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Irreversible change in the T1 temperature dependence with thermal dose using the proton resonance frequency-T1 technique.采用质子共振频率 T1 技术,热剂量下 T1 温度依赖性发生不可逆变化。
Magn Reson Med. 2013 Apr;69(4):1122-30. doi: 10.1002/mrm.24322. Epub 2012 May 10.
2
Hybrid proton resonance frequency/T1 technique for simultaneous temperature monitoring in adipose and aqueous tissues.用于脂肪和水组织中同时温度监测的质子磁共振频率/T1 混合技术。
Magn Reson Med. 2013 Jan;69(1):62-70. doi: 10.1002/mrm.24228. Epub 2012 Mar 5.
3
An analysis of the accuracy of magnetic resonance flip angle measurement methods.磁共振翻转角测量方法准确性分析。
Phys Med Biol. 2010 Oct 21;55(20):6157-74. doi: 10.1088/0031-9155/55/20/008. Epub 2010 Sep 29.
4
On the steady-state properties of actual flip angle imaging (AFI).关于实际翻转角成像(AFI)的稳态特性。
Magn Reson Med. 2009 Jan;61(1):84-92. doi: 10.1002/mrm.21592.
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Uncertainty in T(1) mapping using the variable flip angle method with two flip angles.使用具有两个翻转角的可变翻转角方法进行T(1)映射时的不确定性。
Phys Med Biol. 2009 Jan 7;54(1):N1-8. doi: 10.1088/0031-9155/54/1/N01. Epub 2008 Dec 5.
6
Uncertainty and bias in contrast concentration measurements using spoiled gradient echo pulse sequences.使用扰相梯度回波脉冲序列进行对比剂浓度测量时的不确定性和偏差。
Phys Med Biol. 2008 May 7;53(9):2345-73. doi: 10.1088/0031-9155/53/9/010. Epub 2008 Apr 17.
7
MR thermometry.磁共振温度测量法
J Magn Reson Imaging. 2008 Feb;27(2):376-90. doi: 10.1002/jmri.21265.
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Optimized and combined T1 and B1 mapping technique for fast and accurate T1 quantification in contrast-enhanced abdominal MRI.优化与联合的T1和B1映射技术用于对比增强腹部磁共振成像中快速准确的T1定量分析
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Investigating the effect of exchange and multicomponent T(1) relaxation on the short repetition time spoiled steady-state signal and the DESPOT1 T(1) quantification method.研究交换和多组分T(1)弛豫对短重复时间扰相稳态信号及DESPOT1 T(1)定量方法的影响。
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Whole-brain T1 mapping in multiple sclerosis: global changes of normal-appearing gray and white matter.多发性硬化症中的全脑T1映射:正常外观灰质和白质的整体变化。
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技术说明:在采用平均翻转角假设的可变翻转角方法中,二维激发轮廓对 T1 测量精度的影响。

Technical Note: The effect of 2D excitation profile on T1 measurement accuracy using the variable flip angle method with an average flip angle assumption.

机构信息

Utah Center for Advanced Imaging Research, University of Utah, Salt Lake City, UT, USA.

出版信息

Med Phys. 2017 Nov;44(11):5930-5937. doi: 10.1002/mp.12513. Epub 2017 Aug 31.

DOI:10.1002/mp.12513
PMID:28796308
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5689072/
Abstract

PURPOSE

To study the accuracy and precision of T estimates using the Variable Flip Angle (VFA) method in 2D and 3D acquisitions.

METHODS

Excitation profiles were simulated using numerical implementation of the Bloch equations for Hamming-windowed sinc excitation pulses with different time-bandwidth products (TBP) of 2, 6, and 10 and for T values of 295 ms and 1045 ms. Experimental data were collected in 5° increments from 5° to 90° for the same T and TBP values. T was calculated for every combination of flip angle with and without a correction for B and slice profile variation. Calculations were also made for flat slice profile such as obtained in 3D acquisition. Monte Carlo simulations were performed to obtain T measurement uncertainty.

RESULTS

VFA T measurements in 2D without correction can result in a 40-80% underestimation of true T . Flip angle correction can reduce the underestimation, but results in accurate measurements of T only within a narrow band of flip angle combinations. The narrow band of accuracy increases with TBP, but remains too narrow for any practical range of T values or B variation. Simulated noisy VFA T measurements in 3D were accurate as long as the two angles chosen are on either side of the Ernst angle.

CONCLUSIONS

Accurate T1 estimates from VFA 2D acquisitions are possible, but only a narrow range of T1 values within a narrow range of flip angle combinations can be accurately calculated using a 2D slice. Unless a better flip angle correction method is used, these results demonstrate that accurate measurements of T1 in 2D cannot be obtained robustly enough for practical use and are more likely obtained by a thin slab 3D VFA acquisition than from multiple-slice 2D acquisitions. VFA T measurements in 3D are accurate for wide ranges of flip angle combinations and T values.

摘要

目的

研究二维和三维采集中使用可变翻转角(VFA)方法的 T 估计的准确性和精密度。

方法

使用数值实现的 Bloch 方程模拟汉明窗 sinc 激发脉冲的激发谱,具有不同的时带宽积(TBP)为 2、6 和 10,以及 T 值为 295ms 和 1045ms。对于相同的 T 和 TBP 值,以 5°的增量从 5°收集到 90°的实验数据。对于每个翻转角组合,无论是否进行 B 和切片轮廓变化的校正,都计算了 T。还计算了类似于 3D 采集中获得的平坦切片轮廓的 T。进行了蒙特卡罗模拟以获得 T 测量不确定性。

结果

二维 VFA T 测量未经校正可能导致真实 T 值的 40-80%低估。翻转角校正可以减少低估,但仅在翻转角组合的窄带内准确测量 T。准确性的窄带随着 TBP 的增加而增加,但对于任何实际的 T 值或 B 变化范围仍然太窄。只要选择的两个角度在 Ernst 角的任一侧,模拟的 3D 嘈杂 VFA T 测量都是准确的。

结论

二维 VFA 采集可以准确估计 T1,但只能在非常窄的翻转角组合范围内准确计算非常窄的 T1 值。除非使用更好的翻转角校正方法,否则这些结果表明,二维中 T1 的准确测量不足以满足实际使用的要求,并且更有可能通过薄切片 3D VFA 采集而不是通过多层 2D 采集获得。3D 中的 VFA T 测量对于广泛的翻转角组合和 T 值是准确的。