Bipartite polygon models: entanglement classes and their nonlocal behaviour

Mayalakshmi Kolangatt1, Thigazholi Muruganandan1, Sahil Gopalkrishna Naik2, Tamal Guha3, Manik Banik2, and Sutapa Saha4,5

1School of Physics, IISER Thiruvananthapuram, Vithura, Kerala 695551, India.
2Department of Physics of Complex Systems, S.N. Bose National Center for Basic Sciences, Block JD, Sector III, Salt Lake, Kolkata 700106, India.
3Department of Computer Science, The University of Hong Kong, Pokfulam road 999077, Hong Kong.
4Department of Astrophysics and High Energy Physics, S.N. Bose National Center for Basic Sciences, Block JD, Sector III, Salt Lake, Kolkata 700106, India.
5Harish-Chandra Research Institute, HBNI, Chhatnag Road, Jhunsi, Allahabad 211 019, India.

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Abstract

Hardy's argument constitutes an elegantly logical test for identifying nonlocal features of multipartite correlations. In this paper, we investigate Hardy's nonlocal behavior within a broad class of operational theories, including the qubit state space as a specific case. Specifically, we begin by examining a wider range of operational models with state space descriptions in the form of regular polygons. First, we present a systematic method to characterize the possible forms of entangled states within bipartite compositions of these models. Then, through explicit examples, we identify the classes of entangled states that exhibit Hardy-type nonlocality. Remarkably, our findings highlight a closer analogy between odd polygon models and the qubit state space in terms of their bipartite Hardy nonlocal behavior compared to even-sided polygons. Furthermore, we demonstrate that the emergence of mixed-state Hardy nonlocality in any operational model is determined by a specific symmetry inherent in its dynamic description. Finally, our results uncover an unexplored class of almost-quantum correlations that can be associated with an explicit operational model.

Among various formulations of nonlocality tests, one of the most elegant demonstrations
of quantum nonlocality comes without inequalities, as proposed by Lucian Hardy. Unlike
the celebrated Bell-CHSH test, in the two-qubit scenario, this signature of nonlocality is
uniquely exhibited by pure entangled states. But what is so special about the topology of
the qubit state space? Why not Hardy’s nonlocal argument is robust even with a vanishing
presence of product qubit noises?
This work highlights a key feature of single quanta: the one-to-one correspondence be-
tween their preparation and measurement devices, which leads to such an extreme noise
sensitivity of Hardy’s nonlocal phenomenon in bipartite systems. Moreover, the result ex-
tends to a broader class of operational probabilistic models, encompassing both classical
and quantum theories. This generalization offers theory-independent predictive capability
for identifying noise-robust Hardy-type nonlocal signatures in any operational theory with
exactly two simultaneously distinguishable pure preparations.

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[2] Samrat Sen, Edwin Peter Lobo, Ram Krishna Patra, Sahil Gopalkrishna Naik, Anandamay Das Bhowmik, Mir Alimuddin, and Manik Banik, "Timelike correlations and quantum tensor product structure", Physical Review A 106 6, 062406 (2022).

[3] Ryo Takakura, "Optimal CHSH values for regular polygon theories in generalized probabilistic theories", Journal of Physics A Mathematical General 57 37, 375305 (2024).

[4] Anna Steffinlongo, Nicola D'Alessandro, and Martin J. Renner, "Almost all pure entangled states enable unbounded nonlocality sharing", arXiv:2607.24700, (2026).

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