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Liquid-State Nuclear Magnetic Resonance Measurements for Imaging Using HTS-rf-SQUID in Ultra-Low Field

机译:在超低场中使用HTS-rf-SQUID进行成像的液态核磁共振测量

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In our study, we constructed a ultra-low field (ULF) nuclear magnetic resonance (NMR)/magnetic resonance imaging (MRI) system employing a high-temperature superconductor (HTS)-rf-SQUID and room-temperature coils. In the system, we employed a pulsed polarizing field $B_{rm p}$ perpendicular to a measurement field $B_{rm m}$; a high-speed switching circuit with an optical FET was used to switch off $B_{rm p}$ of approximately 30 mT. When a field gradient ${rm d}B_{z}/{rm d}z$ of approximately 10 nT/cm was applied to a sample, which was designed to contain water in two compartments, a $^{1}{rm H}$-NMR spectrum with two peaks was observed. The frequency difference between the two peaks roughly corresponded to the distance between each center of the water in the two parts. We measured the $^{1}{rm H}$ -NMR signals for water and mineral oil and found a clear difference in their signal amplitudes owing to their different molecular compositions. The longitudinal relaxation times ${rm T}_{1}$ of water and the oil were also estimated by changing the polarizing time of $B_{rm p}$. From these results, it was confirmed that $^{1}{rm H}$- and ${rm T}_{1}$-weighted contrast imaging could be realized by using this system.
机译:在我们的研究中,我们构建了一个采用高温超导体(HTS)-rf-SQUID和室温线圈的超低场(ULF)核磁共振(NMR)/磁共振成像(MRI)系统。在该系统中,我们采用垂直于测量场$ B_ {rm m} $的脉冲偏振场$ B_ {rm p} $;使用带有光学FET的高速开关电路来关断大约30 mT的$ B_ {rm p} $。当将大约10 nT / cm的场梯度$ {rm d} B_ {z} / {rm d} z $应用于设计为在两个隔室中容纳水的样品时,则$ ^ {1} {rm观察到具有两个峰的1 H-NMR谱。两个峰值之间的频率差大致对应于两个部分中水的每个中心之间的距离。我们测量了水和矿物油的$ ^ {1} {rm H} $ -NMR信号,发现由于分子组成的不同,其信号幅度也存在明显差异。还通过改变极化时间$ B_ {rm p} $来估算水和油的纵向弛豫时间$ {rm T} _ {1} $。从这些结果证实,通过使用该系统可以实现$ ^ {1} {rm H} $-和$ {rm T} _ {1} $加权的对比度成像。

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