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Physical Review A

Better bounds on finite-order Grothendieck constants with applications to Bell nonlocality

Sébastien Designolle, Tamás Vértesi, Sebastian Pokutta

Published Dec 10, 2025• 1 citation
Publisher
DOI
10.1103/m5mn-c5dx

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Grothendieck constants KG(d)K_G(d)KG​(d) bound the advantage of ddd-dimensional strategies over 111-dimensional ones in a specific optimisation task. They have applications ranging from approximation algorithms to quantum nonlocality. However, apart from d=2d=2d=2, their values are unknown. Here, we exploit a recent Frank-Wolfe approach to provide good candidates for lower bounding some of these constants. The complete proof relies on solving difficult binary quadratic optimisation problems. For d∈{3,4,5}d\in\{3,4,5\}d∈{3,4,5}, we construct specific rectangular instances that we can solve to certify better bounds than those previously known; by monotonicity, our lower bounds improve on the state of the art for d⩽9d\leqslant9d⩽9. For d∈{4,7,8}d\in\{4,7,8\}d∈{4,7,8}, we exploit elegant structures to build highly symmetric instances achieving even greater bounds; however, we can only solve them heuristically. We also recall the standard relation with violations of Bell inequalities and elaborate on it to interpret generalised Grothendieck constants KG(d↦2)K_G(d\mapsto2)KG​(d↦2) as the advantage of complex ddd-dimensional quantum mechanics over real qubit quantum mechanics. Motivated by this connection, we also improve the bounds on KG(d↦2)K_G(d\mapsto2)KG​(d↦2).
We relate the nonlocal properties of noisy entangled states to Grothendieck's constant, a mathematical constant appearing in Banach space theory. For two-qubit Werner states ${\ensuremath{\rho}}_{p}^{W}=p\ensuremath{\mid}{\ensuremath{\psi}}^{\ensuremath{-}}⟩⟨{\ensuremath{\psi}}^{\ensuremath{-}}\ensuremath{\mid}+(1\ensuremath{-}p)\mathbb{1}∕4$, we show that there is a local model for projective measurements if and only if $p\ensuremath{\leqslant}1∕{K}_{G}(3)$, where KG(3){K}_{G}(3)KG​(3) is Grothendieck's constant of order 3. Known bounds on KG(3){K}_{G}(3)KG​(3) prove the existence of this model at least for $p\ensuremath{\lesssim}0.66$, quite close to the current region of Bell violation, $p\ensuremath{\sim}0.71$. We generalize this result to arbitrary quantum states.
We propose candidate lower bounds on the real Grothendieck constants KG(d)K_{\mathrm G}(d)KG​(d) and their infinite-dimensional limit KGK_{\mathrm G}KG​ using rotationally invariant cubic kernels. For the continuous construction, we identify an explicit threshold above which hemispherical binary strategies are unstable under cubic boundary deformations. Supported by numerical evidence, we conjecture that hemispherical strategies are globally optimal at this threshold. This conjecture would imply KG≥9π/16≃1.767146K_{\mathrm G}\geq9π/16\simeq1.767146KG​≥9π/16≃1.767146, improving the rigorous lower bound 6π/11≃1.7135966π/11\simeq1.7135966π/11≃1.713596. We also construct finite symmetric coefficient matrices from unit vectors in dimensions up to 242424. Large-scale see-saw optimization supports the continuous predictions and suggests improved lower bounds on KG(d)K_{\mathrm G}(d)KG​(d) in the studied dimensions from 444 to 242424, conditional on the conjectured binary optima being exact. Selected matrices also yield finite-setting candidate dimension witnesses when interpreted as bipartite correlation Bell functionals. If the corresponding binary upper bounds hold, these witnesses would certify a local Hilbert-space dimension of at least five for each party.