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J Neurosci Methods. 2009 Feb 15;177(1):160-7. doi: 10.1016/j.jneumeth.2008.10.025. Epub 2008 Nov 5.
3
Quantitative assessment of water pools by T 1 rho and T 2 rho MRI in acute cerebral ischemia of the rat.通过T1ρ和T2ρ磁共振成像对大鼠急性脑缺血中水池进行定量评估。
J Cereb Blood Flow Metab. 2009 Jan;29(1):206-16. doi: 10.1038/jcbfm.2008.113. Epub 2008 Oct 1.
4
Gapped pulses for frequency-swept MRI.用于频率扫描磁共振成像的间隙脉冲。
J Magn Reson. 2008 Aug;193(2):267-73. doi: 10.1016/j.jmr.2008.05.009. Epub 2008 May 20.
5
Water spin dynamics during apoptotic cell death in glioma gene therapy probed by T1rho and T2rho.通过T1rho和T2rho检测胶质瘤基因治疗中凋亡细胞死亡期间的水自旋动力学。
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6
Fast and quiet MRI using a swept radiofrequency.使用扫频射频的快速静音磁共振成像
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7
T1rho MRI contrast in the human brain: modulation of the longitudinal rotating frame relaxation shutter-speed during an adiabatic RF pulse.人脑的T1rho磁共振成像对比:绝热射频脉冲期间纵向旋转框架弛豫快门速度的调制。
J Magn Reson. 2006 Jul;181(1):135-47. doi: 10.1016/j.jmr.2006.04.002. Epub 2006 May 3.
8
Exchange-influenced T2rho contrast in human brain images measured with adiabatic radio frequency pulses.用绝热射频脉冲测量的人脑图像中交换影响的T2rho对比度。
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9
Exploring the limits of broadband excitation and inversion pulses.探索宽带激发和反转脉冲的极限。
J Magn Reson. 2004 Oct;170(2):236-43. doi: 10.1016/j.jmr.2004.06.017.
10
Universal equations for linear adiabatic pulses and characterization of partial adiabaticity.线性绝热脉冲的通用方程及部分绝热性的表征
J Magn Reson. 2002 May;156(1):26-40. doi: 10.1006/jmre.2002.2531.

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.

DOI:10.1016/j.jmr.2010.02.022
PMID:20227899
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC2929662/
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。