Georgiy Solomakha1, Svetlana Egorova1, Alena Shchelokova1, Egor Kretov1, and Stanislav Glybovski1
1Department of Physics and Engineering, ITMO University, Saint Petersburg, Russian Federation
Synopsis
This work proposes a novel transmit
radiofrequency coil integrated into the scanner bore for whole-body MRI for 7
Tesla MRI based on patch antennas. Numerical studies with a homogeneous phantom
demonstrated 4.5-fold higher transmit efficiency in the phantom center compared
to the state-of-the-art bore integrated stripline array.
Synopsys
This
work proposes a novel transmit
radiofrequency coil integrated into the scanner bore for whole-body MRI for 7
Tesla MRI based on patch antennas. Numerical studies with a homogeneous phantom
demonstrated 4.5-fold higher transmit efficiency in the phantom center than the
state-of-the-art bore integrated stripline array.Purpose
To
develop and characterize numerically novel and efficient bore-integrated coil
based on patch antenna array for 7 Tesla whole-body MRI.Introduction
Ultra-high
field (field strength higher than 7 Tesla) imaging is an extensively developing
field. Recently UHF MRI-scanner was approved for limited clinical use for head
and extremity imaging with static CP-mode excitation [1]. For the body imaging
at such high field strengths, volume coils integrated to RF-shield of
MR-scanner became inefficient because of strongly inhomogeneous RF-magnetic
field in the human body due to interference effects [2]. To obtain a homogenous
field in the desired region, local transmit arrays combined with the so-called
RF-shimming procedure [3]. A recently different approach based on eight
stripline coils integrated into the bore of the 7 T scanner was introduced [3].
Such design allows to reduce SAR and optimize receive and transmit coils
separately but suffers from the low Tx-efficiency. This work presents a new
bore integrated array for a 7 T MRI of the human body. The proposed body array
elements demonstrate 4.48 times better B1 in the desired region than the bore
integrated stripline array [3].
Patch-antennas
are well known in the microwave frequency range as low profile and robust
solutions with a simple design that can efficiently operate near the conducting
surfaces. Patch antenna consists of the metallic half-wavelength sheet (patch)
with a rectangular shape above the electric shield. The operation principle of
the patch antenna is based on the excitation of TE10 eigenmode in the volume
under the patch. This resonant mode excites two linear equivalent magnetic
currents at the edges of the patch. Such currents act as two in-phase slot
antennas. Patch antennas were already proposed for MRI application as
CP-polarized forward view antenna for the head [4] or small animal imaging [5].
Here, we describe and demonstrate in simulations a new bore integrated array
for a 7 T MRI of the human body based on patch antennas that allow increasing
Tx-efficiency 4.48 times compared to the state-of-the-art stripline array.
Methods
The
design of the proposed bore-integrated array is presented in Figure 1. It consists
of an octagonal-shaped bore with 680 mm diameter and eight patch antennas with
air substrate. In planar configuration, patch antennas with aligned radiating
slots are well decoupled. When these eight antennas are placed in the bore
environment, coupling between them becomes significant. Passive magnetic
resonators were inserted between non-radiating slots of the patch antennas. The
passive magnetic resonator consisted of two loops connected with two
capacitors.
The
total length of the patch was chosen 460 mm to be resonant at the 298 MHz
frequency inside the bore. The width of each element was chosen at 200 mm to
fit the eight-channel configuration. A bore integrated stripline array was used
as a reference coil array. For numerical simulation, the finite-element method
implemented in CST Microwave Studio 2021 software was used. Decoupling and
resonant frequency of patches were adjusted by changing the length of the
magnetic resonator.Results
Figure
2 demonstrates the distribution of B1+ for two circular polarized modes, CP1
(45 deg phase lag between element) and CP2 (90 deg phase lag between element),
both for patch and stripline arrays in the central axial plane of the
elliptical phantom. CP1 mode of both arrays gives maximum field in the center.
The same field distribution in the sagittal plane is depicted in Figure 3. The power balance of numerical simulation, B1+ value in the
center of the homogenous phantom, local SAR-maxima value, and SAR-efficiency
for the phantom center presented in Table 1Conclusion
We
developed a novel concept of a bore-integrated coil for 7 Т body imaging. We
can conclude from the presented results that the proposed coil increases
Tx-efficiency 4.47 times compared to the stripline array. . However, the SAR efficiency of the proposed and reference was almost
the same. Measured S11 for the
reference and proposed array lower than -20 dB. The coupling between neighbor
elements of the patch array was -3 dB. With an additional decoupling resonator,
it was improved to the -15 dB level. In the future, we plan to perform a
numerical evaluation with a voxel model for SAR performance evaluation and
on-bench and MRI measurements of the prosed coil. After successful evaluation
proposed design could be used as a prototype for the first bore-integrated
transmit coil for clinical 7 Tesla MRI.Acknowledgements
This work was supported by the Russian Science Foundation (Project 21-19-00707).References
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