Higher invariants of complex Hadamard matrices

Primarily AI-generated textHuman understanding: some partsmath.OA — Operator Algebrasmath.QA — Quantum Algebra

Contributed by Teo Banica ↗

Version 1 / Nov 13, 2026 / CC BY 4.0

Abstract

Associated to any complex Hadamard matrix H∈MN(T)H\in M_N(\mathbb T) is a quantum permutation group G⊂uSN+G\subset_uS_N^+, the Hopf image of the representation associated to the magic matrix formed by the rank 1 projections Pij=Proj(Hi/Hj)P_{ij}=Proj(H_i/H_j), and its invariants ck=dim⁡(Fix(u⊗k))c_k=\dim(Fix(u^{\otimes k})) are the dimensions of the relative commutants of the subfactor associated to HH. We compute these invariants well beyond the levels k=2,3k=2,3 previously known, up to k=9k=9 in the best cases, by using Jones--Wenzl and annular decompositions. For the Di\c t\u a deformations of the Fourier matrices we compute GG for all values of the parameters, and we study the order 8 families F8,5F_{8,5}, in connection with free wreath products. For the matrices of small order with c2=2c_2=2, such as the Karlsson ones at generic parameters, we find ck=Catkc_k=Cat_k at all the levels computed. Finally, via an integrality principle and character sums, we prove that the Paley II matrices, and more generally those coming from symmetric conference matrices, have infinite depth, as well as the Paley I matrices with 11≤q<10511\leq q<10^5.

Provenance statement

Written by Claude Opus, with help from Teo Banica.

Tools used

Anthropic
Claude Opus

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Version history

  1. v1 · 58 pagesSubmitted by Teo BanicaInitial depositCurrentNov 13, 2026