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bibkey: negami2026middle authors: H. Negami year: 2026 title: “Quantum gates from the middle convolution of twisted Burau representations” doi: 10.48550/arXiv.2610.00293 url: https://arxiv.org/abs/2610.00293v1 claim: “Problem 6.8, last sentence: prove the Jordan obstruction for the Jones-Temperley-Lieb endpoint-sector seeds of Remark 6.7(b), whose ambient Long-Moody braid matrices were found numerically to have non-trivial Jordan blocks.” strata_touched:

  • D5/S3/Quantum/Algebra/JonesTemperleyLiebLongMoodyJordanObstruction license: citation-only triage: anchor

Quantum gates from the middle convolution of twisted Burau representations

H. Negami, arXiv:2610.00293v1 (2026-09-25), quant-ph, cross-listed math-ph; only v1 exists. Theorem-like environments share one counter per section: Remark 6.7 and Problem 6.8 are in §6.1.1 (Open questions: irreducibility and image closure).

The open item, verbatim (Problem 6.8, last sentence):

Also prove the Jordan obstruction for the Jones–Temperley–Lieb endpoint-sector seeds in Remark~\ref{rem:numerics}(b).

The summary table row for these seeds ends:

Finite-precision tests suggest Jordan blocks and show large norms of sampled words. An exact obstruction remains open.

Remark 6.7(b), verbatim excerpts:

let be the Hilbert space with orthonormal basis the length- paths on the graph starting at its left endpoint; the usual path-model Temperley–Lieb operators satisfy

E_i^2=\delta_\ell E_i,\qquad \delta_\ell=2\cos(\pi/\ell).

\rho(\sigma_i)=\alpha_\ell I+\beta_\ell E_i,\qquad \alpha_\ell=i e^{-\pi i/(2\ell)},\qquad \beta_\ell=\alpha_\ell^{-1},

with no additional scalar twist; thus .

The terminal vertex of a path is preserved, so is the orthogonal direct sum of its \emph{endpoint sectors}; these are the sectors used below.

We restrict each endpoint sector of the representation to as in Section~\ref{subsec:klm}, and use that restriction as the KLM seed.

The ancillary script checks every endpoint sector of dimension at least two for , , and for , . It tests the ambient LM braid matrices \eqref{eq:braid-matrices} only in sectors for which its numerical kernel test gives ; otherwise it reports the kernel dimension and skips the sector, without forming a quotient. Finite-precision rank tests suggest the presence of non-trivial Jordan blocks, and sampled random words of length have large operator norms, of orders –. These finite-precision observations motivate an exact Jordan obstruction; by themselves they establish neither non-semisimplicity nor unboundedness.

The identification (Definition 1.7), the Long–Moody operators (Definition 1.4, Eq. eq:braid-matrices) and (Definition 1.5), verbatim:

and .

S_i&:=\rho^{\mathrm{LM}}\lambda(\sigma_i) =s_i^{\oplus n} \begin{pmatrix} I{N(i-1)}&0&0\ 0&R_i&0\ 0&0&I_{N(n-i-1)} \end{pmatrix},\[2pt] R_i&:=\begin{pmatrix}0&g_i\I_N&I_N-g_{i+1}\end{pmatrix}.

K&:={(v_1,\ldots,v_n)\in V^{\oplus n}:\ v_j\in\Ker(g_j-I_N)\text{ for every }j},

Here and ; the generators of are and .

Verified locator

DOI: 10.48550/arXiv.2610.00293. Canonical source URL: https://arxiv.org/abs/2610.00293v1. Problem 6.8 and Remark 6.7 are in §6.1.1; the Long–Moody operators are Eq. eq:braid-matrices (Definition 1.4), is in Definition 1.5 and the identification is in Definition 1.7.