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arXiv:2605.12828

The Quad-$C_5$ Graph: Maximum Contextuality Gap on Eight Vertices

Ugur Tamer, Özgür E. Müstecaplıoğlu, Alper Dizdar, Zafer Gedik

quant-phSubmitted May 12, 2026• Announced May 14, 2026• 0 citations• Revised May 31, 2026 (v2)
v1 · May 12, 2026v2 · May 31, 2026v3 · Sep 29, 2026
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Abstract

Quantum contextuality rules out classical descriptions in which measurement outcomes are independent of the compatible measurements performed alongside them. While the KCBS pentagon provides the minimal qutrit test, identifying larger but still compact contextuality witnesses remains important for understanding how contextuality can be organized, amplified, and benchmarked. We solve the eight-event version of this problem within the graph-theoretic framework for contextuality. An exhaustive search over all 11,117 connected non-isomorphic graphs with eight vertices identifies a sparse ten-edge graph, which we call Quad-$C_5$, as the maximum-gap witness. The graph has a larger absolute contextuality gap than the Wagner graph, a standard eight-vertex benchmark, despite having fewer exclusivity relations. Its structure is transparent: it is formed from four overlapping KCBS pentagons, with each edge shared by two pentagons. We prove that Quad-$C_5$ is already contextual for a single qutrit by giving an explicit three-dimensional construction. In this qutrit realization its contextuality margin equals that of KCBS, whereas its full quantum advantage is reached numerically in four dimensions and exceeds that of the Wagner graph. Quad-$C_5$ therefore provides a compact bridge between minimal qutrit contextuality and stronger four-dimensional contextuality witnesses.

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The Quad-C5C_5C5​ Graph: Maximum Contextuality Gap on Eight Vertices
Quantum contextuality rules out classical descriptions in which measurement outcomes are independent of the compatible measurements performed alongside them. While the KCBS pentagon provides the minimal qutrit test, identifying larger but still compact contextuality witnesses remains important for understanding how contextuality can be organized, amplified, and benchmarked. We solve the eight-event version of this problem within the graph-theoretic framework for contextuality. An exhaustive search over all 11,117 connected non-isomorphic graphs with eight vertices identifies a sparse ten-edge graph, which we call Quad-C5C_5C5​, as the maximum-gap witness. The graph has a larger absolute contextuality gap than the Wagner graph, a standard eight-vertex benchmark, despite having fewer exclusivity relations. Its structure is transparent: it is formed from four overlapping KCBS pentagons, with each edge shared by two pentagons. We prove that Quad-C5C_5C5​ is already contextual for a single qutrit by giving an explicit three-dimensional construction. In this qutrit realization its contextuality margin equals that of KCBS, whereas its full quantum advantage is reached numerically in four dimensions and exceeds that of the Wagner graph. Quad-C5C_5C5​ therefore provides a compact bridge between minimal qutrit contextuality and stronger four-dimensional contextuality witnesses.
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We present a study of quantum contextuality of three-dimensional mixed states for the Klyachko-Can-Binicio\ifmmode \breve{g}\else \u{g}\fi{}lu-Shumovsky (KCBS) and the Kurzy\ifmmode \acute{n}\else \'{n}\fi{}ski-Kaszlikowski (KK) noncontextuality inequalities. For any class of states whose eigenvalues are arranged in decreasing order, a universal set of measurements always exists for the KK inequality, whereas none exists for the KCBS inequality. This difference can be reflected from the spectral distribution of the overall measurement matrix. Our results would facilitate the error analysis for experimental setups, and our spectral method in the paper combined with graph theory could be useful in future studies on quantum contextuality.
Klyachko–Can–Binicioglu–Shumovsky (KCBS) inequality is a Bell-like inequality,the violation of which can be used to confirm the existence of quantum contextuality.However,the imperfection of detection efficiency may cause the so-called loophole in actual KCBS’s experiments.We derive an alternative KCBS inequality to deal with the loophole in actual KCBS’s experiments.We prove that if the experimental data violate this KCBS inequality,the loophole-free violation of the original KCBS inequality will occur.We show that the minimum detection efficiency needed for a loophole-free violation of the KCBS inequality is about 0.9738.
Klyachko—Can—Binicioğlu—Shumovsky (KCBS) inequality is a Bell-like inequality, the violation of which can be used to confirm the existence of quantum contextuality. However, the imperfection of detection efficiency may cause the so-called loophole in actual KCBS's experiments. We derive an alternative KCBS inequality to deal with the loophole in actual KCBS's experiments. We prove that if the experimental data violate this KCBS inequality, the loophole-free violation of the original KCBS inequality will occur. We show that the minimum detection efficiency needed for a loophole-free violation of the KCBS inequality is about 0.9738.
We show that the maximum quantum violation of the Klyachko-Can-Binicioğlu-Shumovsky (KCBS) inequality is exactly the maximum value satisfying the following principle: The sum of probabilities of pairwise exclusive events cannot exceed 1. We call this principle "global exclusivity," since its power shows up when it is applied to global events resulting from enlarged scenarios in which the events in the inequality are considered jointly with other events. We identify scenarios in which this principle singles out quantum contextuality, and show that a recent proof excluding nonlocal boxes follows from the maximum violation imposed by this principle to the KCBS inequality.
In this paper we analyze the notion of measurement noncontextuality (MNC) and identify contextual scenarios which involve sequential measurements of only a single measurement device. We show that any noncontextual ontological model fails to explain the statistics of outcomes of a single carefully constructed positive-operator-valued measure (POVM) executed sequentially on a quantum system. The context of measurement arises from the different configurations in which the device can be used. We develop an inequality from the noncontextual (NC) ontic model, and construct a quantum situation involving measurements from the Klyachko-Can-Binicio\ifmmode \check{g}\else \v{g}\fi{}lu-Shumovsky (KCBS) inequality. We show that the resultant statistics arising from this device violate our NC inequality. This device can be generalized by incorporating measurements from arbitrary nnn-cycle contextuality inequalities of which n=5n=5n=5 corresponds to the KCBS inequality. We show that the NC and quantum bounds for various scenarios can be derived more easily using only the functional relationships between the outcomes for larger values nnn. This makes it one of the simpler contextual inequalities to analyze.