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采用环形和偶极天线逼近最终的固有信噪比。

Approaching ultimate intrinsic signal-to-noise ratio with loop and dipole antennas.

机构信息

Center for Advanced Imaging Innovation and Research and Bernard and Irene Schwartz Center for Biomedical Imaging, Department of Radiology, New York University School of Medicine, New York, New York, USA.

The Sackler Institute of Graduate Biomedical Sciences, New York University School of Medicine, New York, New York, USA.

出版信息

Magn Reson Med. 2018 Mar;79(3):1789-1803. doi: 10.1002/mrm.26803. Epub 2017 Jul 4.

DOI:10.1002/mrm.26803
PMID:28675512
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5754268/
Abstract

PURPOSE

Previous work with body-size objects suggested that loops are optimal MR detectors at low fields, whereas electric dipoles are required to maximize signal-to-noise ratio (SNR) at ultrahigh fields ( ≥ 7 T). Here we investigated how many loops and/or dipoles are needed to approach the ultimate intrinsic SNR (UISNR) at various field strengths.

METHODS

We calculated the UISNR inside dielectric cylinders mimicking different anatomical regions. We assessed the performance of various arrays with respect to the UISNR. We validated our results by comparing simulated and experimental coil performance maps.

RESULTS

Arrays with an increasing number of loops can rapidly approach the UISNR at fields up to 3 T, but are suboptimal at ultrahigh fields for body-size objects. The opposite is true for dipole arrays. At 7 T and above, 16 dipoles provide considerably larger central SNR than any possible loop array, and minimal g factor penalty for parallel imaging.

CONCLUSIONS

Electric dipoles can be advantageous at ultrahigh fields because they can produce both curl-free and divergence-free currents, whereas loops are limited to divergence-free contributions only. Combining loops and dipoles may be optimal for body imaging at 3 T, whereas arrays of loops or dipoles alone may perform better at lower or higher field strengths, respectively. Magn Reson Med 79:1789-1803, 2018. © 2017 International Society for Magnetic Resonance in Medicine.

摘要

目的

以往对体型物体的研究表明,在低场下,环路是最优的磁共振探测器,而在超高场(≥7T)下,需要电偶极子来最大化信噪比(SNR)。在此,我们研究了在不同场强下需要多少个环路和/或电偶极子才能接近极限固有 SNR(UISNR)。

方法

我们计算了模拟不同解剖区域的介电圆柱内的 UISNR。我们评估了各种阵列相对于 UISNR 的性能。我们通过比较模拟和实验线圈性能图来验证我们的结果。

结果

随着环路数量的增加,阵列可以在高达 3T 的场强下快速接近 UISNR,但在超高场强下对体型物体的性能并不理想。对于偶极子阵列则相反。在 7T 及以上,16 个偶极子提供的中心 SNR 明显大于任何可能的环路阵列,并且对并行成像的最小 g 因子惩罚也较小。

结论

在超高场强下,电偶极子可能具有优势,因为它们可以产生无旋和无散电流,而环路仅局限于无散电流贡献。在 3T 时,环路和偶极子的组合可能是体成像的最佳选择,而单独的环路或偶极子阵列在较低或较高场强下的性能可能更好。磁共振医学 79:1789-1803, 2018。©2017 国际磁共振学会。

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本文引用的文献

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NMR Biomed. 2017 May;30(5). doi: 10.1002/nbm.3691. Epub 2017 Feb 10.
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The ultimate signal-to-noise ratio in realistic body models.真实人体模型中的最终信噪比。
Magn Reson Med. 2017 Nov;78(5):1969-1980. doi: 10.1002/mrm.26564. Epub 2016 Dec 4.
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Dependence of B1+ and B1- Field Patterns of Surface Coils on the Electrical Properties of the Sample and the MR Operating Frequency.表面线圈的B1+和B1-场模式对样品电学性质及磁共振工作频率的依赖性。
Concepts Magn Reson Part B Magn Reson Eng. 2016 Feb;46(1):25-40. doi: 10.1002/cmr.b.21319. Epub 2016 Feb 4.
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Magn Reson Med. 2017 Feb;77(2):884-894. doi: 10.1002/mrm.26153. Epub 2016 Feb 17.
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NMR Biomed. 2016 Sep;29(9):1122-30. doi: 10.1002/nbm.3356. Epub 2015 Aug 17.
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The fractionated dipole antenna: A new antenna for body imaging at 7 Tesla.分段偶极子天线:一种用于7特斯拉人体成像的新型天线。
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