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arXiv 2104.02898quant-ph
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基于量子保护绝热变换的量子精密测量:不完全性、有限持续时间和退相

Quantum metrology based on symmetry-protected adiabatic transformation: Imperfection, finite time duration, and dephasing

Takuya Hatomura, Atsuki Yoshinaga, Yuichiro Matsuzaki, Mamiko Tatsuta

摘要:

量子精密测量的目的是尽可能精确地估计目标参数。本文研究了基于量子保护绝热变换的量子精密测量。我们引入了一个以横场为探针的铁磁伊辛模型,并考虑了纵向场的估计。在没有横场的情况下,探针的基态由Greenberger-Horne-Zeilinger态给出,从而通过宇称测量实现了纵场的海森堡极限估计.在我们的方案中,通过保序绝热变换,将编码在宇称上的纵向场的全部信息精确地映射到全局磁化强度上,从而可以用全局磁化强度测量代替宇称测量.此外,该方案既不需要精确控制单个量子位,也不需要精确控制相互作用强度。我们讨论了有限横场和非绝热跃迁作为绝热变换的不完全性的影响。通过考虑到有限的持续时间的状态准备,传感和读出,我们还比较了本方案的性能与经典的计划在存在和不存在的失相。

英文摘要:

The aim of quantum metrology is to estimate target parameters as precisely as possible. In this paper, we consider quantum metrology based on symmetry-protected adiabatic transformation. We introduce a ferromagnetic Ising model with a transverse field as a probe and consider the estimation of a longitudinal field. Without the transverse field, the ground state of the probe is given by the Greenberger-Horne-Zeilinger state, and thus the Heisenberg limit estimation of the longitudinal field can be achieved through parity measurement. In our scheme, full information of the longitudinal field encoded on parity is exactly mapped to global magnetization by symmetry-protected adiabatic transformation, and thus the parity measurement can be replaced with global magnetization measurement. Moreover, this scheme requires neither accurate control of individual qubits nor that of interaction strength. We discuss the effects of the finite transverse field and nonadiabatic transitions as imperfection of adiabatic transformation. By taking into account finite time duration for state preparation, sensing, and readout, we also compare performance of the present scheme with a classical scheme in the absence and presence of dephasing.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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