Planar algebra

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In mathematics, planar algebras first appeared in the work of Vaughan Jones on the standard invariant of a II1 subfactor. [1] They also provide an appropriate algebraic framework for many knot invariants (in particular the Jones polynomial), and have been used in describing the properties of Khovanov homology with respect to tangle composition.[2][3] Any finite group (and quantum generalization) can be encoded as a planar algebra.[1]


The idea of the planar algebra is to be a diagrammatic axiomatization of the standard invariant. [1] [4] [5]

Planar tangle[edit]

A (shaded) planar tangle is the data of finitely many input disks, one output disk, non-intersecting strings giving an even number, say , intervals per disk and one -marked interval per disk.


Here, the mark is shown as a -shape. On each input disk it is placed between two adjacent outgoing strings, and on the output disk it is placed between two adjacent incoming strings. A planar tangle is defined up to isotopy.


To compose two planar tangles, put the output disk of one into an input of the other, having as many intervals, same shading of marked intervals and such that the -marked intervals coincide. Finally we remove the coinciding circles. Note that two planar tangles can have zero, one or several possible compositions.


Planar operad[edit]

The planar operad is the set of all the planar tangles (up to isomorphism) with such compositions.

Planar algebra[edit]

A planar algebra is a representation of the planar operad; more precisely, it is a family of vector spaces , called -box spaces, on which acts the planar operad, i.e. for any tangle (with one output disk and input disks with and intervals respectively) there is a multilinear map

with according to the shading of the -marked intervals, and these maps (also called partition functions) respect the composition of tangle in such a way that all the diagrams as below commute.



Planar tangles[edit]

The family of vector spaces generated by the planar tangles having intervals on their output disk and a white (or black) -marked interval, admits a planar algebra structure.


The Temperley-Lieb-Jones planar algebra is generated by the planar tangles without input disk; its -box space is generated by


Moreover, a closed string is replaced by a multiplication by .


Note that the dimension of is the Catalan number . This planar algebra encodes the notion of Temperley–Lieb algebra.

Hopf algebra[edit]

A semisimple and cosemisimple Hopf algebra over an algebraically closed field is encoded in a planar algebra defined by generators and relations. [6]

Subfactor planar algebra[edit]


A subfactor planar algebra is a planar -algebra which is:

(1) Finite-dimensional:
(2) Evaluable:
(3) Spherical:
(4) Positive: defines an inner product.

Note that by (2) and (3), any closed string (shaded or not) counts for the same constant .


The tangle action deals with the adjoint by:

with the mirror image of and the adjoint of in .

Examples and results[edit]

No-ghost theorem: The planar algebra has no ghost (i.e. element with ) if and only if

For as above, and after a quotient by the null ideal (generated by elements with ), we get a subfactor planar algebra. Any subfactor planar algebra with constant admits as planar subalgebra.

A planar algebra is a subfactor planar algebra if and only if it is the standard invariant of an extremal subfactor of index , with and .[7] [8] [9] A finite depth or irreducible subfactor is extremal ( on ).

There is a subfactor planar algebra encoding any finite group (and any finite dimensional Hopf -algebra, called Kac algebra), defined by generators and relations. [10] [11]

The subfactor planar algebra associated to an inclusion of finite groups ,[12] does not always remember the (core-free) inclusion. [13] [14]

A Bisch-Jones planar algebra , initially called Fuss-Catalan, can be defined as for but by allowing two colors of string with their own constant and . For as above, and after the null quotient, it is a planar subalgebra of any subfactor planar algebra with an intermediate such that and . [15] [16]

The first finite depth subfactor planar algebra of index is called the Haagerup subfactor planar algebra. [17] It has index .

The subfactor planar algebras are completely classified for index at most [18] and a bit beyond. [19]

Fourier transform and biprojections[edit]

Let be a finite index subfactor, and the corresponding subfactor planar algebra. Assume that is irreducible (i.e. ). Let be an intermediate subfactor. Let the Jones projection . Note that . Let and .


Note that and .

Let the bijective linear map be the Fourier transform, also called -click (of the outer star) or rotation; and let be the coproduct of and .


Note that the word coproduct is a diminutive of convolution product. It is a binary operation.

The coproduct satisfies the equality

For any positive operators , the coproduct is also positive; this can be seen diagrammatically: [20]


Let be the contragredient (also called rotation). The map corresponds to four -clicks of the outer star, so it's the identity map, and then .

In the Kac algebra case, the contragredient is exactly the antipode,[11] which, for a finite group, correspond to the inverse.

A biprojection is a projection with a multiple of a projection. Note that and are biprojections; this can be seen as follows:


A projection is a biprojection iff it is the Jones projection of an intermediate subfactor [21] , iff . [22] [20]

Galois correspondence: [23] in the Kac algebra case, the biprojections are 1-1 with the left coideal subalgebras, which, for a finite group, correspond to the subgroups.

For any irreducible subfactor planar algebra, the set of biprojections is a finite lattice, [24] of the form , as for an interval of finite groups .

Using the biprojections, we can make the intermediate subfactor planar algebras. [25] [26]

The uncertainty principle extends to any irreducible subfactor planar algebra :

Let with the range projection of and the unnormalized trace (i.e. on ).

Noncommutative uncertainty principle: [27] Let , nonzero. Then

Assuming and positive, the equality holds if and only if is a biprojection. More generally, the equality holds if and only if is the bi-shift of a biprojection.


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