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Planar algebras, quantum information theory and subfactors

Vijay Kodiyalam Sruthymurali  and  V. S. Sunder The Institute of Mathematical Sciences, Chennai, India and Homi Bhabha National Institute, Mumbai, India vijay@imsc.res.in,sruthym@imsc.res.in,sunder@imsc.res.in
Abstract.

We define generalised notions of biunitary elements in planar algebras and show that objects arising in quantum information theory such as Hadamard matrices, quantum latin squares and unitary error bases are all given by biunitary elements in the spin planar algebra. We show that there are natural subfactor planar algebras associated with biunitary elements.

2010 Mathematics Subject Classification:
Primary 46L37, 81P45, 81P68
The authors are very grateful to Prof. Ajit Iqbal Singh for bringing the paper of Reutter and Vicary to their attention.

1. Introduction

The motivation for this paper comes from the beautiful results of Reutter and Vicary in [RttVcr2016] in which planar algebraic constructions are used to treat a variety of objects in quantum information theory such as Hadamard matrices, quantum latin squares and unitary error bases. While pictorial and planar algebraic techniques are used throughout that paper, no planar algebra actually makes an appearance, leading to the question as to where these objects actually live.

In §2 we describe Jones’ spin planar algebra and a specific recent presentation of it by generators and relations as discussed in [KdyMrlSniSnd2019].

We define and identify an equivalent formulation of the notion of a biunitary element in a planar algebra in §3 and show that the spin planar algebra is the natural receptacle of all of the following objects - Hadamard matrices, quantum Latin squares, biunitary matrices (and unitary error bases) - by identifying these with appropriate types of biunitary elements (and generalised versions of these) in the spin planar algebra.

The construction of subfactors from biunitary matrices is well known - see [HgrSch1989] and [Snd1989] - and our results naturally suggest that there might be subfactors associated to our biunitary elements and we show in §4 that this is indeed the case - by constructing appropriate planar algebras.

In the particular case of a Latin square arising from a group multiplication table, we identify this planar algebra, unsurprisingly, with the very well understood planar algebra of a group in the final §5.

2. The spin planar algebra

Let us recall Jones’ spin planar algebra PP which was shown to have a presentation in terms of generators and relations in [KdyMrlSniSnd2019] as follows. Let S={s1,,sn}S=\{s_{1},\ldots,s_{n}\} be a finite set. Take the label set L=L(0,)=SL=L_{(0,-)}=S equipped with the identity involution *. Then P=P(S)P=P(S) is defined to be the quotient P=P(L,R)P=P(L,R) of the universal planar algebra P(L)P(L) by the set RR of relations given in Figures 1 and 2.

The facts that we will need about the spin planar algebra are summarised in the following two results.

\psfrag{v+}{\huge$v_{+}$}\psfrag{v-}{\huge$s_{i}$}\psfrag{u1}{\Huge$\displaystyle{\frac{1}{\mu(v_{+})}}$}\psfrag{u2}{\Huge$\displaystyle{\frac{1}{\mu(v_{-})}}$}\psfrag{text1}{\Huge$=\displaystyle{\sqrt{n}}$}\psfrag{text2}{\Huge$=\displaystyle{\frac{1}{\sqrt{n}}}$}\includegraphics{modulus.eps}
Figure 1. The white and black modulus relations
\psfrag{fi}{\Huge$s_{i}$}\psfrag{fj}{\Huge$s_{j}$}\psfrag{text2}{\Huge$\displaystyle{\sum\limits_{i}}$}\psfrag{=}{\Huge$=\frac{1}{\sqrt{n}}$}\psfrag{=dij}{\bf{\Huge$=\delta_{ij}$}}\includegraphics{mult.eps}
Figure 2. The multiplication relation and the black channel relation
\psfrag{v+}{\huge$v_{+}$}\psfrag{v-}{\huge$s_{i}$}\psfrag{u1}{\Huge$\displaystyle{\frac{1}{\mu(v_{+})}}$}\psfrag{u2}{\Huge$\displaystyle{\frac{1}{\mu(v_{-})}}$}\psfrag{xi}{\Huge$\xi,\xi$}\psfrag{text3}{\Huge$=\displaystyle{\sqrt{n}}$}\psfrag{text1}{\Huge$=\displaystyle{\sum\limits_{v_{+}\in\mathcal{V}_{+}}}$}\psfrag{text2}{\Huge$=\displaystyle{\sum\limits_{i}}$}\includegraphics{unit2.eps}
Figure 3. The unit and modulus relations
\psfrag{fi}{\Huge$s_{i}$}\psfrag{fj}{\Huge$s_{j}$}\psfrag{text2}{\Huge$\displaystyle{\sum\limits_{i}}$}\psfrag{=}{\Huge$=$}\psfrag{=dij}{\bf{\Huge$=\delta_{ij}$}}\includegraphics{inter.eps}
Figure 4. Another unit relation
Lemma 1 (Lemma 2 of [KdyMrlSniSnd2019]).

The unit and modulus relations of Figures 3 and 4 hold in the planar algebra PP.

Theorem 2 (Theorem 1 of [KdyMrlSniSnd2019]).

The spin planar algebra PP is a finite dimensional CC^{*}- planar algebra with modulus n\sqrt{n} and such that dim(P(0,+))=1\text{dim}(P_{(0,+)})=1, dim(P(0,))=n\text{dim}(P_{(0,-)})=n and dim(P(k,±))=nk\text{dim}(P_{(k,\pm)})=n^{k} for all k>0k>0. Bases for P(k,±)P_{(k,\pm)} for k>0k>0 are given as in Figures 5 and 6 for kk even and odd respectively while a basis of dim(P(0,))\text{dim}(P_{(0,-)}) is given by S(i)S(i) which will denote the (0,)(0,-)-tangle with a single internal (0,)(0,-) box labelled sis_{i} (which appears on the right hand sides of the multiplication relation of Figure 2 or of the unit relation of Figure 3).

\psfrag{si1}{\Huge$s_{i_{1}}$}\psfrag{si2}{\Huge$s_{i_{2}}$}\psfrag{sik}{\Huge$s_{i_{m}}$}\psfrag{sj1}{\Huge$s_{j_{1}}$}\psfrag{sj2}{\Huge$s_{j_{2}}$}\psfrag{sjk}{\Huge$s_{j_{m}}$}\psfrag{sp}{\Huge$s_{p}$}\psfrag{sq}{\Huge$s_{q}$}\psfrag{sim}{\Huge$s_{i_{m}}$}\psfrag{sikm1}{\Huge$s_{i_{m-1}}$}\psfrag{sjkm1}{\Huge$s_{j_{2}}$}\psfrag{fi}{\Huge$s_{i}$}\psfrag{fj}{\Huge$s_{j}$}\psfrag{cdots}{\Huge$\displaystyle{\cdots}$}\psfrag{=}{\Huge$=$}\psfrag{=dij}{\bf{\Huge$=\delta_{ij}$}}\includegraphics{bases1.eps}
Figure 5. Bases (2m,+){\mathcal{B}}_{(2m,+)} for m1m\geq 1 and (2m+2,){\mathcal{B}}_{(2m+2,-)} for m0m\geq 0
\psfrag{si1}{\Huge$s_{i_{1}}$}\psfrag{si2}{\Huge$s_{i_{2}}$}\psfrag{sik}{\Huge$s_{i_{m}}$}\psfrag{sj1}{\Huge$s_{j_{1}}$}\psfrag{sj2}{\Huge$s_{j_{2}}$}\psfrag{sjk}{\Huge$s_{q}$}\psfrag{sp}{\Huge$s_{p}$}\psfrag{sjmm1}{\Huge$s_{j_{2}}$}\psfrag{sjm}{\Huge$s_{j_{m}}$}\psfrag{sikm1}{\Huge$s_{i_{m}}$}\psfrag{simp1}{\Huge$s_{j_{m}}$}\psfrag{sjkm1}{\Huge$s_{j_{m}}$}\psfrag{cdots}{\Huge$\displaystyle{\cdots}$}\psfrag{fi}{\Huge$s_{i}$}\psfrag{fj}{\Huge$s_{j}$}\psfrag{cdots}{\Huge$\displaystyle{\cdots}$}\psfrag{=}{\Huge$=$}\psfrag{=dij}{\bf{\Huge$=\delta_{ij}$}}\includegraphics{bases2.eps}
Figure 6. Bases (2m+1,±){\mathcal{B}}_{(2m+1,\pm)} for m0m\geq 0

3. Biunitarity in planar algebras

In this section we will first define the notion of biunitary element in a *- planar algebra. For each kk\in{\mathbb{N}}, we have the rotation tangle R(k,ϵ)=R(k,ϵ)(k,ϵ)(k,ϵ)R(k,\epsilon)=R(k,\epsilon)_{(k,\epsilon)}^{(k,-\epsilon)} and its \ell-fold iteration R(k,ϵ,)R(k,\epsilon,\ell) given as in Figure 7.

