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HS n RF 脉冲的实现方程。

Implementation equations for HS n RF pulses.

机构信息

Oklahoma Medical Research Foundation, 825 NE 13th St, OKC, OK 73104, USA.

出版信息

J Magn Reson. 2010 Jun;204(2):333-9. doi: 10.1016/j.jmr.2010.02.022. Epub 2010 Feb 25.

Abstract

Implementation equations for the family of stretched hyperbolic secant (HS(n)) pulses are derived in the linear adiabatic range for inversion of spins. These master equations provide convenience relations for relating the peak amplitude RF(max) of the pulse to the frequency sweep (bwdth) range of the pulse and its duration T(p). The bandwidth of the pulse can also be related to the effective coverage (bw(eff)) of the pulse to a defined or chosen spectral region. The choice of pulse determined by the use of these derived expressions guarantees uniform inversion to a prescribed efficiency across the selected spectral region. The performance of HS(n) pulses in determining the cut-off region between spectral regions was also examined. It is found that beyond a unique T(p)bwdth product no additional gain may be obtained by extending pulse durations for a chosen bwdth of pulse. An example of practical implementation of the inversion pulses is presented for adiabatic decoupling using HS(7) and HS(8) pulses. It is shown that despite added B(1) inhomogeneity in the form of additional amplifier power to 400% from optimal, these pulses can still yield reproducible decoupled spectra.

摘要

在反转自旋的线性绝热范围内,推导出了拉伸双曲正割(HS(n))脉冲族的实现方程。这些主方程提供了方便的关系,将脉冲的峰值幅度 RF(max)与脉冲的频率扫描(带宽)范围及其持续时间 T(p)联系起来。脉冲的带宽也可以与脉冲的有效覆盖范围(bw(eff))与定义或选择的光谱区域相关联。通过使用这些导出的表达式来选择脉冲,可以保证在选定的光谱区域内以规定的效率实现均匀反转。还检查了 HS(n)脉冲在确定光谱区域之间的截止区域方面的性能。结果发现,在独特的 T(p)带宽产物之外,通过延长脉冲持续时间来获得所选带宽的脉冲,不会获得额外的增益。给出了使用 HS(7)和 HS(8)脉冲进行绝热去耦的实际实现示例。结果表明,尽管由于额外的放大器功率导致 B(1)非均匀性增加了 400%,但这些脉冲仍可产生可重复的去耦光谱。

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Implementation equations for HS n RF pulses.HS n RF 脉冲的实现方程。
J Magn Reson. 2010 Jun;204(2):333-9. doi: 10.1016/j.jmr.2010.02.022. Epub 2010 Feb 25.

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