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首页> 外文期刊>Journal of magnetic resonance >Microwave field distribution in a magic angle spinning dynamic nuclear polarization NMR probe
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Microwave field distribution in a magic angle spinning dynamic nuclear polarization NMR probe

机译:魔角旋转动态核极化NMR探针中的微波场分布

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We present a calculation of the microwave field distribution in a magic angle spinning (MAS) probe utilized in dynamic nuclear polarization (DNP) experiments. The microwave magnetic field (B_(1S)) profile was obtained from simulations performed with the High Frequency Structure Simulator (HFSS) software suite, using a model that includes the launching antenna, the outer Kel-F stator housing coated with Ag, the RF coil, and the 4 mm diameter sapphire rotor containing the sample. The predicted average B_(1S) field is 13 μT/W~(1/2), where S denotes the electron spin. For a routinely achievable input power of 5 W the corresponding value is γ _SB_(1S) = 0.84 MHz. The calculations provide insights into the coupling of the microwave power to the sample, including reflections from the RF coil and diffraction of the power transmitted through the coil. The variation of enhancement with rotor wall thickness was also successfully simulated. A second, simplified calculation was performed using a single pass model based on Gaussian beam propagation and Fresnel diffraction. This model provided additional physical insight and was in good agreement with the full HFSS simulation. These calculations indicate approaches to increasing the coupling of the microwave power to the sample, including the use of a converging lens and fine adjustment of the spacing of the windings of the RF coil. The present results should prove useful in optimizing the coupling of microwave power to the sample in future DNP experiments. Finally, the results of the simulation were used to predict the cross effect DNP enhancement vs. ω_(1S)/(2π) for a sample of ~(13)C-urea dissolved in a 60:40 glycerol/water mixture containing the polarizing agent TOTAPOL; very good agreement was obtained between theory and experiment.
机译:我们介绍了在动态核极化(DNP)实验中使用的魔角旋转(MAS)探针中微波场分布的计算。微波磁场(B_(1S))曲线是通过使用高频结构模拟器(HFSS)软件套件进行的仿真获得的,使用的模型包括发射天线,涂有Ag的外部Kel-F定子壳体,RF线圈,以及包含样品的直径4毫米的蓝宝石转子。预测的平均B_(1S)场为13μT/ W〜(1/2),其中S表示电子自旋。对于常规可达到的5 W输入功率,相应值为γ_SB_(1S)= 0.84 MHz。这些计算提供了对微波功率与样品耦合的洞察力,包括来自RF线圈的反射和通过线圈传输的功率的衍射。还成功地模拟了转子壁厚度的增强变化。使用基于高斯光束传播和菲涅耳衍射的单程模型执行第二次简化计算。该模型提供了更多的物理见解,并且与完整的HFSS仿真完全吻合。这些计算表明增加微波功率与样品耦合的方法,包括使用会聚透镜和微调RF线圈绕组的间距。在未来的DNP实验中,目前的结果应被证明有助于优化微波功率与样品的耦合。最后,模拟结果用于预测溶解在含有极化剂的60:40甘油/水混合物中的〜(13)C-尿素样品的DNP增强对ω_(1S)/(2π)的交叉效应。代理商TOTAPOL;理论与实验之间取得了很好的一致性。

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