使用直流SQUID放大器的宽带核磁共振

C.P. Lusher , Junyun Li , M.E. Digby , R.P. Reed , B. Cowan , J. Saunders , D. Drung , T. Schurig
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引用次数: 13

摘要

我们构建了两个脉冲核磁共振光谱仪,其中信号使用超导磁通变压器耦合到低Tc直流SQUID的输入线圈,产生宽带响应,其带宽由SQUID电子元件决定。利用50 kHz带宽商用系统,在温度1.4 ~ 4.2 K、频率5 ~ 40 kHz范围内,对铂粉、体铂、3He气体和3He表面单分子层的自由感应衰减信号进行了观测。观察到的信噪比与除大块金属外所有样品中SQUID中以通量噪声为主的噪声计算一致。另一个系统工作在带宽为3.4 MHz的磁锁环模式下,使用带有附加正反馈的SQUID,用于观察铂粉在38至513 kHz频率和4.2 K温度下的核磁共振信号。讨论了该技术在研究频率低于1mhz的短T2系统中的优势。此外,我们讨论了宽带和调谐输入电路对核磁共振检测的好处,并描述了具有调谐输入电路的光谱仪的性能,该电路已用于从4.2 K的铂粉和1.7 K时吸收在0.11 m2表面积上的~ 2层3He中获得1 MHz的信号。在3He实验中,预测放大器噪声温度为60 mK。这证明了在低毫开尔文温度下对低自旋密度和T2大于几百微秒的系统进行测量的调谐装置的潜力。
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Broadband nuclear magnetic resonance using DC SQUID amplifiers

We have constructed two pulsed NMR spectrometers in which the signal is coupled to the input coil of a low Tc DC SQUID using a superconducting flux transformer, yielding broadband response, with bandwidth determined by the SQUID electronics. A 50 kHz bandwidth commercial system has been used to observe free induction decay signals from platinum powder, bulk platinum, 3He gas and surface monolayers of 3He in the temperature range from 1.4 to 4.2 K and at frequencies from 5 to 40 kHz. The observed signal-to-noise ratio is as calculated with the noise dominated by flux noise in the SQUID in all samples but the bulk metal. A second system, which operates in flux-locked loop mode with bandwidth of 3.4 MHz using a SQUID with additional positive feedback, has been used to observe NMR signals from platinum powder at frequencies from 38 to 513 kHz and at a temperature of 4.2 K. The advantage of this technique in the study of systems with short T2 at frequencies below 1 MHz is discussed. In addition we discuss the benefits of both broadband and tuned input circuits for NMR detection and we describe the performance of a spectrometer with a tuned input circuit which has been used to obtain signals at 1 MHz from platinum powder at 4.2 K and from ∼2 layers of 3He absorbed on a surface area of 0.11 m2 at 1.7 K. The amplifier noise temperature is predicted to be 60 mK in the 3He experiment. This demonstrates the potential of the tuned set-up for measurements at low millikelvin temperatures on systems with low spin density and with T2 greater than several hundred microseconds.

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