Jiafu Wei1, Zhiguang Mo1, Enhua Xiao1, Chao Luo1, Jiaxu Li1, and Ye Li1,2
1Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen, China, 2Key Laboratory for Magnetic Resonance and Multimodality Imaging of Guangdong Province, Shenzhen, China
Synopsis
Keywords: Non-Array RF Coils, Antennas & Waveguides, RF Arrays & Systems, signal-to-noise ratio, high-resolution, cryogenic, RF coils.
Motivation: The signal-to-noise ratio of high-field RF surface coils decays with distance, and we propose cryogenic coils to compensate for the SNR of MR Imaging.
Goal(s): The cryogenic coil in our work aims to significantly improve the SNR of the images at long distances while guaranteeing a large imaging FOV.
Approach: We design a large size RF coil and cool it down for rat imaging.
Results: The experimental results show that the cryogenic coil obtained a SNR of 1.8-fold higher than a room-temperature coil and 1.1-fold higher than that of a commercial multi-channel rat coil.
Impact: The designed coil can help to improve the quality of MR imaging in some scenarios where the object to be measured is far away from the RF receive coil.
Synopsis
Many methods
exist to enhance MRI imaging performance under a constant main
magnetic field. This study
proposes that reducing the coil temperature can significantly enhance the signal-to-noise
ratio (SNR) of the images at a greater imaging distance. The cryogenic coil can
provide a 1.8-fold increase in the SNR gain compared to a room-temperature coil.
It is noteworthy that our homemade cryogenic coil has a 1.1-fold higher SNR
gain times than the commercially available rat coils. As cooling down the coil
without a complex cryogenic system is easy to use and cost-effective, it can
work as an additional option for acquiring high-resolution images for scientific
research and clinical application.Introduction
Cryogenic coils have been reported that they can
enhance the SNR of MR images for general small-animal imaging. The general SNR
gain of a receive coil is determined by sample noise, coil noise,etc1,2, where the distance between
the sample and the coil significantly affects the signal noise. Previous
studies have shown that cryogenic coils (including superconducting coils) can
improve the overall SNR by reducing the coil noise, but usually require the
cryogenic coil to be very close to the sample, which puts high demands on the
cooling system. In this work, we demonstrate that cryogenic coils can still
improve the SNR of images at a longer distance for MR imaging.Methods
Fig.1
shows our homemade single-channel RF receive-only coil.
The diameter of the typical cryogenic copper coil is less than 2 cm3,4, but considering the larger size of the rat
compared to smaller animals, we choose a diameter of 4 cm, which guarantees a better
radiofrequency field and FOV. When the coil works at 77K, we add liquid
nitrogen to the Dewar. In addition, another room-temperature coil with a same
circuit is used for comparison. The coil is located approximately 3 cm above
the head surface of a rat as shown in Fig.1, which is almost an order of
magnitude larger than the previously reported typical imaging distance of 5 mm
of cryogenic surface coils3,5.
We then evaluate the Q value of
the two coils in both the unloaded and loaded cases based on a commercial
network analyzer.
In
this work, we investigate three different RF receive coils: room-temperature
coil (RC), cryogenic coil (CC), and commercial 12-channel rat coil (Com) with
an inner diameter of 6.8 cm. For SNR calculation and high-resolution images at a test distance of 3cm, we scan the transverse (TRA)
plane and the sagittal (SAG) plane of the rat on a 3T MRI scanner (uMR 790,
Shanghai United Imaging Healthcare) using a T2
FSE sequence ( For high-resolution scanning: TR/TE=4500ms/85.1ms, FOV= 50mm× 50mm for TRA, thickness = 2.0mm,
flip angle= 90°, average number of repetitions = 2, scan time = 02:56min).Results
According to Table I, the loaded Q
values of both coils vary slightly compared to the unloaded Q. This
suggests that the coil noise dominates the whole noise of this experiment at a
distance of 3 cm. Then we can see the loaded Q of CC is enhanced by a
factor of 1.43 compared to that of RC which is approximately consistent with
the comparison of the SNR map of CC and RC according
to the classical calculation model between Q and SNR6,7. Therefore, we
can demonstrate that decreasing the coil noise can result in a considerable
enhancement of its intrinsic performance, even at an imaging distance of 3 cm.
Furthermore, it also offers significantly clearer images than the commercial 12-channel
coil in the upper half of the field of vision (FOV).
The
SNR map shown in Fig.2 (a) and Fig.2 (b) demonstrates that the cryogenic coil
achieves a 1.8-fold SNR gain and it is significantly better than the commercial
rat coil at a 3 cm distance. This strongly validates the performance advantage
of the cryogenic coil. The imaging results also show that we can obtain a high
SNR gain under the premise of expanding the coil diameter and imaging FOV. Fig.
3 presents high-resolution images of the same slice of the rat brain region
under three conditions. The results indicate that cooling down the coil
enhan over all three cases.Discussions and Conclusions
The cryogenic coil in our work
can significantly improve the SNR of the images at long distances while
guaranteeing a large imaging FOV, and demonstrates a better performance than a type
of commercial rat coil under the same conditions. The designed coil can help to improve the quality of MR
imaging in some scenarios where the object to be measured is far away from the
RF receive coil.Acknowledgements
This
work was supported in part by the Project on Global Common Challenges of
Chinese Academy of Sciences (No. 321GJHZ2022081GC), the NSFC grant (U22A20344),
the Key Laboratory for Magnetic Resonance and Multimodality Imaging of
Guangdong Province (2023B1212060052), the Funding Program of Shenzhen, China (RCYX20200714114735123),
the Chinese Academy of Sciences Youth Innovation Promotion Association funded
project (Y2021098).
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