where <math>\{ B_i\}_{i\geq 1}</math> are the algebras in the Jones tower for <math>B_0\subset B_1</math>, with the canonical actions of <math>G</math> coming from the action <math>G\to Aut(B_1)</math>, and whose planar algebra is given by: | |||
<math display="block"> | |||
P_k=(B_0'\cap B_k)^G | |||
</math> | |||
These subfactors generalize the Jones, Ocneanu and Wassermann subfactors. | |||
|This is something which is routine, from <ref name="ba3">T. Banica, Introduction to quantum groups, Springer (2023).</ref>, following Wassermann <ref name="was">A. Wassermann, Coactions and Yang-Baxter equations for ergodic actions and subfactors, ''London Math. Soc. Lect. Notes'' '''136''' (1988), 203--236.</ref>, and we will be back to this in a moment, with details, directly in a more general setting.}} | |||
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: | |||
{{proofcard|Proposition|proposition-5|Given a discrete group <math>\Gamma= < g_1,\ldots,g_n > </math>, acting faithfully via outer automorphisms on a <math>{\rm II}_1</math> factor <math>P</math>, we have the following “diagonal” subfactor | |||
<math display="block"> | |||
\left\{ \begin{pmatrix} | |||
g_1(q)\\ | |||
&\ddots\\ | |||
&& g_n(q) | |||
\end{pmatrix} \Big| q\in P\right\} \subset M_n(P) | |||
</math> | |||
having index <math>N=n^2</math>, called Popa subfactor. | |||
|This is something standard, a bit as for the Jones, Ocneanu and Wassermann subfactors, with the result basically coming from the work of Popa <ref name="po1">S. Popa, Classification of amenable subfactors of type II, ''Acta Math.'' '''172''' (1994), 163--255.</ref>, <ref name="po2">S. Popa, An axiomatization of the lattice of higher relative commutants of a subfactor, ''Invent. Math.'' '''120''' (1995), 427--445.</ref>.}} | |||
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: | |||
<math display="block"> | |||
(P\rtimes\Gamma)^{\widehat{\Gamma}}\subset(M_n(\mathbb C)\otimes (P\rtimes\Gamma))^{\widehat{\Gamma}} | |||
</math> | |||
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: | |||
<math display="block"> | |||
\oplus g_i :\widehat{\Gamma}\to {\mathbb C}^n | |||
</math> | |||
Summarizing, we are led into quantum groups. So, let us start with: | |||
{{defncard|label=|id=|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: | |||
<ul><li> Coassociativity: <math>(\Phi\otimes id)\Phi=(id\otimes\Delta)\Phi</math>. | |||
</li> | |||
<li> Trace equivariance: <math>(tr\otimes id)\Phi=tr(.)1</math>. | |||
</li> | |||
<li> Smoothness: <math>\overline{\mathcal Q}^{\,w}=Q</math>, where <math>\mathcal Q=\Phi^{-1}(Q\otimes_{alg}\mathcal A)</math>. | |||
</li> | |||
</ul>}} | |||
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: | |||
{{defncard|label=|id=|A coaction <math>\Phi:Q\to Q\otimes A''</math> as above is called: | |||
<ul><li> Ergodic, if the algebra <math>Q^\Phi=\left\{p\in Q\big|\Phi(p)=p\otimes1\right\}</math> reduces to <math>\mathbb C</math>. | |||
</li> | |||
<li> Faithful, if the span of <math>\left\{(f\otimes id)\Phi(Q)\big|f\in Q_*\right\}</math> is dense in <math>A''</math>. | |||
</li> | |||
<li> Minimal, if it is faithful, and satisfies <math>(Q^\Phi)'\cap Q=\mathbb C</math>. | |||
</li> | |||
</ul> }} | |||
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 <ref name="ba2">T. Banica, Principles of operator algebras (2024).</ref>, we have: | |||
{{proofcard|Proposition|proposition-6|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 | |||
<math display="block"> | |||
\beta:B\to B\otimes A\quad,\quad | |||
\pi:Q\to Q\otimes A_\sigma | |||
</math> | |||
with <math>B</math> being finite dimensional, the following linear map, while not being multiplicative in general, is coassociative with respect to the comultiplication <math>\sigma\Delta</math> of <math>A_\sigma</math>, | |||
<math display="block"> | |||
\beta\odot\pi:B\otimes Q\to B\otimes Q\otimes A_\sigma | |||
</math> | |||
<math display="block"> | |||
b\otimes p\to \pi (p)_{23}((id\otimes S)\beta(b))_{13} | |||
</math> | |||
and its fixed point space, which is by definition the following linear space, | |||
<math display="block"> | |||
(B\otimes Q)^{\beta\odot\pi}=\left\{x\in B\otimes Q\Big|(\beta\odot\pi )x=x\otimes 1\right\} | |||
