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Recent developments in the field of radiofrequency (RF) coils for magnetic resonance imaging (MRI) offer flexible and patient-friendly solutions. Previously, we demonstrated a proof-of-concept single-element stretchable coil design based on liquid metal and a self-tuning smart geometry. In this work, we numerically analyze and experimentally study a multi-channel stretchable coil array and demonstrate its application in dynamic knee imaging. We also compare our flexible coil array to a commonly used commercial rigid coil array. Our numerical analysis shows that the proposed coil array maintains its resonance frequency (<1% variation) and sensitivity (<6%) at various stretching configurations from 0% to 30%. We experimentally demonstrate that the signal-to-noise ratio (SNR) of the acquired MRI images is improved by up to four times with the stretchable coil array due to its conformal and therefore tight-fitting nature. This stretchable array allows for dynamic knee imaging at different flexion angles, infeasible with traditional, rigid coil arrays. These findings are significant as they address the limitations of current rigid coil technology, offering a solution that enhances patient comfort and image quality, particularly in applications requiring dynamic imaging.
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http://dx.doi.org/10.3390/ma17133325 | DOI Listing |
Biomed Phys Eng Express
September 2025
Institute of Electrical Engineering Chinese Academy of Sciences, No.6, Zhongguancun Road, Haidian District, Beijing , China, Beijing, Beijing, 100190, CHINA.
Objective: Transcranial magnetic stimulation (TMS) is a promising neuromodulation therapy for treating diseases such as depression and Alzheimer's disease. However, its efficacy depends on precise magnetic field targeting. Current measurement methods face a trade-off between accuracy and complexity.
View Article and Find Full Text PDFIEEE Trans Biomed Eng
September 2025
The multi-channel synchronous stimulator, aimed at achieving efficient and precise neural regulation, typically utilizes a monolithic microelectrode array structure. However, this structure limits the flexibility of electrode placement and the expansion to a large number of nodes, particularly in discontinuous locations. To address this, this paper designs a distributed passive micro-magnetic stimulation (DP-μMS) neuro-regulation device with multi-brain region collaborative stimulation functionality.
View Article and Find Full Text PDFNMR Biomed
October 2025
Athinoula A. Martinos Center for Biomedical Imaging, Massachusetts General Hospital, Charlestown, Massachusetts, USA.
∆B shim optimization performed at the beginning of an MR scan is unable to correct for ∆B field inhomogeneities caused by patient motion or hardware instability during scans. Navigator-based methods have been demonstrated previously to be effective for motion and shim correction. The purpose of this work was to accelerate volumetric navigators to allow fast acquisition of the parent navigated sequence with short real-time feedback time and high spatial resolution of the ∆B field mapping.
View Article and Find Full Text PDFJ Magn Reson
August 2025
School of Information Technology and Electrical Engineering, University of Queensland, Brisbane, QLD 4072, Australia. Electronic address:
Gradient coils play a critical role in magnetic resonance imaging (MRI) systems by enabling spatial encoding through generating rapidly switching magnetic fields. However, these time-varying fields induce eddy currents in surrounding conductive structures, leading to gradient field distortions and imaging artifacts. In this study, we propose an automatic eddy current compensation method implemented on a field-programmable gate array (FPGA) platform.
View Article and Find Full Text PDFThis study presents the design, simulation, and experimental validation of a novel multimodal concentric surface coil for MR imaging, developed to achieve higher B1 field efficiency while maintaining low SAR for enhanced imaging performance. The coil comprises multiple electromagnetically coupled concentric resonators of varying sizes. The resonant frequency of a desired mode is tuned to 127 MHz, as an example, to demonstrate the performance of the proposed technique at 3 Tesla.
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