Shared randomness allows violation of macroscopic realism using a single measurement

Macro-realistic description of systems is based majorly on two basic intuitions about the classical world, namely, macrorealism per se, that is, the system is always in a distinct state, and non-invasive measurements, that is, measurements do not disturb the system. Given the assumption of no-signaling in time, one utilizes Leggett–Garg inequalities to observe a violation of macroscopic realism, which requires at least three measurements. In this work, we show that if one has access to shared randomness, then one can observe a violation of macroscopic realism using a single measurement even if no signaling in time is satisfied. Interestingly, using the proposed scheme one can also rule out a larger class of models, which we term macroscopic no-signaling theories that cannot violate the no-signaling in time conditions. We further construct a witness to observe the violation of macroscopic no-signaling.

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Publication Details

Journal
APL Quantum
Published
2025-05-27
DOI
https://doi.org/10.1063/5.0252123
Primary Topic
Quantum Mechanics and Applications
Type
article
Field-Weighted Citation Impact
0.00

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article

Shared randomness allows violation of macroscopic realism using a single measurement

Shubhayan Sarkar
APL Quantum
Quantum Mechanics and Applications
article

Shared randomness allows violation of macroscopic realism using a single measurement

Shubhayan Sarkar
article en

Abstract

Macro-realistic description of systems is based majorly on two basic intuitions about the classical world, namely, macrorealism per se, that is, the system is always in a distinct state, and non-invasive measurements, that is, measurements do not disturb the system. Given the assumption of no-signaling in time, one utilizes Leggett–Garg inequalities to observe a violation of macroscopic realism, which requires at least three measurements. In this work, we show that if one has access to shared randomness, then one can observe a violation of macroscopic realism using a single measurement even if no signaling in time is satisfied. Interestingly, using the proposed scheme one can also rule out a larger class of models, which we term macroscopic no-signaling theories that cannot violate the no-signaling in time conditions. We further construct a witness to observe the violation of macroscopic no-signaling.

APL QuantumVol. 2(2)
Université Libre de Bruxelles (BE)
QuantERA
Openalex Percentile: Top 91%
Quantum Mechanics and Applications
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