\psfrag{k-1}{\tiny$k-1$}\psfrag{1}{\tiny$1$}\psfrag{k-l}{\tiny$k-\ell$}\psfrag{l}{\tiny$\ell$}\psfrag{R}{$R(k,\epsilon)=R(k,\epsilon)_{(k,\epsilon)}^{(k,-\epsilon)}$}\psfrag{R^l}{$R(k,\epsilon,\ell)=\displaystyle{R(k,\epsilon,\ell)_{(k,\epsilon)}^{(k,(-1)^{\ell}\epsilon)}}$}\includegraphics[height=99.58464pt]{rotation.eps}
Figure 7. Rotation tangles

In Figure 7 and in the sequel we adopt two conventions: (i) ()(-)^{\ell} denotes ±\pm according to the parity of \ell, and (ii) In view of the difficulty of shading diagrams which depend on the parity of \ell, we will dispense with shading figures since the shading is uniquely determined by the sub- and superscripts of the tangle.

Definition 3.

Let PP be a *-planar algebra and let uP(k,ϵ)u\in P_{(k,\epsilon)}. For 0<<k0<\ell<k, the element uu is said to be a {0,}\{0,\ell\}-biunitary element if the elements uP(k,ϵ)u\in P_{(k,\epsilon)} and ZR(k,ϵ,)(u)P(k,ϵ())Z_{R(k,\epsilon,\ell)}(u)\in P_{(k,\epsilon(-)^{\ell})} are both unitary.

Lemma 4.

The element uP(k,ϵ)u\in P_{(k,\epsilon)} is {0,}\{0,\ell\}-biunitary if and only if the relations in Figure 8 hold in P(k,ϵ)P_{(k,\epsilon)}.

\psfrag{kml}{\tiny{$k-\ell$}}\psfrag{l}{\tiny{$\ell$}}\psfrag{u}{\small$u$}\psfrag{u*}{\small$u^{*}$}\psfrag{=}{\tiny{$=$}}\includegraphics[height=184.9429pt]{biunitary.eps}
Figure 8. {0,}\{0,\ell\}-biunitarity relations
Proof.

After choosing the external *-arc appropriately, the relations on top in Figure 8 are equivalent to the unitarity of uu while the relations on the bottom are equivalent to the unitarity of ZR(k,ϵ,)(u)Z_{R(k,\epsilon,\ell)}(u). \Box

Remark 5.

Observe that if uP(k,ϵ)u\in P_{(k,\epsilon)} is a {0,}\{0,\ell\}-biunitary element, then so are ZR(k,ϵ,k)(u)P(k,ϵ()k)Z_{R(k,\epsilon,k)}(u)\in P_{(k,\epsilon(-)^{k})} and ZR(k,ϵ,)(u)P(k,ϵ())Z_{R(k,\epsilon,-\ell)}(u^{*})\in P_{(k,\epsilon(-)^{\ell})}.

In the rest of this section we will show that certain biunitary elements in the spin planar algebra are in one-to-one correspondence with some objects that arise in quantum information theory. We first define these objects.

Definition 6.

An n×nn\times n complex matrix H=((hij))H=((h_{ij})) is said to be a complex Hadamard matrix if HH=nIHH^{*}=nI and |hij|=1|h_{ij}|=1 for each i,ji,j.

Example 7.

Let ω\omega\in{\mathbb{C}} be a primitive nthn^{th}-root of unity. The matrix

H=[1111ωωn11ω2(ω2)n11ωn1(ωn1)n1]\displaystyle{H=\begin{bmatrix}1&1&\cdots&1\\ 1&\omega&\cdots&\omega^{n-1}\\ 1&\omega^{2}&\cdots&(\omega^{2})^{n-1}\\ \vdots&\vdots&\cdots&\vdots\\ 1&\omega^{n-1}&\cdots&(\omega^{n-1})^{n-1}\end{bmatrix}}

is a complex Hadamard matrix which is a multiple of the so-called Fourier matrix.

Definition 8.

A Latin square is an n×nn\times n array filled with n different symbols, each occurring exactly once in each row and in each column.

Example 9.

The multiplication table of a finite group is a Latin square. The smallest example which is not (equivalent to one) of this type is of size 5 and is given by:

[1234524153354214153253214].\begin{bmatrix}1&2&3&4&5\\ 2&4&1&5&3\\ 3&5&4&2&1\\ 4&1&5&3&2\\ 5&3&2&1&4\end{bmatrix}.
Definition 10.

A quantum Latin square of size nn is an n×nn\times n matrix of vectors in n\mathbb{C}^{n} such that each row and each column is an orthonormal basis for n\mathbb{C}^{n}.

Example 11.

Any Latin square gives a quantum Latin square in the following simple-minded way. Let {e1,,en}\{e_{1},\ldots,e_{n}\} be the standard orthonormal basis of n\mathbb{C}^{n}. Consider the 5×55\times 5 Latin square in the Example 9. It gives the following quantum Latin square:

[e1e2e3e4e5e2e4e1e5e3e3e5e4e2e1e4e1e5e3e2e5e3e2e1e4]\begin{bmatrix}e_{1}&e_{2}&e_{3}&e_{4}&e_{5}\\ e_{2}&e_{4}&e_{1}&e_{5}&e_{3}\\ e_{3}&e_{5}&e_{4}&e_{2}&e_{1}\\ e_{4}&e_{1}&e_{5}&e_{3}&e_{2}\\ e_{5}&e_{3}&e_{2}&e_{1}&e_{4}\end{bmatrix}

For more on quantum Latin squares and non-trivial examples see [MstVcr2015].

Definition 12.

A matrix U=((uijkl))Mn2()U=((u^{ij}_{kl}))\in M_{n^{2}}(\mathbb{C}) (for i,j,k,l{1,,n}i,j,k,l\in\{1,\cdots,n\}) is said to be a biunitary matrix if both UU and its block transpose, say V=((vijkl))V=((v^{ij}_{kl})), defined by vijkl=ukjilv^{ij}_{kl}=u^{kj}_{il}, are unitary matrices.

Example 13.

For examples of biunitary matrices of size 9 which are, in addition, permutation matrices, and their applications in subfactor theory see [KrsSnd1996].

Definition 14.

A unitary error basis for Mn()M_{n}({\mathbb{C}}) is a collection of n2n^{2} unitary matrices which form an orthonormal basis with respect to the normalised trace inner product given by A|B=Tr(BA)n\displaystyle{\langle A|B\rangle=\frac{Tr(B^{*}A)}{n}}.

Example 15.

The matrices {UiVj:1i,jn}\{U^{i}V^{j}:1\leq i,j\leq n\}, where UU is the n×nn\times n Fourier matrix and VV is the permutation matrix corresponding to the cycle (12n)(1~{}2~{}\cdots~{}n), form a unitary error basis.

We will now state and prove the main theorem of this section. Let P=P(S)P=P(S) be the spin planar algebra where S={s1,,sn}S=\{s_{1},\cdots,s_{n}\}. We will need some notation for the normalised version of the bases for P(k,±)P_{(k,\pm)} for k=1,k=1,\ldots given in Figures 5 and 6. We denote (n)m(\sqrt{n})^{m} times the elements on the top and bottom in Figure 5 by ei1imj1jme^{i_{1}\cdots i_{m}}_{j_{1}\cdots j_{m}} and e[p)i1imj1jm(q]e[p)^{i_{1}\cdots i_{m}}_{j_{1}\cdots j_{m}}(q] respectively. Similarly, we denote (n)m(\sqrt{n})^{m} times the elements on the top and bottom in Figure 6 by ei1imj1jm(q]e^{i_{1}\cdots i_{m}}_{j_{1}\cdots j_{m}}(q] and e[p)i1imj1jme[p)^{i_{1}\cdots i_{m}}_{j_{1}\cdots j_{m}}. In the following proof we will implicitly use the multiplication relations among these elements as in Lemma 10 of [KdyMrlSniSnd2019]. We will also require the action of the rotation tangle on the bases as stated in Lemma 16 below (in the proof of Equations 3.2, 3.4 and 3.6).