</math> | |||
is then a von Neumann subalgebra of <math>B\otimes Q</math>. | |||
|This is something standard, which follows from a straightforward algebraic verification, explained in <ref name="ba2">T. Banica, Principles of operator algebras (2024).</ref>. As mentioned in the statement, to be noted is that the tensor product coaction <math>\beta\odot\pi</math> is not multiplicative in general. See <ref name="ba2">T. Banica, Principles of operator algebras (2024).</ref>.}} | |||
Our first task is to investigate the factoriality of such algebras, and we have here: | |||
{{proofcard|Theorem|theorem-3|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: | |||
<ul><li> The von Neumann algebra <math>(B\otimes Q)^{\beta\odot\pi}</math> is a factor. | |||
</li> | |||
<li> The coaction <math>\beta</math> is centrally ergodic, <math>Z(B)\cap B^\beta=\mathbb C</math>. | |||
</li> | |||
</ul> | |||
|This is something standard, from <ref name="ba2">T. Banica, Principles of operator algebras (2024).</ref>, the idea being as follows: | |||
(1) Our first claim, which is something whose proof is a routine verification, explained in <ref name="ba2">T. Banica, Principles of operator algebras (2024).</ref>, is that the following diagram is a non-degenerate commuting square: | |||
<math display="block"> | |||
\begin{matrix} | |||
Q&\subset&B\otimes Q\\ | |||
\cup &\ &\cup \\ | |||
Q^\pi&\subset&(B\otimes Q)^{\beta\odot\pi} | |||
\end{matrix} | |||
</math> | |||
(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>: | |||
<math display="block"> | |||
Z((B\otimes Q)^{\beta\odot\pi})=(Z(B)\cap B^\beta)\otimes 1 | |||
</math> | |||
But this follows from the non-degeneracy of the above commuting square. See <ref name="ba2">T. Banica, Principles of operator algebras (2024).</ref>.}} | |||
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: | |||
{{proofcard|Theorem|theorem-4|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 | |||
<math display="block"> | |||
B_0\subset B_1 | |||
</math> | |||
and let <math>G\to Aut(B_1)</math> be an action which leaves invariant <math>B_0</math> and which is such that its restrictions to the centers of <math>B_0</math> and <math>B_1</math> are ergodic. We have then a subfactor | |||
<math display="block"> | |||
(B_0\otimes Q)^G\subset (B_1\otimes Q)^G | |||
</math> | |||
of index <math>N=[B_1:B_0]</math>, called generalized Wassermann subfactor, whose Jones tower is | |||
<math display="block"> | |||
(B_1\otimes Q)^G\subset(B_2\otimes Q)^G\subset(B_3\otimes Q)^G\subset\ldots | |||
</math> | |||
where <math>\{ B_i\}_{i\geq 1}</math> are the algebras in the Jones tower for <math>B_0\subset B_1</math>, with the canonical actions of <math>G</math> coming from the action <math>G\to Aut(B_1)</math>, and whose planar algebra is given by: | |||
<math display="block"> | |||
P_k=(B_0'\cap B_k)^G | |||
</math> | |||
These subfactors generalize the Jones, Ocneanu, Wassermann and Popa subfactors. | |||
|This is something routine, based on the above general theory and results, and for the full story here, and technical details, we refer to <ref name="ba2">T. Banica, Principles of operator algebras (2024).</ref>, <ref name="was">A. Wassermann, Coactions and Yang-Baxter equations for ergodic actions and subfactors, ''London Math. Soc. Lect. Notes'' '''136''' (1988), 203--236.</ref>.}} | |||
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 <ref name="jo4">V.F.R. Jones, The planar algebra of a bipartite graph, in “Knots in Hellas '98'' (2000), 94--117.</ref>, 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 <ref name="ba2">T. Banica, Principles of operator algebras (2024).</ref>, <ref name="jo4">V.F.R. Jones, The planar algebra of a bipartite graph, in “Knots in Hellas '98'' (2000), 94--117.</ref>, <ref name="twa">P. Tarrago and J. Wahl, Free wreath product quantum groups and standard invariants of subfactors, ''Adv. Math.'' '''331''' (2018), 1--57.</ref>. | |||
==General references== | |||
{{cite arXiv|last1=Banica|first1=Teo|year=2024|title=Calculus and applications|eprint=2401.00911|class=math.CO}} | |||
==References== | |||
{{reflist}} |
Latest revision as of 19:40, 21 April 2025
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.