aiqbench analysis
This research presents a novel method for extracting rotation angles using pairwise Bell state analysis, effectively overcoming the inefficiencies of traditional state tomography in quantum sensing protocols. By leveraging the specific transformation properties of symmetric Bell states, the study achieves optimal precision that saturates the Quantum Cramer-Rao Bound for second-order anti-coherent states. This advancement is significant for enhancing the sensitivity and practicality of quantum metrology devices without requiring complex full-state reconstruction.
Bell State Analysis Provides an Optimal Basis Saturating the Quantum Cramer-Rao in Rotation Sensing
arXiv:2605.24108v2 Announce Type: replace Abstract: The second-order anti-coherent state of light is known to saturate the Cramer-Rao Bound (QCRB) for rotation sensing around an arbitrary axis. However, due to the complexity of the state and the inefficiency of state tomography, parameter extraction remains an open problem. In this manuscript, we approach the problem of parameter extraction using pairwise Bell state analysis with an additional path degree of freedom. Due to the transformation property of rotation, only the symmetric Bell states will show up in projection in the final state. We exploit this advantage to develop a scheme for extracting the rotation angle for N=4 and N=6 second-order anti-coherent states.
Abstract:The second-order anti-coherent state of light is known to saturate the Cramer-Rao Bound (QCRB) for rotation sensing around an arbitrary axis. However, due to the complexity of the state and the inefficiency of state tomography, parameter extraction remains an open problem. In this manuscript, we approach the problem of parameter extraction using pairwise Bell state analysis with an additional path degree of freedom. Due to the transformation property of rotation, only the symmetric Bell states will show up in projection in the final state. We exploit this advantage to develop a scheme for extracting the rotation angle for N=4 and N=6 second-order anti-coherent states.
arXiv:2605.24108 [quant-ph]
(or arXiv:2605.24108v2 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2605.24108 Focus to learn more arXiv-issued DOI via DataCite
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