Lemma 16.

With notation as above,

ZR(2m,+)(ei1imj1jm)\displaystyle Z_{R(2m,+)}(e^{i_{1}\cdots i_{m}}_{j_{1}\cdots j_{m}}) =\displaystyle= ne[j1)i1im1j2jm(im]\displaystyle\sqrt{n}~{}e[j_{1})^{i_{1}\cdots i_{m-1}}_{j_{2}\cdots j_{m}}(i_{m}]
ZR(2m+2,)(e[p)i1imj1jm(q])\displaystyle Z_{R(2m+2,-)}(e[p)^{i_{1}\cdots i_{m}}_{j_{1}\cdots j_{m}}(q]) =\displaystyle= 1nepi1imj1jmq\displaystyle\frac{1}{\sqrt{n}}~{}e^{p\ \!\!i_{1}\cdots i_{m}}_{j_{1}\cdots j_{m}q}
ZR(2m+1,+)(ei1imj1jm(q])\displaystyle Z_{R(2m+1,+)}(e^{i_{1}\cdots i_{m}}_{j_{1}\cdots j_{m}}(q]) =\displaystyle= e[j1)i1imj2jmq\displaystyle e[j_{1})^{i_{1}\ \cdots\ i_{m}}_{j_{2}\cdots j_{m}q}
ZR(2m+1,)(e[p)i1imj1jm)\displaystyle Z_{R(2m+1,-)}(e[p)^{i_{1}\cdots i_{m}}_{j_{1}\cdots j_{m}}) =\displaystyle= epi1im1j1jm(im]\displaystyle e^{pi_{1}\cdots i_{m-1}}_{j_{1}\ \cdots\ j_{m}}(i_{m}]
Theorem 17.

There are natural 1-1 correspondences between the following sets:
1) {0,1}\{0,1\}-biunitary elements in P(2,+)P_{(2,+)} and Hadamard matrices of size n×nn\times n,
2) {0,1}\{0,1\}-biunitary elements in P(3,+)P_{(3,+)} and quantum Latin squares of size n×nn\times n, and
3) {0,2}\{0,2\}-biunitary elements in P(4,+)P_{(4,+)} and biunitary matrices of size n2×n2n^{2}\times n^{2}.

Proof.

1) Let u=i,jaijeijP(2,+)\displaystyle{u=\sum_{i,j}a^{i}_{j}~{}~{}e^{i}_{j}\in P_{(2,+)}}. Then,

(3.1) uu=1jaijapj¯=δi,pi,p=1,,n,uu^{*}=1\Leftrightarrow\displaystyle{\sum_{j}a^{i}_{j}~{}~{}\overline{a^{p}_{j}}=\delta_{i,p}}~{}~{}\forall~{}i,p=1,\ldots,n,

and

(3.2) ZR(2,+)(u)(ZR(2,+)(u))=1naijaij¯=1i,j=1,,n.Z_{R(2,+)}(u)(Z_{R(2,+)}(u))^{*}=1\Leftrightarrow n~{}a^{i}_{j}~{}~{}\overline{a^{i}_{j}}=1~{}~{}\forall~{}i,j=1,\ldots,n.

Let H=((naij))H=((\sqrt{n}a^{i}_{j})). Then Equation 3.1 is equivalent to HH=nIHH^{*}=n~{}I and Equation 3.2 is equivalent to |naij|=1|\sqrt{n}a^{i}_{j}|=1. Thus the association of uu with HH is a 1-1 correspondence between {0,1}\{0,1\}-biunitary elements of P(2,+)P_{(2,+)} and Hadamard matrices of size n×nn\times n.

2) Now let u=i,j,kaijkeik(j]P(3,+)\displaystyle{u=\sum_{i,j,k}a_{ij}^{k}~{}~{}e^{i}_{k}(j]\in P_{(3,+)}}. Then,

(3.3) uu=1kaijkapjk¯=δi,p,j,i,p=1,,n,uu^{*}=1\Leftrightarrow\displaystyle{\sum_{k}~{}a_{ij}^{k}~{}~{}\overline{a_{pj}^{k}}=\delta_{i,p},~{}~{}\forall~{}~{}j,i,p=1,\ldots,n},

and

(3.4) ZR(3,+)(u)(ZR(3,+)(u))=1jaijkapjk¯=δi,p,k,i,p=1,,n.Z_{R(3,+)}(u)(Z_{R(3,+)}(u))^{*}=1\Leftrightarrow\displaystyle{\sum_{j}~{}a_{ij}^{k}~{}~{}\overline{a_{pj}^{k}}=\delta_{i,p},~{}~{}\forall~{}~{}k,i,p=1,\ldots,n}.

Let Q=((Qij))Q=((Q^{i}_{j})) where Qij=(a1ji,a2ji,,anji)nQ^{i}_{j}=(a_{1j}^{i},a_{2j}^{i},\ldots,a_{nj}^{i})\in{\mathbb{C}}^{n}. Then, Equation 3.3 is equivalent to the column vectors of QQ forming an orthonormal basis for n\mathbb{C}^{n} and Equation 3.4 is equivalent to the row vectors of QQ forming an orthonormal basis for n\mathbb{C}^{n}. Thus the association of uu with QQ is a 1-1 correspondence between {0,1}\{0,1\}-biunitary elements of P(3,+)P_{(3,+)} and quantum Latin squares of size n×nn\times n.

3) Let u=i,j,k,aijkeijkP(4,+)\displaystyle{u=\sum_{i,j,k,\ell}a^{ij}_{k\ell}e^{ij}_{\ell k}\in P_{(4,+)}}. Then,

(3.5) uu=1k,aijkapqk¯=δi,pδj,q,i,j,p,q=1,,nuu^{*}=1\Leftrightarrow\displaystyle{\sum_{k,\ell}~{}~{}a^{ij}_{k\ell}~{}~{}\overline{a^{pq}_{k\ell}}=\delta_{i,p}~{}~{}\delta_{j,q}},~{}~{}\forall~{}~{}i,j,p,q=1,\ldots,n

and

(3.6) ZR(4,+,2)(u)(ZR(4,+,2)(u))=1j,kaijkapjks¯=δi,pδ,s,i,p,,s=1,,nZ_{R(4,+,2)}(u)(Z_{R(4,+,2)}(u))^{*}=1\Leftrightarrow\displaystyle{\sum_{j,k}~{}~{}a^{ij}_{k\ell}~{}~{}\overline{a^{pj}_{ks}}=\delta_{i,p}~{}~{}\delta_{\ell,s}},~{}~{}\forall~{}~{}i,p,\ell,s=1,\ldots,n

Here let U=((aijk))U=((a^{ij}_{k\ell})). Then, Equation 3.5 is equivalent to UU being unitary and Equation 3.6 is equivalent to the block transpose of UU being unitary. Thus the association of uu with UU is a 1-1 correspondence between {0,2}\{0,2\}-biunitary elements of P(4,+)P_{(4,+)} and biunitary matrices of size n2×n2n^{2}\times n^{2}. \Box

An analogous 1-1 correspondence result for unitary error bases requires a modified version of the notion of biunitary element which we will now define. Recall that a labelled annular tangle in a planar algebra PP is a tangle AA all of whose internal boxes except for one have been labelled by elements of the appropriate P(k,ϵ)P_{(k,\epsilon)}’s. Actually we would like to consider linear extensions of the definition and of the vector operations to linear combinations of such tangles, provided of course that all the annular tangles involved yield maps between the same spaces. We will use the term modified annular tangle for such linear combinations.

Definition 18.

Let PP be a *- planar algebra and A,BA,B be modified annular tangles with their unlabelled box of colour (k,ϵ)(k,\epsilon). An element uP(k,ϵ)u\in P_{(k,\epsilon)} is said to be an {A,B}\{A,B\}-biunitary element if ZA(u)Z_{A}(u) and ZB(u)Z_{B}(u) are both unitary.

Remark 19.

