量子计量学与局部哈密尔顿人的通用射击噪声极限
Hai-Long Shi1,2,3, Xi-Wen Guan1,3,4, Jing Yang5
1Innovation Academy for Precision Measurement Science and Technology, Chinese Academy of Sciences, Wuhan 430071, China.
Physical review letters
|March 22, 2024
概括
局部量子相互作用无法提高超出可分离状态的射击噪声极限的传感精度. 超越这个极限需要非局部相互作用,这对于量子增强传感应用至关重要.
科学领域:
- 量子物理学的量子物理学
- 凝聚物质理论 凝聚物质理论
- 量子信息科学是一种量子信息科学.
背景情况:
- 由多体相互作用产生的量子纠是量子增强感知的关键.
- 量子系统中的操作员增长受到局部相互作用的利布-罗宾逊边界的限制.
研究的目的:
- 将量子费舍尔信息增长的边界与利布-罗宾逊边界联系起来.
- 调查量子传感与局部相互作用和可分离的初始状态的精度极限.
主要方法:
- 连接量子费舍尔信息增长和利布-罗宾逊边界的理论分析.
- 在远程Ising模型上进行数值模拟.
主要成果:
- 具有可分离的初始状态的局部多体相互作用不能超过射击噪声限制.
- 这一精度限制也适用于局部的非退化的基态,隙的哈密尔顿人.
- 非局部和远程相互作用是超越射击噪声限制所必需的.
结论:
- 当局相互作用本身不足以超出射击噪声极限的量子传感,当从可分离状态开始时.
- 这些发现凸显了非局部相互作用在先进量子传感中的关键作用.
- 开辟了探索量子传感,控制,多体物理学和信息编码的途径.
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