Abstract
After recalling the notion of higher roots (or hyper-roots) associated with “quantum modules” of type (G, k), for G a semi-simple Lie group and k a positive integer, following the definition given by A. Ocneanu in 2000, we study the theta series of their lattices. Here we only consider the higher roots associated with quantum modules (aka module-categories over the fusion category defined by the pair (G, k)) that are also “quantum subgroups.” For G = SU(2) the notion of higher roots coincides with the usual notion of roots for ADE Dynkin diagrams and the self-fusion restriction (the property of being a quantum subgroup) selects the diagrams of type Ar, Dr with r even, E6 and E8; their theta series are well known. In this paper we take G = SU(3), where the same restriction selects the modules \({\mathcal A}_k\), \({\mathcal D}_k\) with mod(k, 3) = 0, and the three exceptional cases \({\mathcal E}_5\), \({\mathcal E}_9\) and \({\mathcal E}_{21}\). The theta series for their associated lattices are expressed in terms of modular forms twisted by appropriate Dirichlet characters.
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Notes
- 1.
- 2.
Of course they are not Dynkin diagrams.
- 3.
It is defined by a monoidal functor from \({\mathcal A}_k\) to the category of endofunctors of an abelian category \({\mathcal E}\), [27]. Terminological warning: a module-category is usually not a modular category!
- 4.
The Fn are sometimes called “annular matrices” when \({\mathcal A}_k\) and \({\mathcal E}_k\) are distinct (if they are the same, then Fn = Nn), and the τa are sometimes called (by the author) “essential matrices.”
- 5.
The adjacency matrices of the graphs given at the end of the introduction are precisely the (unextended) matrices F(1,0).
- 6.
This is the shifted Weyl action: w ⋅ n = w(n + ρ) − ρ where ρ is the Weyl vector.
- 7.
The terminology “ribbon” comes from A. Ocneanu.
- 8.
The number of higher roots for \({\mathcal A}_k (\mathrm {SU}(3))\) is therefore also given by the number of 3-cycles in the rook graph \(M_N=K_N \square K_N\), the Cartesian square of the complete graph KN on N vertices (one recognizes the A288961 sequence of the OEIS [26]).
- 9.
- 10.
Using Eq. (4) one could define a periodic inner product on \(\Lambda \times _{\mathcal Z}{\mathcal E}\) that would not be positive definite because of the periodicity, but we consider directly its non-degenerate quotient, naturally defined on the ribbon \(D \times _{\mathcal Z}{\mathcal E}\).
- 11.
With G = SU(2), one recovers the fact that roots of simply laced Dynkin diagrams have norm 2 and that the inner product of two roots can be written as a sum of two fusion coefficients.
- 12.
This general result was claimed in the last two slides of [23] and it can be explicitly checked in all the cases that we consider below.
- 13.
This parameter q is not related to the root of unity, called athfrak q, that appears in Sect. 2.2.
- 14.
As Γ1(ℓ) ⊂ Γ0(ℓ), one can sometimes use modular forms (and bases of spaces of modular forms) twisted by Dirichlet characters on the congruence subgroup Γ1(ℓ).
- 15.
In the table, the subscript x of Γx may be 0 or 1 (see footnote 10) and the entry kiss gives the smallest term of the theta series, its coefficient being the kissing number.
- 16.
Its expression in terms of the elliptic theta function 𝜗3 reads:
$$\displaystyle \begin{aligned} \begin{array}{rcl} \theta(z) & =&\displaystyle \frac{\vartheta _3(0,q){}^3+\vartheta _3\left(\frac{\pi }{3},q\right){}^3+\vartheta _3\left(\frac{2 \pi }{3},q\right){}^3}{3 \vartheta _3\left(0,q^3\right)}. \end{array} \end{aligned} $$
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Coquereaux, R. (2023). SU(3) Higher Roots and Their Lattices. In: Flandrin, P., Jaffard, S., Paul, T., Torresani, B. (eds) Theoretical Physics, Wavelets, Analysis, Genomics. Applied and Numerical Harmonic Analysis. Birkhäuser, Cham. https://doi.org/10.1007/978-3-030-45847-8_11
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