Note that a {0,}\{0,\ell\}-biunitary element in P(k,ϵ)P_{(k,\epsilon)} is nothing but an {I,R(k,ϵ,)}\{I,R(k,\epsilon,\ell)\}-biunitary element, where II denotes the identity tangle of colour (k,ϵ)(k,\epsilon).

In order to state the analogue of Theorem 17 for unitary error bases we will need the modified annular tangle A=A(4,+)(4,+)A=A_{(4,+)}^{(4,+)}, with labelled internal boxes coming from the spin planar algebra PP, defined by Figure 9.

\psfrag{si}{\tiny$s_{i}$}\psfrag{sj}{\tiny$s_{j}$}\psfrag{n}{$n$}\psfrag{sum_ij}{\large$\displaystyle{\sum_{i,j=1}^{n}}$}\psfrag{*}{\tiny$*$}\includegraphics[height=99.58464pt]{uebpicture.eps}
Figure 9. The annular tangle AA

Observe that ZA(eijkl)=eilkjZ_{A}(e^{ij}_{kl})=e^{il}_{kj}.

Proposition 20.

There is a natural 1-1 correspondence between {A,R(4,+)}\{A,R(4,+)\}-biunitary elements in P(4,+)P_{(4,+)} and unitary error bases in Mn()M_{n}({\mathbb{C}}).

Proof.

Let u=i,j,k,aijkeijkP(4,+)\displaystyle{u=\sum_{i,j,k,\ell}~{}~{}a^{ij}_{k\ell}~{}~{}e^{ij}_{\ell k}~{}~{}}\in P_{(4,+)}. Then,

ZR(4,+)(u)\displaystyle Z_{R(4,+)}(u) =\displaystyle= i,j,k,naijke[)ik(j],and\displaystyle\sum_{i,j,k,\ell}~{}~{}\sqrt{n}~{}~{}a^{ij}_{k\ell}~{}~{}e[\ell)^{i}_{k}(j],~{}{\text{and}}
ZA(u)\displaystyle Z_{A}(u) =\displaystyle= i,j,k,aijkeikj.\displaystyle\sum_{i,j,k,\ell}~{}~{}a^{ij}_{k\ell}~{}~{}e^{ik}_{\ell j}.

by Lemma 16 and the observation above. Hence

(3.7) (ZA(u))ZA(u)=1i,kaijkaiqks¯=δsδjq,s,j,q=1,,n(Z_{A}(u))^{*}Z_{A}(u)=1\Leftrightarrow\sum_{i,k}~{}~{}a^{ij}_{k\ell}~{}~{}\overline{a^{iq}_{ks}}=\delta_{\ell s}~{}~{}\delta_{jq}~{}~{}\forall~{}~{}\ell,s,j,q=1,\ldots,n

and

(3.8) ZR(4,+)(u)(ZR(4,+)(u))=1kaijkapjk¯=1nδipj,,i,p=1,,nZ_{R(4,+)}(u)(Z_{R(4,+)}(u))^{*}=1\Leftrightarrow\sum_{k}~{}~{}a^{ij}_{k\ell}~{}~{}\overline{a^{pj}_{k\ell}}=\frac{1}{n}~{}~{}\delta_{ip}~{}~{}\forall j,\ell,i,p=1,\ldots,n

Let B(j,)B(j,\ell) be the n×nn\times n matrix given by B(j,)=((naijk))B(j,\ell)=((\sqrt{n}a^{ij}_{k\ell})). Then Equation 3.8 is equivalent to B(j,)B(j,\ell) being a unitary matrix for all j,j,\ell and Equation 3.7 is equivalent to the collection {B(j,)}j,\{B(j,\ell)\}_{j,\ell} forming an orthonormal basis for Mn()M_{n}({\mathbb{C}}). Thus the association of uu with {B(j,)}j,\{B(j,\ell)\}_{j,\ell} is a 1-1 correspondence between {A,R(4,+)}\{A,R(4,+)\}-biunitary elements of P(4,+)P_{(4,+)} and unitary error bases of Mn()M_{n}({\mathbb{C}}). \Box

4. From biunitary elements to subfactor planar algebras

Throughout this section, PP will be a spherical CC^{*}-planar algebra with modulus δ\delta and uP(k,ϵ)u\in P_{(k,\epsilon)} will be a {0,}\{0,\ell\}-biunitary. To this data, we will associate a CC^{*}-planar subalgebra QQ of the (,ϵ)th(\ell,\epsilon)^{th} cabling (,ϵ)P{}^{(\ell,\epsilon)}P of PP. The notion of cabling that we use here is a generalised version of the one defined in [DeKdy2018], so we give a careful definition.

Definition 21.

Let (,ϵ)×{±}(\ell,\epsilon)\in{\mathbb{N}}\times\{\pm\}. Define (n,η)(,ϵ)(n,\eta)^{(\ell,\epsilon)} to be (n,ϵη)(n\ell,\epsilon\eta^{\ell}). Next, define the (,ϵ)(\ell,\epsilon)-cable of a tangle TT, denoted by T(,ϵ)T^{(\ell,\epsilon)}, as follows. Consider the tangle TT ignoring its shading and replace each of its strands (including the closed loops) by a cable of \ell parallel strands without changing the *-arcs. Introduce shading in this picture such that an (n,η)(n,\eta)-box of TT becomes an (n,η)(,ϵ)(n,\eta)^{(\ell,\epsilon)}-box of T(,ϵ)T^{(\ell,\epsilon)}.

We omit the verification that this extends uniquely to a chequerboard shading of T(,ϵ)T^{(\ell,\epsilon)} making it a tangle and that TT(,ϵ)T\mapsto T^{(\ell,\epsilon)} is an ‘operation on tangles’ in the sense of [KdySnd2004]. The corresponding operation on planar algebras will be denoted by P(,ϵ)PP\mapsto^{(\ell,\epsilon)}\!\!\!P. To give an example of cabling, note that the (,ϵ)(\ell,\epsilon)-cable of the rotation tangle R(n,η)R(n,\eta) of Figure 7 is given as in Figure 10 below. The shading of the *-arc of the external box is given by ϵ(η)\epsilon(-\eta)^{\ell}.

\psfrag{k-1}{\tiny$(n-1)\ell$}\psfrag{1}{\tiny$\ell$}\includegraphics[height=99.58464pt]{cabrot.eps}
Figure 10. The (,ϵ)(\ell,\epsilon)-cabling of the rotation tangle R(n,η)R(n,\eta)
Definition 22.

For (,ϵ)×{±}(\ell,\epsilon)\in{\mathbb{N}}\times\{\pm\}, the planar algebra (,ϵ)P{}^{(\ell,\epsilon)}P has underlying vector spaces given by (,ϵ)P(n,η)=P(n,η)(,ϵ){}^{(\ell,\epsilon)}P_{(n,\eta)}=P_{(n,\eta)^{(\ell,\epsilon)}} with the tangle action given by ZT(,ϵ)P=ZT(,ϵ)PZ_{T}^{{}^{(\ell,\epsilon)}P}=Z_{T^{(\ell,\epsilon)}}^{P}.

Before proceeding to define subspaces Q(n,η)Q_{(n,\eta)} of (,ϵ)P(n,η){}^{(\ell,\epsilon)}P_{(n,\eta)}, we begin with the inevitable notation. For n=0,1,n=0,1,\ldots, define the elements u(n,η)P(n+k,ϵη)u_{(n,\eta)}\in P_{(n\ell+k-\ell,\epsilon\eta^{\ell})} as in Figure 11 - where the label in the last box is uu or uu^{*} depending on the parity of nn.

\psfrag{u_{(0,pm)}}{$u_{(0,\pm)}$}\psfrag{u_{(n,-)}:n>0}{$u_{(n,-)}:n>0$}\psfrag{u_{(n,+)}:n>0}{$u_{(n,+)}:n>0$}\psfrag{l}{\tiny$\ell$}\psfrag{k-l}{\tiny$k-\ell$}\psfrag{u}{\tiny$u$}\psfrag{u^*}{\tiny${u^{*}}$}\psfrag{u/u^*}{\tiny$u~{}~{}/~{}~{}u^{*}$}\psfrag{hdots}{$\dots$}\includegraphics[height=128.0374pt]{definingtangle1.eps}
Figure 11. The elements u(n,±)u_{(n,\pm)}
Proposition 23.

