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Multi-Coil Multi-Contrast Random Matrix Theory-Based Denoising for Liver Fat and R2* Quantification at 0.55T
Shu-Fu Shih1,2, Zhaohuan Zhang1,2, Bilal Tasdelen3, Ecrin Yagiz3, Sophia X. Cui4, Xiaodong Zhong4, Krishna S. Nayak3, and Holden H. Wu1,2
1Radiological Sciences, David Geffen School of Medicine, University of California Los Angeles, Los Angeles, CA, United States, 2Bioengineering, University of California Los Angeles, Los Angeles, CA, United States, 3Ming Hsieh Department of Electrical and Computer Engineering, University of Southern California, Los Angles, CA, United States, 4MR R&D Collaborations, Siemens Medical Solutions USA, Inc., Los Angles, CA, United States

Synopsis

Keywords: Low-Field MRI, Low-Field MRI

Liver fat and R2* quantification has been extensively validated at 1.5T and 3T. Recently, there is renewed interest in lower-field MRI because of potential advantages such as a larger bore and lower costs. However, it is challenging to acquire images with sufficient signal-to-noise ratio for accurate fat and R2* quantification at 0.55T. Previous random matrix theory (RMT)-based approaches leverage Gaussian noise characteristics to markedly reduce the noise without compromising the tissue signal. In this work, we investigated a multi-coil multi-contrast RMT-based denoising approach which is compatible with parallel imaging and we demonstrated improved liver fat and R2* quantification at 0.55T.

Introduction

Liver fat and R2* can be quantified using a multi-echo Dixon sequence followed by signal fitting to a model that resolves the fat spectrum and R2* 1-3. This approach has been extensively studied and validated at 1.5T and 3T1-3. In recent years, there is renewed interest in lower-field MRI (e.g., 0.55T) because of potential advantages such as a larger bore diameter and lower siting/hardware costs4-6. Previous studies investigated liver proton-density fat fraction (PDFF) and/or R2* quantification at lower fields7-9. However, it has been challenging to acquire images with sufficient signal-to-noise ratio (SNR) for accurate PDFF/R2* quantification. Recently, random matrix theory (RMT)-based denoising methods have been used in various MRI applications to improve image SNR10-12. RMT-based approaches leverage inherent Gaussian noise characteristics to markedly reduce the noise without compromising or smoothing the tissue signal10-12. Previous works on RMT denoising typically used datasets with large numbers of measurements/encodings or were performed in magnitude images only. Inspired by previous RMT denoising methods10-12, we investigated a multi-coil multi-contrast RMT-based denoising approach which can be compatible with parallel imaging and demonstrated its denoising capability for improving liver PDFF/R2* quantification at 0.55T.

Methods

RMT-based denoising: RMT shows that if the additive noise in a dataset has zero-mean Gaussian distribution, the singular values of the noise matrices will follow the Marchenko-Pastur distribution as long as the number of data samples/measurements is large enough13. Based on RMT, a theoretical upper bound of these singular values can be estimated and used to specifically remove the Gaussian noise from the data.

Several aspects need to be considered to apply RMT denoising in MRI images. First, sufficient number of data measurements is required to estimate noise characteristics. This limitation can be partially relieved by incorporating images from multiple coils and contrasts (e.g., multiple echo times). Second, parallel imaging is frequently used in clinical sequences. However, parallel imaging reconstruction can distort the noise characteristics and violate the noise assumptions in RMT.

Therefore, we used a reconstruction pipeline that allows us to apply RMT with parallel imaging (Figure 1). First, multi-coil multi-echo images were reconstructed using GeneRalized Autocalibrating Partially Parallel Acquisitions (GRAPPA), and divided by coil-by-coil g-factor maps14 to normalize noise characteristics. Second, the non-spatial dimensions were flattened into one dimension. Third, at each spatial location, a local patch with different coils and contrasts was extracted and flattened to a 2D matrix. Singular value shrinkage15 was performed using Marchenko-Pastur theory and the estimated noise variance. Fourth, multi-coil multi-echo images were scaled back by the coil-by-coil g-factor maps. Lastly, the multi-echo images were coil-combined16 and fitted to a 7-peak fat model with a single R2* term to generate PDFF and R2* maps17.

