1. 中国电力科学研究院有限公司,北京,100192
2. 国家高电压计量站,武汉,430074
收稿:2025-08-31,
纸质出版:2025
移动端阅览
周峰, 肖铮, 胡浩亮, 等. 量子电流测量技术研究进展与应用综述[J]. 高电压技术, 2025,51(8):4368-4380.
ZHOU Feng, XIAO Zheng, HU Haoliang, et al. 量子电流测量技术研究进展与应用综述[J]. 2025, 51(8): 4368-4380.
周峰, 肖铮, 胡浩亮, 等. 量子电流测量技术研究进展与应用综述[J]. 高电压技术, 2025,51(8):4368-4380. DOI: 10.13336/j.1003-6520.hve.20250729.
ZHOU Feng, XIAO Zheng, HU Haoliang, et al. 量子电流测量技术研究进展与应用综述[J]. 2025, 51(8): 4368-4380. DOI: 10.13336/j.1003-6520.hve.20250729.
近年来,随着新型电力系统及量子测量技术的快速发展,工程现场对宽频宽量程电流测量的灵敏度和准确度提出了更高要求。该文调研了3种基于磁测量原理与量子效应的电流测量路线:气态碱金属光泵磁力计、超导量子干涉低温电流比较器与金刚石氮-空位色心测量装置。气态碱金属光泵磁力计在室温(原子气室加热至50~150 ℃)下,基于气态原子自旋进动原理,磁测量灵敏度可达fT·Hz−1/2量级,在直流至数千赫兹范围内可实现毫安级至安级电流的测量。超导量子干涉仪体系基于磁通量子化与约瑟夫森效应,在良好屏蔽与优化拾取线圈条件下,磁测量灵敏度可提升至aT·Hz−1/2量级,通过匝数比与反馈设计,其可测电流量程覆盖皮安级至安级,并在直流至兆赫兹带宽内提供计量级准确度。金刚石氮-空位色心方案基于光学检测磁共振原理,通过微波操控与光学读出实现磁场测量,磁测量灵敏度可达pT·Hz−1/2量级,可测电流上限为千安级,常规连续带宽覆盖直流至千赫兹,针对某一固定频率的窄带交流信号,中心工作频率可扩展至兆赫兹。通过对比3种技术的底层机理、关键性能和工程化难点,得出以下结论:光泵磁力计需要提升现场抗噪能力和系统集成度,以适应复杂环境的需求;超导量子干涉仪低温电流比较器受限于低温制冷和高成本,亟需实现小型化和简化维护;金刚石氮-空位色心测量装置虽然灵敏度稍低,但凭借绝缘与小型化特性已在高压、大电流的非接触测量中展现出更大的潜力。
In recent years
the rapid development of new-type power system and quantum measurement technologies has imposed more stringent requirements on the sensitivity and accuracy of wide-bandwidth
wide-dynamic-range current metrology in field environments. This paper surveys three current-measurement approaches based on magnetic sensing principles and quantum effects: alkali-vapor optically pumped magnetometers(OPMs)
superconducting quantum interference device(SQUID)-based cryogenic current comparators(CCCs)
and diamond nitrogen-vacancy(NV)-center sensors. OPMs
operating at room temperature with vapor cells typically heated to 50~150 ℃
exploit atomic spin precession and can achieve fT·Hz−1/2 magnetic-field sensitivity; in practice they enable current measurements from the milliampere to ampere scale over DC to several kilohertz. SQUID-based systems
leveraging flux quantization and the Josephson effect
can reach aT·Hz−1/2 magnetic sensitivity under adequate magnetic shielding and optimized pickup-coil design. With suitable turns ratios and flux-locked-loop feedback
their measurable current range spans picoamperes to amperes
and they can deliver metrological accuracy from DC up to the megahertz band. NV-center sensors
based on optically detected magnetic resonance(ODMR) with microwave control and optical readout
routinely achieve pT·Hz−1/2 sensitivity. In non-contact current sensing configurations
the upper measurable current reaches the kiloampere range. Continuous-mode bandwidth typically covers DC to the kilohertz range
while narrowband AC readout at a fixed carrier frequency can extend the center frequency into the megahertz regime. By comparing the underlying mechanisms
key performance metrics
and engineering challenges
we conclude: OPMs must improve noise immunity and system integration to better withstand complex field environments; SQUID/CCC systems are constrained by cryogenic cooling and cost
motivating miniaturization and simplified maintenance; and although NV sensors are somewhat less sensitive
their electrical insulation and compact form factor offer clear advantages for non-contact measurements in high-voltage
high-current settings.
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