For (n,η)({0})×{±}(n,\eta)\in({\mathbb{N}}\cup\{0\})\times\{\pm\} and xP(n,ϵη)x\in P_{(n\ell,\epsilon\eta^{\ell})}, the following three conditions are equivalent.
(1) There exists yP(n,ϵη()k)y\in P_{(n\ell,\epsilon\eta^{\ell}(-)^{k-\ell})} such that the equation in Figure 12 holds.

\psfrag{une}{$u_{(n,\eta)}$}\psfrag{une*}{$u_{(n,\eta)}^{*}$}\psfrag{d}{$\delta^{k-\ell}$}\psfrag{nl}{\tiny$n\ell$}\psfrag{kml}{\tiny$k-\ell$}\psfrag{x}{$x$}\psfrag{y}{$y$}\includegraphics[height=85.35826pt]{xyeqn.eps}
Figure 12. Relation between xP(n,ϵη)x\in P_{(n\ell,\epsilon\eta^{\ell})} and yP(n,ϵη()k)y\in P_{(n\ell,\epsilon\eta^{\ell}(-)^{k-\ell})}

(2) There exists yP(n,ϵη()k)y\in P_{(n\ell,\epsilon\eta^{\ell}(-)^{k-\ell})} such that the equations in Figure 13 hold.

\psfrag{une}{\small$u_{(n,\eta)}$}\psfrag{une*}{\small$u_{(n,\eta)}^{*}$}\psfrag{x}{$x$}\psfrag{y}{$y$}\psfrag{d}{$\delta^{k-\ell}$}\psfrag{nl}{\tiny$n\ell$}\psfrag{kml}{\tiny$k-\ell$}\includegraphics[height=91.04872pt]{xyeqn2.eps}
Figure 13. Expressions for xx and yy in terms of each other

(3) The equation in Figure 14 holds.

\psfrag{une}{\small$u_{(n,\eta)}$}\psfrag{une*}{\small$u_{(n,\eta)}^{*}$}\psfrag{d}{\small$\delta^{-2(k-\ell)}$}\psfrag{nl}{\tiny$n\ell$}\psfrag{kml}{\tiny$k-\ell$}\psfrag{x}{$x$}\includegraphics[height=142.26378pt]{dcircle.eps}
Figure 14. The double circle relation

The proof of Proposition 23 that we give here is an adaptation of the one in [Jns1999] with a few more details included. We pave the way for the proof by defining and proving some properties of a map from P(n,ϵη)P_{(n\ell,\epsilon\eta^{\ell})} to P(n+k,ϵη)P_{(n\ell+k-\ell,\epsilon\eta^{\ell})}. Recall - see Definition 12 of [KdyMrlSniSnd2019] - that a *-planar algebra PP is said to be a CC^{*}-planar algebra if there exist positive normalised traces τ±:P(0,±)\tau_{\pm}:P_{(0,\pm)}\rightarrow{\mathbb{C}} such that all the traces τ±ZTR(0,±)\tau_{\pm}\circ Z_{TR^{(0,\pm)}} defined on P(k,±)P_{(k,\pm)} are faithful and positive. Thus all the spaces P(k,±)P_{(k,\pm)} equipped with the trace inner product are Hilbert spaces.

Lemma 24.

The map σ:P(n,ϵη)P(n+k,ϵη)\sigma:P_{(n\ell,\epsilon\eta^{\ell})}\rightarrow P_{(n\ell+k-\ell,\epsilon\eta^{\ell})} defined as in the left of Figure 15 is an isometry with adjoint σ\sigma^{*} given as in the right of Figure 15.

\psfrag{une}{\small$u_{(n,\eta)}$}\psfrag{une*}{\small$u_{(n,\eta)}^{*}$}\psfrag{d}{\small$\delta^{-(k-\ell)}$}\psfrag{nl}{\tiny$n\ell$}\psfrag{kml}{\tiny$k-\ell$}\psfrag{x}{$x$}\psfrag{z}{$z$}\psfrag{u}{\small$u_{(n,\eta)}$}\psfrag{u*}{\small$u_{(n,\eta)}^{*}$}\includegraphics[height=142.26378pt]{sigmadef.eps}
Figure 15. σ(x)\sigma(x) and σ(z)\sigma^{*}(z) for xP(n,ϵη)x\in P_{(n\ell,\epsilon\eta^{\ell})} and zP(n+k,ϵη)z\in P_{(n\ell+k-\ell,\epsilon\eta^{\ell})}

Further, both σ\sigma and σ\sigma^{*} are equivariant for the *-operations on P(n,ϵη)P_{(n\ell,\epsilon\eta^{\ell})} and P(n+k,ϵη)P_{(n\ell+k-\ell,\epsilon\eta^{\ell})}.

Proof.

Consider the maps σ\sigma and σ\sigma^{*} defined by the left and right side pictures in Figure 15 respectively. It is clear that they are equivariant for the *-operations on P(n,ϵη)P_{(n\ell,\epsilon\eta^{\ell})} and P(n+k,ϵη)P_{(n\ell+k-\ell,\epsilon\eta^{\ell})}. To show that they are actually adjoints of each other, it suffices to verify the equality of Figure 16 for arbitrary xP(n,ϵη)x\in P_{(n\ell,\epsilon\eta^{\ell})} and zP(n+k,ϵη)z\in P_{(n\ell+k-\ell,\epsilon\eta^{\ell})}.

\psfrag{une}{\small$u_{(n,\eta)}$}\psfrag{une*}{\small$u_{(n,\eta)}^{*}$}\psfrag{d}{\tiny$=$}\psfrag{nl}{\tiny$n\ell$}\psfrag{kml}{\tiny$k-\ell$}\psfrag{x}{$x$}\psfrag{z}{$z^{*}$}\psfrag{u}{\small$u_{(n,\eta)}$}\psfrag{u*}{\small$u_{(n,\eta)}^{*}$}\includegraphics[height=227.62204pt]{equality.eps}
Figure 16. Equality to be verified

This is clear by isotopy. Finally, that σσ=id\sigma^{*}\sigma=id is a simple pictorial verification using the equalities of Figure 8. \Box

From Lemma 24 it follows that E=σσE=\sigma\sigma^{*} is a projection onto ran(σ)P(n+k,ϵη)ran(\sigma)\subseteq P_{(n\ell+k-\ell,\epsilon\eta^{\ell})} that is equivariant for the *-operations. Pictorially EE is given by the picture on the left in Figure 17. We will also the need the picture on the right in Figure 17 which is the projection onto the subspace P(k,n+k,ϵη)P_{(k-\ell,n\ell+k-\ell,\epsilon\eta^{\ell})} of P(n+k,ϵη)P_{(n\ell+k-\ell,\epsilon\eta^{\ell})}, which also is *-equivariant.

\psfrag{une}{\small$u_{(n,\eta)}$}\psfrag{une*}{\small$u_{(n,\eta)}^{*}$}\psfrag{d}{\small$\delta^{-(k-\ell)}$}\psfrag{nl}{\tiny$n\ell$}\psfrag{kml}{\tiny$k-\ell$}\psfrag{x}{$x$}\psfrag{z}{}\psfrag{u}{\small$u_{(n,\eta)}$}\psfrag{u*}{\small$u_{(n,\eta)}^{*}$}\includegraphics[height=227.62204pt]{eandf.eps}
Figure 17. The projections EE and FF
Proof of Proposition 23.

(1) \Rightarrow (2) Using the relations in Figure 8, it is easy to see that the equation in Figure 12 implies those of Figure 13.
(2) \Rightarrow (3) This is clear.
(3) \Rightarrow (1) We need to see that the double circle relation of Figure 14 implies the existence of a yy satisfying the equation in Figure 12.

Observe that the picture on the left in Figure 14 is given by σFσ(x)\sigma^{*}F\sigma(x). Thus the double circle relation implies that σFσ(x)=x\sigma^{*}F\sigma(x)=x and hence (applying σ\sigma on both sides and using the definition of EE) that EFσ(x)=σ(x)EF\sigma(x)=\sigma(x). Since EE and FF are projections, norm considerations imply that ||EFσ(x)||||Fσ(x)||||σ(x)||||EF\sigma(x)||\leq||F\sigma(x)||\leq||\sigma(x)||. Therefore equality holds throughout and so Fσ(x)=σ(x)F\sigma(x)=\sigma(x). Now define yy by the first equality in Figure 13. The equation Fσ(x)=σ(x)F\sigma(x)=\sigma(x) then implies that the equation on the left of Figure 18 holds and therefore also the equation on the right.