MRI Experiments: Two healthy subjects were scanned under an IRB-approved protocol, after providing written informed consent. Scans were performed using a whole-body 0.55T MRI system (prototype MAGNETOM Aera, Siemens Healthineers, Erlangen, Germany) equipped with high-performance shielded gradients (45 mT/m amplitude, 200 T/m/s slew rate). Phased-array receiver coils (18-channel spine array and 6-channel body array) were used. Data were acquired using a multi-echo gradient-echo 3D Cartesian sequence3. Key sequence parameters included TE=[2.16, 4.32, 6.48, 8.64, 10.8, 12.96]ms, TR=14.7ms, field of view=380x380mm2, slice thickness 5mm, and matrix size 192x192. Flip angle of 8° was used to balance between SNR and T1 bias for PDFF quantification. Parallel imaging factor R=2 was used for a single breath-hold acquisition (19 sec). For RMT denoising, a local patch size of 19x19x5 was used.

Results

Figure 2 shows the denoising performance in each coil in both magnitude and phase images. The signal difference between RMT-denoised and original single-coil-channel images exhibited Gaussian-like noise. Figures 3 and 4 compare coil-combined multi-echo images reconstructed with and without RMT denoising. RMT denoising improved image SNR without smoothing the tissue features. Figure 5 shows the reconstructed PDFF, R2*, and B0 field maps using RMT denoising. Based on ROI analysis on the quantitative maps, RMT denoising can provide PDFF quantification with a lower bias and R2* measurements with substantially reduced standard deviation because of less noise (i.e., enhanced SNR).

Discussion

Many previous RMT-based denoising methods only used coil-combined magnitude images11,12, which did not exploit the rich information across coils. Using the multi-coil information can increase the number of data samples by an order of magnitude to better comply with the RMT assumptions. In this work, we showed that if g-factor correction is not performed, the supposed noise removed by RMT denoising would deviate from a Gaussian distribution, increasing risk of removing or smoothing actual tissue signal. The proposed method makes RMT denoising compatible with parallel imaging acquisition and can be extended to different sequences and applications. It can especially benefit MRI applications at lower fields, which has a common fundamental challenge of low SNR. The performance of RMT denoising highly depends on the number of samples to accurately estimate the noise characteristics. In future work, we will investigate the required number of slices/contrasts for stable performance of RMT denoising.

Conclusion

We demonstrated that multi-coil multi-contrast RMT denoising can be compatible with parallel imaging acquisition and improved liver PDFF and R2* quantification at 0.55T.

Acknowledgements

We acknowledge grant support from the National Science Foundation (#1828736) and the National Institutes of Health (R01DK124417 and U01EB031894), and research support from Siemens Medical Solutions USA, Inc.

References

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Figures

Figure 1. Multi-coil multi-contrast random matrix theory (RMT)-based denoising pipeline for PDFF and R2* mapping. Multi-coil multi-echo k-space undersampled data were reconstructed using GRAPPA. Coil-by-coil g-factor maps were used to normalize the noise characteristics. Complex signals in local patches were extracted and flattened. Singular value shrinkage was applied to remove only Gaussian-like noise. The whole dataset was denoised after all the local patches were processed. Coil-combination and fat-water signal fitting were performed to generate the PDFF and R2* maps.

Figure 2. (a,b) Representative results comparing noise characteristics from g-factor-corrected coil images, images after RMT denoising, and their signal difference. Phase information, which is critical in fat-water separation, can be recovered in low-SNR regions (red arrows). (c) Histogram showing the distribution of the signal difference across the entire multi-coil multi-contrast images. (d) Signal difference compared to Gaussian-distributed signal. The signal difference deviates from Gaussian distribution if the g-factor was not corrected.


Figure 3. Example of reconstructed coil-combined 6-echo images from a 28-year-old male for (a) conventional GRAPPA reconstruction, and (b) GRAPPA reconstruction with RMT denoising. RMT denoising removed the Gaussian noise and improved image quality and sharpness in the multi-echo images. OP: out-of-phase; IP: in-phase.


Figure 4. Example of reconstructed coil-combined 6-echo images from a 27-year-old male for (a) conventional GRAPPA reconstruction, and (b) GRAPPA reconstruction with RMT denoising. RMT denoising removed the Gaussian noise and improved image quality and sharpness in the multi-echo images. OP: out-of-phase; IP: in-phase.


Figure 5. Reconstructed liver PDFF, R2*, and B0 field maps with and without RMT denoising from the subjects in Figures 3 and 4, respectively. The conventional reconstruction results suffer from lower SNR, which led to quantification errors or noisy quantitative estimates. RMT denoising can improve the quantitative maps.

Proc. Intl. Soc. Mag. Reson. Med. 31 (2023)
0311
DOI: https://doi.org/10.58530/2023/0311