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27.4 A sub-1dB NF dual-channel on-coil CMOS receiver for Magnetic Resonance Imaging

机译:27.4低于1dB的NF双通道线圈上CMOS接收器,用于磁共振成像

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Magnetic Resonance Imaging (MRI) is a widely used medical imaging technique. It employs a strong static magnetic field (1.5 to 10.5T for human imaging) to split the spin states of the 1H nuclei in the body, and RF excitation to induce transitions and coherence among them. Gradient fields are superimposed to modulate the 1H resonance frequency, which enables spatially distinguishable signals to be picked up by RF receive coils. A high-field MRI provides better sensitivity and resolution but requires better receivers (RX), as signal DR and 1H resonance increase (128MHz for 3T, 300MHz for 7T). Overall sensitivity and imaging speed can be enhanced by closely surrounding the target anatomy with tens of RX coils (as in MIMO) [1], at the expense of as many shielded RF cables to carry the information out of the field. Progress in PCB size has allowed multi-channel RX to be placed inside the magnetic field (in-bore), reducing the RF cable length to less than 1m [2,3]. Ultimately, the RX should be placed directly on-coil to avoid bulky coaxial cables and improve patient comfort and safety by acquiring data in-bore and sending them digitally to the MRI scanner via an optical fiber link. The latter is cheap, flexible and insensitive to magnetic fields. The immediate vicinity of the coils and the patient is, however, a hostile as well as sensitive electromagnetic environment, which tolerates only the smallest of PCBs and virtually no magnetic material in its components. Integration of the full RX chain in a CMOS chip, which is small, non-magnetic and low power, holds the key to the next wave of compact MRI coil arrays for advanced medical imaging. This paper presents a fully integrated dual-receiver RFIC for coil arrays intended for (ultra-) high field (1.5 to 10.5T and 64 to 450MHz) scanners for clinical MRI, where requirements are considerably stricter than previously reported transceiver ICs [4,5] on palm-held NMR devices for spectroscopy or lab-on-chip applications.
机译:磁共振成像(MRI)是一种广泛使用的医学成像技术。它使用强静态磁场(用于人体成像时为1.5到10.5T)来分裂人体中1H核的自旋状态,并利用RF激发在它们之间引起跃迁和相干。叠加梯度场以调制1H谐振频率,从而使RF接收线圈能够拾取空间上可区分的信号。高场MRI可提供更好的灵敏度和分辨率,但由于信号DR和1H共振增加(3T为128MHz,7T为300MHz),因此需要更好的接收器(RX)。通过用数十个RX线圈紧紧围绕目标解剖结构(如MIMO),可以提高整体灵敏度和成像速度[1],但要牺牲许多屏蔽的RF电缆来将信息带出现场。 PCB尺寸的进步允许将多通道RX放置在磁场(孔内)内部,从而将RF电缆长度减小到小于1m [2,3]。最终,RX应该直接放在线圈上,以避免笨重的同轴电缆,并通过获取孔内数据并将其以数字方式通过光纤链路发送给MRI扫描仪,从而提高患者的舒适度和安全性。后者便宜,灵活且对磁场不敏感。但是,线圈和患者的直接邻近区域是充满敌意和敏感的电磁环境,该环境只能容忍最小的PCB,并且其组件中几乎没有磁性材料。小型,无磁性,低功耗的CMOS芯片中的完整RX链集成是下一波用于高级医学成像的紧凑型MRI线圈阵列的关键。本文提出了一种用于线圈阵列的完全集成的双接收器RFIC,用于用于临床MRI的(超)高场(1.5至10.5T和64至450MHz)扫描仪,其要求比以前报道的收发器IC严格得多[4,5用于光谱学或芯片实验室应用的手持式NMR设备上。

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