Metadata
bibkey: denkerimaiguhne2025chiral
authors: Sophia Denker; Satoya Imai; Otfried Gühne
year: 2025
title: "Chiral Symmetries and Multiparticle Entanglement"
doi: null
url: https://arxiv.org/abs/2506.15609v1
claim: "The paper constructs highly entangled three-qudit subspaces from chiral and flip-conjugate symmetries, shows that all states of the flip-conjugate symmetric subspace are local-unitary equivalent, proves the bound G >= 1 - d/(d^2-1) for their geometric measure, and conjectures from numerics for d <= 12 that G = 1 - d^2/((d^2-1)(d+1)) for every state of the subspace."
strata_touched:
- D5/S3/Quantum/Entanglement/GeometricMeasure/FlipConjugateGeometricMeasure
license: citation-only
triage: anchor
Chiral Symmetries and Multiparticle Entanglement
S. Denker, S. Imai and O. Gühne, arXiv:2506.15609v1 (2025-06-18). Quotations are from the v1 TeX source.
The geometric measure:
The quantity is known as the \textit{geometric measure of entanglement} and can be directly extended to the multiparticle case
particles defined as .
The flip-conjugate symmetric subspace:
\ket{\phi_n} &= \frac{1}{\sqrt{d+1}} \left (z_d^*\sum_{i=0}^{d-1}\ket{ini}+z_d\sum_{i=0}^{d-1}\ket{iin} \right)
with . Analogously, the complex conjugate vectors span a flip-conjugate symmetric subspace as well (denoted ).
The conjecture:
\textbf{Conjecture:}\textit{ The geometric measure of entanglement for any state in the flip-conjugate symmetric subspace (and respectively ) is given by G(\ket{\psi}) = 1-\frac{d^2}{(d^2-1)(d+1)}, where denotes the local dimension, which coincides with the dimension of the subspace. }
Verified locator
Source: https://arxiv.org/abs/2506.15609v1
- URL: https://arxiv.org/abs/2506.15609v1 (source
paper-plan.tex, md52340b0f14e9e557cbd8cae8020fe909a):- the geometric measure, l. 196–206 and l. 262–265;
- the subspace, l. 625–638 and l. 1426–1431;
- the local-unitary proposition, l. 1435–1449;
- the conjecture, l. 1451–1460.