\psfrag{une}{\small$u_{(n,\eta)}$}\psfrag{une*}{\small$u_{(n,\eta)}^{*}$}\psfrag{x}{$x$}\psfrag{y}{$y$}\psfrag{d}{$\delta^{k-\ell}$}\psfrag{nl}{\tiny$n\ell$}\psfrag{kml}{\tiny$k-\ell$}\psfrag{u}{\small$u_{(n,\eta)}$}\psfrag{u*}{\small$u_{(n,\eta)}^{*}$}\includegraphics[height=165.02606pt]{xyeqn3.eps}
Figure 18. Expressions for xx and yy in terms of each other

Finally, using the relations of Figure 8, this completes the proof. \Box

We now define subspaces Q(n,η)Q_{(n,\eta)} of (,ϵ)P(n,η){}^{(\ell,\epsilon)}P_{(n,\eta)} by Q(n,η)={x(,ϵ)P(n,η)=P(n,ϵη):The equivalent conditions (1)-(3) of Proposition 23 hold for x}Q_{(n,\eta)}=\{x\in\,\!^{(\ell,\epsilon)}\!P_{(n,\eta)}=P_{(n\ell,\epsilon\eta^{\ell})}:\hbox to0.0pt{$\displaystyle\text{The equivalent conditions (1)-(3) of Proposition \ref{xycircles} hold for~{}}x\}$\hss}

The main result of this section is the following theorem.

Theorem 25.

The subspaces Q(n,η)Q_{(n,\eta)} yield a CC^{*}-planar subalgebra QQ of (,ϵ)P{}^{(\ell,\epsilon)}P.

Proof.

In order to prove that QQ is a CC^{*}-planar subalgebra of (,ϵ)P{}^{(\ell,\epsilon)}P it is enough to prove that it is a planar subalgebra of (,ϵ)P{}^{(\ell,\epsilon)}P and that it is closed under *. Closure under * is clear from the double circle condition of Figure 14.

To verify that QQ is a planar subalgebra of (,ϵ)P{}^{(\ell,\epsilon)}P, it suffices to see that it is closed under the action of any set of ‘generating tangles’. A set of such generating tangles, albeit for the class of ‘restricted tangles’ - see [DeKdy2018] - was given in Theorem 3.5 of [KdySnd2004]. It follows easily from that result that a set of generating tangles for all tangles is given by {1(0,±)}{M(n,η),(n,η)(n,η),I(n,η)(n+1,η),E(n+1,η)(n,η):n0}{R(n,η)(n,η):n1}\{1^{(0,\pm)}\}\cup\{M_{(n,\eta),(n,\eta)}^{(n,\eta)},I_{(n,\eta)}^{(n+1,\eta)},E_{(n+1,\eta)}^{(n,\eta)}:n\geq 0\}\cup\{R^{(n,-\eta)}_{(n,\eta)}:n\geq 1\}. Here EE, MM and II are the tangles in Figure 19 below. We will show, case by case, that QQ is closed under the action of each of these tangles.

\psfrag{n}{\tiny$n$}\psfrag{*}{\tiny$*$}\psfrag{E}{\small$E_{(n+1,\eta)}^{(n,\eta)}$}\psfrag{M}{\small$M_{(n,\eta),(n,\eta)}^{(n,\eta)}$}\psfrag{I}{\small$I_{(n,\eta)}^{(n+1,\eta)}$}\includegraphics[height=71.13188pt]{commontangles.eps}
Figure 19. Conditional expectation, multiplication and inclusion tangles

Closure under 1(0,±)1^{(0,\pm)}: We need to check that Z1(0,±)((,ϵ)P)(1)=1(0,ϵ(±))Q(0,±)Z_{1^{(0,\pm)}}^{(^{(\ell,\epsilon)}P)}(1)=1_{(0,\epsilon(\pm)^{\ell})}\in Q_{(0,\pm)}. This follows directly from the double circle relation of Figure 14.

Closure under M=M(n,η),(n,η)(n,η)M=M_{(n,\eta),(n,\eta)}^{(n,\eta)}: We need to check that if x1,x2Q(n,η)x_{1},x_{2}\in Q_{(n,\eta)}, then ZM((,ϵ)P)(x1x2)=ZM(,ϵ)P(x1x2)Q(n,η)Z_{M}^{(^{(\ell,\epsilon)}P)}(x_{1}\otimes x_{2})=Z_{M^{(\ell,\epsilon)}}^{P}(x_{1}\otimes x_{2})\in Q_{(n,\eta)}. Observe that M(,ϵ)M^{(\ell,\epsilon)} is the multiplication tangle of colour (n,ϵη)(n\ell,\epsilon\eta^{\ell}). Now suppose that y1,y2P(n,ϵη()k)y_{1},y_{2}\in P_{(n\ell,\epsilon\eta^{\ell}(-)^{k-\ell})} are such that the equation in Figure 12 holds for x1,y1x_{1},y_{1} and for x2,y2x_{2},y_{2}. It is easy to see that then the same equation also holds for x1x2,y1y2x_{1}x_{2},y_{1}y_{2}.

Closure under I=I(n,η)(n+1,η)I=I_{(n,\eta)}^{(n+1,\eta)}: We need to see that if xQ(n,η)x\in Q_{(n,\eta)}, then ZI((,ϵ)P)(x)=ZPI(,ϵ)Q(n+1,η)Z_{I}^{(^{(\ell,\epsilon)}P)}(x)=Z^{P}_{I^{(\ell,\epsilon)}}\in Q_{(n+1,\eta)}. Observe that the tangle I(,ϵ)I^{(\ell,\epsilon)} is the \ell-fold iterated inclusion tangle from P(n,ϵη)P_{(n\ell,\epsilon\eta^{\ell})} to P((n+1),ϵη)P_{((n+1)\ell,\epsilon\eta^{\ell})}. Suppose that yP(n,ϵη()k)y\in P_{(n\ell,\epsilon\eta^{\ell}(-)^{k-\ell})} is such that the equation in Figure 12 holds for x,yx,y. Again, an easy verification shows that the equation in Figure 12 also holds for ZI(,ϵ)(x),ZI~(,ϵ)(y)Z_{I^{(\ell,\epsilon)}}(x),Z_{\tilde{I}^{(\ell,\epsilon)}}(y), where I~(,ϵ)\tilde{I}^{(\ell,\epsilon)} is the \ell-fold iterated inclusion tangle from P(n,ϵη()k)P_{(n\ell,\epsilon\eta^{\ell}(-)^{k-\ell})} to P((n+1),ϵη()k))P_{((n+1)\ell,\epsilon\eta^{\ell}(-)^{k-\ell}))}.

Closure under E=E(n+1,η)(n,η)E=E_{(n+1,\eta)}^{(n,\eta)}: We need to see that if xQ(n+1,η)x\in Q_{(n+1,\eta)}, then ZE((,ϵ)P)(x)Z_{E}^{(^{(\ell,\epsilon)}P)}(x) =ZPE(,ϵ)(x)Q(n,η)=Z^{P}_{E^{(\ell,\epsilon)}}(x)\in Q_{(n,\eta)}. Observe that the tangle E(,ϵ)E^{(\ell,\epsilon)} is the \ell-fold iterated conditional expectation tangle from P((n+1),ϵη)P_{((n+1)\ell,\epsilon\eta^{\ell})} to P(n,ϵη)P_{(n\ell,\epsilon\eta^{\ell})}. Take yP((n+1),ϵη()k)y\in P_{((n+1)\ell,\epsilon\eta^{\ell}(-)^{k-\ell})} such that the equation in Figure 12 holds for x,yx,y. We will verify that then, the equation in Figure 12 also holds for ZE(,ϵ)(x),ZE~(,ϵ)(y)Z_{E^{(\ell,\epsilon)}}(x),Z_{\tilde{E}^{(\ell,\epsilon)}}(y), where E~(,ϵ)\tilde{E}^{(\ell,\epsilon)} is the \ell-fold iterated conditional expectation tangle from P((n+1),ϵη()k)P_{((n+1)\ell,\epsilon\eta^{\ell}(-)^{k-\ell})} to P(n,ϵη()k))P_{(n\ell,\epsilon\eta^{\ell}(-)^{k-\ell}))}.

