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本文引用的文献

1
Transceiver-Phased Arrays for Human Brain Studies at 7 T.用于7T人脑研究的收发相控阵
Appl Magn Reson. 2011 Dec;41(2-4):483-506. doi: 10.1007/s00723-011-0280-y.
2
A conformal transceive array for 7 T neuroimaging.用于 7T 神经成像的共形收发阵列。
Magn Reson Med. 2012 May;67(5):1487-96. doi: 10.1002/mrm.23124. Epub 2011 Aug 16.
3
ICE decoupling technique for RF coil array designs.射频线圈阵列设计的 ICE 去耦技术。
Med Phys. 2011 Jul;38(7):4086-93. doi: 10.1118/1.3598112.
4
Size-optimized 32-channel brain arrays for 3 T pediatric imaging.用于 3T 儿科成像的优化尺寸 32 通道脑阵列。
Magn Reson Med. 2011 Dec;66(6):1777-87. doi: 10.1002/mrm.22961. Epub 2011 Jun 7.
5
A 32-channel lattice transmission line array for parallel transmit and receive MRI at 7 tesla.一种用于 7 特斯拉并行发射和接收 MRI 的 32 通道晶格传输线阵列。
Magn Reson Med. 2010 Jun;63(6):1478-85. doi: 10.1002/mrm.22413.
6
Shielded microstrip array for 7T human MR imaging.用于 7T 人体磁共振成像的屏蔽微带阵列。
IEEE Trans Med Imaging. 2010 Jan;29(1):179-84. doi: 10.1109/TMI.2009.2033597. Epub 2009 Oct 9.
7
An eight-channel phased array RF coil for spine MR imaging at 7 T.用于 7T 脊柱磁共振成像的八通道相控阵射频线圈。
Invest Radiol. 2009 Nov;44(11):734-40. doi: 10.1097/RLI.0b013e3181b24ab7.
8
Short echo spectroscopic imaging of the human brain at 7T using transceiver arrays.使用收发阵列在7T对人脑进行短回波磁共振波谱成像。
Magn Reson Med. 2009 Jul;62(1):17-25. doi: 10.1002/mrm.21970.
9
Insight into RF power requirements and B1 field homogeneity for human MRI via rigorous FDTD approach.通过严格的时域有限差分法深入了解人体磁共振成像的射频功率要求和B1场均匀性。
J Magn Reson Imaging. 2007 Jun;25(6):1235-47. doi: 10.1002/jmri.20919.
10
Reduction of transmitter B1 inhomogeneity with transmit SENSE slice-select pulses.使用发射敏感编码(SENSE)切片选择脉冲减少发射机B1不均匀性。
Magn Reson Med. 2007 May;57(5):842-7. doi: 10.1002/mrm.21221.

收发器阵列的谐振感应去耦 (RID) 可补偿互阻抗的电抗和电阻分量。

Resonant inductive decoupling (RID) for transceiver arrays to compensate for both reactive and resistive components of the mutual impedance.

机构信息

Department of Neurosurgery, Yale University, New Haven, CT, USA.

出版信息

NMR Biomed. 2013 Nov;26(11):1547-54. doi: 10.1002/nbm.2989. Epub 2013 Jun 18.

DOI:10.1002/nbm.2989
PMID:23775840
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC3800502/
Abstract

Transceiver surface coil arrays improve transmit performance (B1/√kW) and B1 homogeneity for head imaging up to 9.4 T. To further improve reception performance and parallel imaging, the number of array elements must be increased with a corresponding decrease in their size. With a large number of small interacting antennas, decoupling is one of the most challenging aspects in the design and construction of transceiver arrays. Previously described decoupling techniques using geometric overlap, inductive or capacitive decoupling have focused on the elimination of the reactance of the mutual impedance only, which can limit the obtainable decoupling to -10 dB as a result of residual mutual resistance. A novel resonant inductive decoupling (RID) method, which allows compensation for both reactive and resistive components of the mutual impedance between the adjacent surface coils, has been developed and verified experimentally. This method provides an easy way to adjust the decoupling remotely by changing the resonance frequency of the RID circuit through the adjustment of a variable capacitor. As an example, a single-row (1 × 16) 7-T transceiver head array of n = 16 small overlapped surface coils using RID decoupling between adjacent coils was built. In combination with overlapped coils, the RID technique achieved better than -24 dB of decoupling for all adjacent coils.

摘要

收发表面线圈阵列可提高发射性能(B1/√kW),并在 9.4T 以内提高头部成像的 B1 均匀性。为了进一步提高接收性能和并行成像,必须增加阵列元件的数量,同时相应减小其尺寸。对于大量相互作用的小天线,去耦是收发阵列设计和构建中最具挑战性的方面之一。以前描述的使用几何重叠、电感或电容去耦的去耦技术仅侧重于消除互阻抗的电抗,由于残余互电阻,这可能将可获得的去耦限制为-10dB。已经开发并通过实验验证了一种新的谐振电感去耦(RID)方法,该方法允许补偿相邻表面线圈之间互阻抗的电抗和电阻分量。通过调整可变电容器来改变 RID 电路的谐振频率,这种方法提供了一种远程调整去耦的简单方法。例如,使用 RID 去耦在相邻线圈之间构建了一个 7-T 的单排(1×16)16 个小型重叠表面线圈的收发头阵列。与重叠线圈结合使用时,RID 技术实现了所有相邻线圈之间优于-24dB 的去耦。