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NMR imaging of solids with multiple-pulse line narrowing and radiofrequency gradients

机译:具有多脉冲线变窄和射频梯度的固体核磁共振成像

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摘要

The usual methods of magnetic resonance imaging fail in rigid solids due to the line shape contributions of dipolar coupling, chemical shift dispersion and anisotropy, and bulk magnetic susceptibility. This dissertation presents a new method of solid-state imaging by nuclear magnetic resonance which averages away these contributions with multiple-pulse line-narrowing and encodes spatial information with pulsed radiofrequency field gradients. This method is closely related to simultaneously developed methods utilizing pulsed DC gradients, and offers similar improvements in sensitivity and resolution. The advantage of rf gradients is that they can be rapidly switched without inducing eddy currents in the probe or the magnet. In addition, the phases and amplitudes of the rf gradients can be switched by equipment which is already part of an NMR spectrometer capable of solid-state spectroscopy. The line-narrowing and gradient pulses originate in separate rf circuits tuned to the same frequency. Interactions between the circuits have been minimized by a method of active Q-switching which employs PIN diodes in the matching networks of these circuits.Both one- and two-dimensional images are presented. The latter are obtained by a novel method in which the two dimensions of imaging transverse to the static magnetic field are encoded by two orthogonal components of a single rf gradient. A [pi]/2 phase shift of the rf phase relative to that of the line-narrowing pulses selects one component or the other. This arrangement allows the solid-state analogs of versatile imaging sequences based on Fourier imaging and eliminates the need for sample rotation and back-projection methods.Coherent averaging theory is used to analyze this imaging technique and exact numerical simulations on several coupled spins are discussed. These lend insight to the residual linewidth and its dependence on pixel position as well as to the range of applicability of this technique.
机译:由于偶极耦合的线形贡献,化学位移分散和各向异性以及体磁化率,通常的磁共振成像方法在刚性固体中失败。本文提出了一种通过核磁共振进行固态成像的新方法,该方法通过多脉冲变窄来平均这些贡献,并利用脉冲射频场梯度对空间信息进行编码。此方法与同时开发的利用脉冲直流梯度的方法密切相关,并且在灵敏度和分辨率方面提供了类似的改进。射频梯度的优势在于,它们可以快速切换而不会在探头或磁体中产生涡流。此外,rf梯度的相位和幅度可以通过设备进行切换,该设备已经是能够进行固态光谱分析的NMR光谱仪的一部分。变窄脉冲和梯度脉冲起源于单独的射频电路,调谐到相同的频率。通过在这些电路的匹配网络中使用PIN二极管的有源Q开关方法,可以最大程度地减少电路之间的相互作用,并提供一维和二维图像。后者是通过一种新颖的方法获得的,其中横向于静态磁场的二维成像是由单个rf梯度的两个正交分量编码的。 rf相相对于细线脉冲的π/ 2相移选择一个分量或另一分量。这种安排允许基于傅立叶成像的通用成像序列的固态类似物,并且不需要样品旋转和反投影方法。相干平均理论用于分析这种成像技术,并讨论了几个耦合自旋的精确数值模拟。这些使人们对残余线宽及其对像素位置的依赖性以及该技术的适用范围有了更深入的了解。

著录项

  • 作者

    Werner Margat Hoppe;

  • 作者单位
  • 年度 1993
  • 总页数
  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
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