First note that, it is an easy consequence of the relations in Figure 8 that the relations of Figure 20 hold for all (n,η)(n,\eta).

\psfrag{nl}{\tiny$n\ell$}\psfrag{*}{\tiny$*$}\psfrag{l}{\tiny$\ell$}\psfrag{u}{\small$u_{(n,\eta)}$}\psfrag{u'}{\small$u_{(n+2,\eta)}$}\psfrag{k-l}{\tiny$k-\ell$}\psfrag{=}{\small$=$}\includegraphics[height=142.26378pt]{exprelation1.eps}
Figure 20. Consequence of {0,}\{0,\ell\}-biunitarity relations

Now, these relations, in turn, imply the equations in Figure 21. In this figure, the first and the third equalities follow from Figure 20 while the second equality is a consequence of the proof of closure under II.

\psfrag{nl}{\tiny$n\ell$}\psfrag{*}{\tiny$*$}\psfrag{x}{\small$x$}\psfrag{y}{\small$y$}\psfrag{l}{\tiny$\ell$}\psfrag{u}{\small$u_{(n,\eta)}$}\psfrag{u'}{\small$u_{(n+2,\eta)}$}\psfrag{k-l}{\tiny$k-\ell$}\psfrag{=}{\small$=$}\includegraphics[height=184.9429pt]{exprelation2.eps}
Figure 21. Proof of closure under EE

Closure under R=R(n,η)(n,η)R=R^{(n,-\eta)}_{(n,\eta)}: We need to see that if xQ(n,η)x\in Q_{(n,\eta)}, then ZR((,ϵ)P)(x)=ZPR(,ϵ)(x)Q(n,η)Z_{R}^{(^{(\ell,\epsilon)}P)}(x)=Z^{P}_{R^{(\ell,\epsilon)}}(x)\in Q_{(n,-\eta)}. We illustrate how this is done when (n,η)=(3,+)(n,\eta)=(3,+). It should be clear that the proof of the general case is similar. Begin by observing that since xQ(3,+)P(3,ϵ)x\in Q_{(3,+)}\subseteq P_{(3\ell,\epsilon)}, it satisfies the double circle relation of Figure 22.

\psfrag{nl}{\tiny$n\ell$}\psfrag{*}{\tiny$*$}\psfrag{delta}{$\delta^{-2(k-\ell)}$}\psfrag{u}{\small$u$}\psfrag{u^*}{\small$u^{*}$}\psfrag{l}{\tiny$\ell$}\psfrag{k-l}{\tiny$k-\ell$}\psfrag{x}{\small$x$}\psfrag{=}{\small$=$}\includegraphics[height=147.95424pt]{3casedoublecircle.eps}
Figure 22. Double circle relation for xQ(3,+)x\in Q_{(3,+)}

Now, moving the external * \ell steps counterclockwise and redrawing yields the equation in Figure 23.

\psfrag{nl}{\tiny$n\ell$}\psfrag{*}{\tiny$*$}\psfrag{delta}{$\delta^{-2(k-\ell)}$}\psfrag{u}{\small$u$}\psfrag{u^*}{\small$u^{*}$}\psfrag{l}{\tiny$\ell$}\psfrag{k-l}{\tiny$k-\ell$}\psfrag{x}{\small$x$}\psfrag{=}{\small$=$}\includegraphics[height=147.95424pt]{3casedoublecircley.eps}
Figure 23. Rotated double circle relation for xQ(3,+)x\in Q_{(3,+)}

A little thought now shows that this is precisely the double circle relation for ZPR(,ϵ)(x)P(3,ϵ())Z^{P}_{R^{(\ell,\epsilon)}}(x)\in P_{(3\ell,\epsilon(-)^{\ell})}, establishing that ZPR(,ϵ)(x)Z^{P}_{R^{(\ell,\epsilon)}}(x) indeed belongs to Q(3,)Q_{(3,-)} as desired. \Box

Next we will consider conditions under which QQ is a subfactor planar algebra.

Proposition 26.

Let PP be the spin planar algebra on nn generators and QQ be the planar subalgebra of (,ϵ)P{}^{(\ell,\epsilon)}P corresponding to a {0,}\{0,\ell\}-biunitary element uP(k,ϵ)u\in P_{(k,\epsilon)}. Then, QQ is a subfactor planar algebra with modulus (n)(\sqrt{n})^{\ell}.

Proof.

Given Theorem 25, what remains to be seen is that QQ is connected, has modulus (n)(\sqrt{n})^{\ell} and is spherical with positive definite picture trace. Since PP has modulus n\sqrt{n}, the cabling (,ϵ)P{}^{(\ell,\epsilon)}P has modulus (n)(\sqrt{n})^{\ell} and so does QQ. The other assertions need a little work.

Note that Q(0,η)Q_{(0,\eta)} is a subspace of ((,ϵ)P)(0,η)=P(0,ϵη)(^{(\ell,\epsilon)}P)_{(0,\eta)}=P_{(0,\epsilon\eta^{\ell})} and so if ϵη=+\epsilon\eta^{\ell}=+, then Q(0,η)Q_{(0,\eta)} is 1-dimensional since P(0,+)P_{(0,+)} is so. If ϵη=\epsilon\eta^{\ell}=-, then, Q(0,η)Q_{(0,\eta)} is the subspace of all xP(0,)x\in P_{(0,-)} such that the double circle relation of Figure 14 holds for xx. From Theorem 2, a basis of P(0,)P_{(0,-)} is given by all S(i)S(i) for i=1,,ni=1,\cdots,n and by the black and white modulus relations, a double circle around these gives a scalar multiple of 1(0,)1^{(0,-)}. It follows that xx is necessarily a scalar multiple of 1(0,)1^{(0,-)} so that Q(0,η)Q_{(0,\eta)} is 1-dimensional, in this case as well. Hence QQ is connected.

To see that QQ is spherical, observe first that on any P(n,η)P_{(n,\eta)} the composites of the left and right picture traces with the traces τ±\tau_{\pm} on P(0,±)P_{(0,\pm)} (which specify its CC^{*}-planar algebra structure - see Definition 12 of [KdyMrlSniSnd2019]) are equal. This is seen by explicit computation with the bases of P(n,η)P_{(n,\eta)} and can be regarded as a version of sphericality for PP. It is clear that this property descends to QQ.

Finally observe that the picture trace on Q(n,η)Q_{(n,\eta)} is exactly the composite of τ±\tau_{\pm} with the picture trace on P(n,ϵη)P_{(n\ell,\epsilon\eta^{\ell})} and is consequently positive definite. \Box

Remark 27.

In particular, Hadamard matrices, quantum Latin squares and biunitary matrices all yield subfactor planar algebras via this construction. It is not clear, however, how to get a subfactor planar algebra from a unitary error basis.

Remark 28.

An even easier proof than that of Proposition 26 shows that if PP is a subfactor planar algebra and QQ is the planar subalgebra of (,ϵ)P{}^{(\ell,\epsilon)}P corresponding to a {0,}\{0,\ell\}-biunitary element uP(k,ϵ)u\in P_{(k,\epsilon)}, then, QQ is a subfactor planar algebra with modulus (n)(\sqrt{n})^{\ell}.

In case =1\ell=1, the planar algebra QQ is even irreducible.

Proposition 29.

Let PP be the spin planar algebra on nn generators and QQ be the planar subalgebra of (1,ϵ)P{}^{(1,\epsilon)}P corresponding to a {0,1}\{0,1\}-biunitary element uP(k,ϵ)u\in P_{(k,\epsilon)}. Then, QQ is an irreducible subfactor planar algebra.

Proof.

Only the irreducibility of QQ needs to be seen and we will show using explicit bases computations that dim(Q(1,+))=1dim(Q_{(1,+)})=1. We only consider the ϵ=+\epsilon=+ case, the proof in the other case being similar. Thus Q(1,+)P(1,+)Q_{(1,+)}\subseteq P_{(1,+)}. Begin with x=iλie(i]Q(1,+)x=\sum_{i}\lambda_{i}e(i]\in Q_{(1,+)}. The double circle relation for xx implies that the equation of Figure 4 holds.

