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中国物理学会期刊

应用于超导脑磁系统的集成超导量子干涉器件芯片的设计与性能评估

CSTR: 32037.14.aps.74.20250426

Design and performance evaluation of integrated superconducting quantum interference device chips for superconducting brain magnetometer systems

CSTR: 32037.14.aps.74.20250426
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  • 超导量子干涉器件(SQUID)作为一种超灵敏的磁通传感器, 在生物磁探测、低场核磁共振、地球物理探矿等领域得到广泛应用. 本文设计开发了一种用于脑磁(MEG)系统的集成SQUID芯片, 并进行了批量封装测试. 其中, 每个芯片上集成了两个一阶平面梯度计和一个磁强计, 采用亚微米约瑟夫森结制备技术, 实现0.7 μm×0.7 μm的亚微米结尺寸. SQUID与探测线圈采用Nb超导引线连接, 集成到同一芯片上. 对171个SQUID器件的测试结果显示, 这些器件在磁场白噪声、I-V特性、V-Φ特性等方面表现优异. 本文制备的SQUID器件工作电流集中在15—20 μA, 电压摆幅集中在80—120 μV. 此外, 超过80%的SQUID器件的磁场白噪声低于 5\text fT/\sqrt \textHz , 能够满足多通道SQUID脑磁系统的要求.

     

    Superconducting quantum interference device (SQUID) is one of the most sensitive flux sensors and is critical in fields such as biomagnetism, low-field nuclear magnetic resonance (NMR), and geophysics. In this paper, an integrated magnetoencephalography (MEG) SQUID chip is investigated in detail, which consists of a magnetometer and two gradiometers. The SQUID and pick-up coils are fabricated on different-sized wafers. The SQUID is fabricated on a commercial silicon substrate using micro- and nano-fabrication processes, including thin-film growth, i-line stepper photolithography, and reactive ion etching (RIE). The sub-micron Josephson junction technology is employed to achieve a junction size of 0.7 μm×0.7 μm with a junction capacitance of only 0.05 pF. The pick-up coil is designed as a single-turn coil for a magnetometer and a planar first-order gradient coil for a gradient sensor. The MEG SQUID chips are tested in a well-shielded chamber with the helium-liquid temperature (4.2 K). Customized low-voltage noise readout circuit and source measure units are used to characterize the magnetic field white noise, current-voltage (I-V) characteristics, and voltage modulation amplitude of 171 SQUID channels. The results show that 81% of the SQUID chips exhibit the lower magnetic field noise (< 5 \textfT/\sqrt \textHZ ), and the high modulation amplitudes (in a range of 80–120 μV) with the low working currents of 15–20 μA, yielding a wafer yield rate of 78%. In summary, the SQUIDs show excellent performance in terms of magnetic field white noises, modulation amplitudes, and working currents, which are suitable for the very weak magnetic signal detection. One of future studies will focus on optimizing the SQUID chip fabrication process to minimize performance variations between chips on the same wafer.

     

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