R. Körber, O. Kieler, P. Hömmen, N. Höfner, J. Storm
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引用次数: 3
摘要
我们介绍了我们的超灵敏SQUID系统在生物磁性和超低场(ULF) MRI领域的应用。电流传感器配置中,拾取线圈电感耦合到SQUID。一阶轴向梯度仪系统在噪声可忽略的液体He杜瓦瓶中工作,测量到的耦合能量灵敏度$\epsilon_{c}$为40 $h$,白噪声低于200 aT $\mathrm{Hz}^{-1/2}$。作为其在生物磁学中使用的一个例子,我们讨论了来自体感觉皮层的600 Hz高频脉冲的单次试验脑磁图测量,这与单个神经元的同步峰活动有关。我们还将该系统应用于超低场MRI,该系统在MRI线圈系统中运行,该系统具有几个快速切换的场和梯度线圈。这需要在输入电路中使用限流器和二阶轴向梯度仪,导致噪声增加380 aT $\mathrm{Hz}^{-1/2}$。在这里,我们展示了在幻影中外加电流的全张量电流密度成像。为了进一步改善噪声,基于HfTi自分流结技术的纳米Josephson结的制造工艺已扩展到以AlOx为绝缘层的SIS工艺。我们获得了330 $\mathrm{n}\Phi_{0}\mathrm{Hz}^{-1/2}$和550 $\mathrm{n}\Phi_{0}\mathrm{Hz}^{-1/2}$的噪声水平,对应于未耦合和耦合squid的能量灵敏度分别为5 $h$和20 $h$。
Ultra-sensitive SQUID systems for applications in biomagnetism and ultra-low field MRI
We present the use of our ultra-sensitive SQUID system in the field of biomagnetism and ultra-low field (ULF) MRI. A current sensor configuration is used where a pickup coil is inductively coupled to the SQUID. A 1st-order axial gradiometer system, operated in a liquid He dewar with negligible noise, achieves a measured coupled energy sensitivity $\epsilon_{c}$ of 40 $h$ and a white noise below 200 aT $\mathrm{Hz}^{-1/2}$. As an example of its use in biomagnetism, we discuss single trial magnetoencephalography measurements of high frequency bursts at 600 Hz from the somatosensory cortex which are related to synchronized spiking activity of individual neurons. We also deploy this system for ultra-low field MRI where it is operated inside an MRI coil system with several fast-switchable field and gradient coils. This necessitates the use of a current limiter in the input circuit and a 2nd-order axial gradiometer leading to an increased noise of 380 aT $\mathrm{Hz}^{-1/2}$. Here, we demonstrated full tensor current density imaging of impressed currents in phantoms. For further improvement of the noise, the fabrication process for the nanometer-sized Josephson junctions based on the HfTi self-shunted junction technology has been extended to a SIS process with AlOx as the insulating layer. We achieved noise levels of 330 $\mathrm{n}\Phi_{0}\mathrm{Hz}^{-1/2}$ and 550 $\mathrm{n}\Phi_{0}\mathrm{Hz}^{-1/2}$, corresponding to energy sensitivities of 5 $h$ and 20 $h$ for uncoupled and coupled SQUIDs, respectively.