\psfrag{une}{\small$u$}\psfrag{une*}{\small$u^{*}$}\psfrag{d}{\small$\sum_{i}\lambda_{i}(\sqrt{n})^{-2(k-1)}$}\psfrag{nl}{\tiny$$}\psfrag{kml}{\tiny k-1}\psfrag{x}{x}\psfrag{s1}{\tiny s_{i}}\includegraphics[height=142.26378pt]{irredproof.eps}
Figure 24. Equationsatisfiedbyx

Now, using the biunitarity relations of Figure 8 together with the black and white modulus relations, the left hand side of Figure 4 simplifies to 1niλi1(1,+)\frac{1}{n}\sum_{i}\lambda_{i}1_{(1,+)}, finishing the proof. \Box

Remark 30.

The proof of Theorem 25 relies heavily on Proposition 23, and in particular, the double circle relation, which uses the assumption that PP is a spherical CC^{*}-planar algebra. However, even if PP is just a *-planar algebra, without the positivity conditions or sphericality holding, QQ can still be shown to be a *-planar subalgebra of PP. The proof is a little longer using a different larger set of generating tangles.

5. The planar algebra associated to a finite group Latin square

Throughout this section, GG will be a finite group of order nn. Associated to GG is its multiplication table which is an n×nn\times n Latin square and consequently yields - see Example 11 - a quantum Latin square of size nn. If PP is the spin planar algebra on nn generators, this quantum Latin square gives, by Theorem 17(2), a {0,1}\{0,1\}-biunitary element in P(3,+)P_{(3,+)}. Applying the construction of Theorem 25 to this biunitary element, we get an irreducible subfactor planar algebra. The main result of this section identifies this planar algebra with the well known group planar algebra P(G)P(G) - see [Lnd2002].

We begin with a notational convention. The generating set for the spin planar algebra is the underlying set of the group GG and we will use notation such as e[g)h1hmk1km(]e[g)^{h_{1}\cdots h_{m}}_{k_{1}\cdots k_{m}}(\ell] for g,hi,kj,Gg,h_{i},k_{j},\ell\in G to denote basis elements of PP. With this notation, the {0,1}\{0,1\}-biunitary element uP(3,+)u\in P_{(3,+)} corresponding to the multiplication table of the group GG is seen to be given by

u=h,kekhk(h]P(3,+),u=\sum_{h,k}e^{kh}_{k}(h]\in P_{(3,+)},

according to Theorem 17(2).

Let QQ be the planar subalgebra of PP corresponding to the biunitary element uu as in Theorem 25. The next proposition identifies QQ and we sketch a proof leaving out most of the computational details.

Proposition 31.

The planar algebra QQ is isomorphic to P(G)P(G).

Proof.

The planar algebra P(G)P(G) has a presentation by generators and relations. We show that it is isomorphic to QQ in a series of steps - (1) computing the dimensions of the spaces of QQ and observing that these are equal to those of the spaces of P(G)P(G), (2) by specifying a map from the universal planar algebra on L=L(2,+)=GL=L_{(2,+)}=G to QQ and checking that the relations hold in QQ, thereby yielding a planar algebra map from P(G)P(G) to QQ and (3) verifying that this map is surjective.

Step 1: We first observe that for m1m\geq 1, the elements u(2m,+)u_{(2m,+)} and u(2m+1,+)u_{(2m+1,+)} are given explicitly by:

u(2m,+)\displaystyle u_{(2m,+)} =\displaystyle= g,h1,,hmeg,h11,,hm1gh1,gh2,,ghm,g\displaystyle\sum_{g,h_{1},\cdots,h_{m}}e^{g,h_{1}^{-1},\cdots,h_{m}^{-1}}_{gh_{1},gh_{2},\cdots,gh_{m},g}
u(2m+1,+)\displaystyle u_{(2m+1,+)} =\displaystyle= g,h1,,hm+1eg,h11,,hm1gh1,gh2,,ghm+1(hm+11]\displaystyle\sum_{g,h_{1},\cdots,h_{m+1}}e^{g,h_{1}^{-1},\cdots,h_{m}^{-1}}_{gh_{1},gh_{2},\cdots,gh_{m+1}}(h_{m+1}^{-1}]

Now consider elements x,yP(2m,+)x,y\in P_{(2m,+)} given by:

x\displaystyle x =\displaystyle= k1,,km,1,,mα(k1,,km,1,,m)ek1,,km1,,m\displaystyle\sum_{k_{1},\cdots,k_{m},\ell_{1},\cdots,\ell_{m}}\alpha_{(k_{1},\cdots,k_{m},\ell_{1},\cdots,\ell_{m})}e^{k_{1},\cdots,k_{m}}_{\ell_{1},\cdots,\ell_{m}}
y\displaystyle y =\displaystyle= k1,,km,1,,mβ(k1,,km,1,,m)ek1,,km1,,m,\displaystyle\sum_{k_{1},\cdots,k_{m},\ell_{1},\cdots,\ell_{m}}\beta_{(k_{1},\cdots,k_{m},\ell_{1},\cdots,\ell_{m})}e^{k_{1},\cdots,k_{m}}_{\ell_{1},\cdots,\ell_{m}},

for α(k1,,km,1,,m),β(k1,,km,1,,m)\alpha_{(k_{1},\cdots,k_{m},\ell_{1},\cdots,\ell_{m})},\beta_{(k_{1},\cdots,k_{m},\ell_{1},\cdots,\ell_{m})}\in{\mathbb{C}}. The condition that x,yx,y satisfy the condition in Figure 12 is seen to imply that for all gGg\in G,

α(k1,,km,1,,m)=α(gk1,,gkm,g1,,gm).\alpha_{(k_{1},\cdots,k_{m},\ell_{1},\cdots,\ell_{m})}=\alpha_{(gk_{1},\cdots,gk_{m},g\ell_{1},\cdots,g\ell_{m})}.

Conversely, if this condition holds, setting β(k1,,km,1,,m)=α(k11,,km1,11,,m1)\beta_{(k_{1},\cdots,k_{m},\ell_{1},\cdots,\ell_{m})}=\alpha_{(k_{1}^{-1},\cdots,k_{m}^{-1},\ell_{1}^{-1},\cdots,\ell_{m}^{-1})}, the elements xx and yy are checked satisfy the condition in Figure 12.

Thus, a basis of Q(2m,+)Q_{(2m,+)} is given by the set of all

gGegk1,,gkmg1,,gm\sum_{g\in G}e^{gk_{1},\cdots,gk_{m}}_{g\ell_{1},\cdots,g\ell_{m}}

as (k1,,km,1,,m)(k_{1},\cdots,k_{m},\ell_{1},\cdots,\ell_{m}) vary over the representatives of the diagonal action of GG on G2mG^{2m}. It follows that the dimension of Q(2m,+)Q_{(2m,+)} is given by n2m1n^{2m-1} and a similar proof shows that the dimension of Q(2m+1,+)Q_{(2m+1,+)} is given by n2mn^{2m}.

Step 2: Next we define a map from the universal planar algebra on the label set L=L(2,+)=GL=L_{(2,+)}=G to QQ given by sending gGg\in G to

Xg=qGeqqgQ(2,+).X_{g}=\sum_{q\in G}e^{q}_{qg}\in Q_{(2,+)}.

A long but routine verification - which we omit entirely - establishes that all relations satisfied by the gGg\in G in the planar algebra P(G)P(G) also hold for their images XgX_{g} in QQ thus giving a planar algebra map from P(G)P(G) to QQ.

\psfrag{une}{\small$u$}\psfrag{une*}{\small$u^{*}$}\psfrag{d}{\small$\sum_{i}\lambda_{i}(\sqrt{n})^{-2(k-1)}$}\psfrag{nl}{\tiny$$}\psfrag{kml}{\tiny k-1}\psfrag{x}{x}\psfrag{s1}{\tiny s_{i}}\psfrag{k1}{\tiny k_{1}}\psfrag{k2}{\tiny k_{2}}\psfrag{k3}{\tiny k_{3}}\psfrag{kmm1}{\tiny k_{m-1}}\psfrag{km}{\tiny k_{m}}\psfrag{l1}{\tiny\ell_{1}}\psfrag{l2}{\tiny\ell_{2}}\psfrag{l3}{\tiny\ell_{3}}\psfrag{lmm1}{\tiny\ell_{m-1}}\psfrag{lm}{\tiny\ell_{m}}\psfrag{cdots}{\cdots}\includegraphics[height=113.81102pt]{basiselt.eps}
Figure 25. A