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Physica Scripta

Sharing nonlocality sequentially with imprecise measurements

Jia Ji, Jinchuan Hou, Shu-Zheng Yang, Kan He

Published Jun 26, 2025• 0 citations
Publisher

Abstract

Abstract Previous studies have shown that quantum nonlocality can theoretically be shared infinitely, but this relies on the precise implementation of measurement schemes. However, in practice, experimenters often struggle to precisely control measurement devices to perfectly align with the target measurements, inevitably introducing measurement error. To address this issue, we introduce an operational notion of inaccuracy that can be directly estimated in the laboratory to formalize the problem. Based on this method, we investigate the impact of imprecise measurements on infinite nonlocality sharing. We first consider the scenario where participants use imprecise measurements to detect nonlocal correlations via the Clauser-Horne-Shimony-Holt (CHSH) inequality and prove the necessary and sufficient conditions for determining the maximum number of shares based on measurement error. Building on this condition, we conduct detailed numerical analyses, the results of which indicate that even minor alignment error can significantly limit the number of nonlocality shares. Finally, we extend our research to the tripartite sequential sharing scenario.

DOI
10.1088/1402-4896/ade8b6

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Abstract Previous studies have shown that quantum nonlocality can theoretically be shared infinitely, but this relies on the precise implementation of measurement schemes. However, in practice, experimenters often struggle to precisely control measurement devices to perfectly align with the target measurements, inevitably introducing measurement error. To address this issue, we introduce an operational notion of inaccuracy that can be directly estimated in the laboratory to formalize the problem. Based on this method, we investigate the impact of imprecise measurements on infinite nonlocality sharing. We first consider the scenario where participants use imprecise measurements to detect nonlocal correlations via the Clauser-Horne-Shimony-Holt (CHSH) inequality and prove the necessary and sufficient conditions for determining the maximum number of shares based on measurement error. Building on this condition, we conduct detailed numerical analyses, the results of which indicate that even minor alignment error can significantly limit the number of nonlocality shares. Finally, we extend our research to the tripartite sequential sharing scenario.
Sequential sharing of quantum nonlocality enables multiparty collaborative information processing, which is typically realized through unsharp measurements in previous studies. By contrast, we experimentally demonstrate that the sequential sharing of quantum nonlocality can be observed using only projective measurements, with the introduction of classical randomness. We achieve sequential violations of the Clauser-Horne-Shimony-Holt inequality in a bipartite quantum system by sharing classical randomness or using a probabilistic projective measurement. Extending the first protocol to a tripartite quantum system, sequential tripartite nonlocality is observed with the Greenberger-Horne-Zeilinger state, where violations of the Mermin inequality are observed in sequential measurements. We experimentally demonstrate these phenomena through the preparation and measurement of a three-photon entangled state. Our work reveals the key role of projective measurements in the sequential sharing of quantum nonlocality, providing a new experimental complement for measuring quantum nonlocality and opening new technological pathways for distributed utilization nonlocality in quantum networks.
There exist bipartite entangled states whose violations of Clauser-Horne-Shimony-Holt (CHSH) Bell inequality can be observed by a single Alice and arbitrarily many sequential Bobs [Phys. Rev. Lett. 125, 090401 (2020)]. Here we consider its analogues for tripartite systems: a tripartite entangled state is shared among Alice, Bob and multiple Charlies. The first Charlie measures his qubit and then passes his qubit to the next Charlie who measures again with other measurements and so on. The goal is to maximize the number of Charlies that can observe some kind of nonlocality with the single Alice and Bob. It has been shown that at most two Charlies could share genuine nonlocality of the Greenberger-Horne-Zeilinger (GHZ) state via the violation of Svetlichny inequality with Alice and Bob [Quantum Inf. Process. 18, 42 (2019) and Phys. Rev. A 103, 032216 (2021)]. In this work, we show that arbitrarily many Charlies can have standard nonlocality (via violations of Mermin inequality) and some other kind of genuine nonlocality (which is known as genuinely nonsignal nonlocality) with the single Alice and single Bob.
Bipartite entangled states whose violations of the Clauser-Horne-Shimony-Holt Bell inequality can be observed by a single Alice and arbitrarily many sequential Bobs exist [Brown and Colbeck, Phys. Rev. Lett. 125, 090401 (2020)]. Here we consider their analogs for tripartite systems: a tripartite entangled state is shared among Alice, Bob, and multiple Charlies. The first Charlie measures his qubit and then passes his qubit to the next Charlie, who measures again with other measurements, and so on. The goal is to maximize the number of Charlies that can observe some kind of nonlocality with the single Alice and Bob. It has been shown that at most two Charlies can share genuine nonlocality of the Greenberger-Horne-Zeilinger state via the violation of the Svetlichny inequality with Alice and Bob [S. Saha et al., Quantum Inf. Process. 18, 42 (2019); Zhang and Fei, Phys. Rev. A 103, 032216 (2021)]. In this work, we show that arbitrarily many Charlies can have standard nonlocality (via violations of the Mermin inequality) and some other kind of genuine nonlocality (which is known as genuinely nonsignal nonlocality) with a single Alice and single Bob.
We address the recently posed question as to whether the nonlocality of a single member of an entangled pair of spin 1/21/21/2 particles can be shared among multiple observers on the other wing who act sequentially and independently of each other [1]. We first show that the optimality condition for the trade-off between information gain and disturbance in the context of weak or non-ideal measurements emerges naturally when one employs a one-parameter class of positive operator valued measures (POVMs). Using this formalism we then prove analytically that it is impossible to obtain violation of the Clauser-Horne-Shimony-Holt (CHSH) inequality by more than two Bobs in one of the two wings using unbiased input settings with an Alice in the other wing.
Unsharp measurements are widely seen as the key resource for recycling the nonlocality of an entangled state shared between several sequential observers. Contrasting this, we here show that nonlocality can be recycled using only standard, projective, qubit measurements. Focusing on the Clauser-Horne-Shimony-Holt inequality and allowing parties to share classical randomness, we determine the optimal trade-off in the magnitude of Bell violations for a maximally entangled state. We then find that nonmaximally entangled states make possible larger sequential violations, which contrasts the standard Clauser-Horne-Shimony-Holt scenario. Furthermore, we show that nonlocality can be recycled using projective qubit measurements even when no shared classical randomness is available. We discuss the implications of our results for experimental implementations of sequential nonlocality.
We address the recently posed question as to whether the nonlocality of a single member of an entangled pair of spin 1 / 2 particles can be shared among multiple observers on the other wing who act sequentially and independently of each other. We first show that the optimality condition for the trade-off between information gain and disturbance in the context of weak or non-ideal measurements emerges naturally when one employs a one-parameter class of positive operator valued measures (POVMs). Using this formalism we then prove analytically that it is impossible to obtain violation of the Clauser-Horne-Shimony-Holt (CHSH) inequality by more than two Bobs in one of the two wings using unbiased input settings with an Alice in the other wing.