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Acceleration of IR-prepared Ultra Short Echo Time Imaging of Bones exploiting a Plug-and-Play Denoising Prior
Philipp Hans Nunn1, Oliver Schad1, Jan-Peter Grunz1, Johannes Tran-Gia2, and Tobias Wech1
1Department of Diagnostic and Interventional Radiology, University Hospital Würzburg, Würzburg, Germany, 2Department of Nuclear Medicine, University Hospital Würzburg, Würzburg, Germany

Synopsis

Keywords: Bone, Bone, Plug-and-Play Denoiser, IR-UTE, AI and Machine Learning

Motivation: (IR-)UTE MRI enables (quantitative) investigation of bony tissue. Imaging protocols, however, are still time consuming.

Goal(s): To develop a reconstruction method, which can transfer undersampled / accelerated IR-UTE scans of bone into high quality images.

Approach: A thresholded Landweber algorithm was implemented, which uses both an L1-sparsity model and a pre-trained denoising convolutional network as regularizers of the physical MR model.

Results: The reconstruction method was capable of delivering superior image quality compared to reconstructions based on straightforward NUFFT or iterative SENSE, especially in the case of significant undersampling.

Impact: IR-UTE imaging accelerated by our proposed reconstruction based on L1-sparsity and a pre-trained denoising convolutional neural network shortens investigations by a factor of up to five, thereby facilitating further research on the topic as well as clinical transfer.

Introduction

MR-based depiction of bony tissue is increasingly being investigated as a radiation-free alternative to computed tomography for various diagnostic questions. However, to reach adequate image quality, lengthy exams are typically still required. In this work, we implemented and tested a deep learning driven strategy to shorten the overall acquisition time in IR-prepared ultra-short echo time (UTE) MR imaging.

Methods

An IR-prepared UTE sequence similar to [1] was implemented in Pulseq [2] (see Fig. 1). Data sampling was performed using ramp sampling and a 3D radial trajectory, equally distributed on the k-space sphere (a.k.a koosh ball). Using a long adiabatic inversion pulse, this approach suppresses the signal of tissues with longer T2 relaxation times, thereby enabling a robust differentiation of compartments of cortical and trabecular bone with short T2*. For each adiabatic IR pulse, seven projections centered around TI = 64$$$\ $$$ms were recorded with a temporal spacing of τ = 4.1$$$\,$$$ms between each. The adiabatic IR pulse had the shape of a hyperbolic secant with a duration of 10$$$\,$$$ms centered around -220 Hz, which corresponds to the midpoint between fat and water at 3$$$\,$$$T. kmax corresponded to an isotropic spatial resolution of 1.6$$$\,$$$mm. Sample data were acquired in the left ankle of one healthy volunteer and the head of another at 3$$$\,$$$T field strength (Siemens Magnetom Prisma). Benchmark data consisting of 56$$$\,$$$k projections, as well as prospectively undersampled data with 21$$$\,$$$k projections were acquired in 20:00$$$\,$$$min (ankle) and 7:30$$$\,$$$min (head) scan time. The corresponding minimum FOV (corresponding to largest gap in k-space until kmax) was 21$$$\,$$$cm for 56$$$\,$$$k projections and 13$$$\,$$$cm for 21$$$\,$$$k projections. From the fully sampled dataset (ankle), undersampled versions were simulated by retrospectively removing projections to build sets with 28$$$\,$$$k and 11.2$$$\,$$$k respectively. Higher acceleration was also simulated in the head dataset by using only half of the acquired data (10.5$$$\,$$$k projections).
To enable the reconstruction of undersampled and thus accelerated scans, a thresholded Landweber styled algorithm was implemented which features the enforcement of the physical measurement model (acquired data $$$y$$$, coil sensitivities), the sparsity in image space (minimization of L1-norm) as well as the integration of a pre-trained denoising convolutional neural network (DnCNN,[3]). In the current version of the algorithm, we used an “off-the-shelf” DnCNN model provided by MathWorks, not specifically trained for bone MRI.

Pseudo-code:

Input: $$$x_{0} = A^{*}y, \gamma = 1, P_{0}=angle(x_{0})$$$
for $$$m=1,2,...,n$$$
$$$\,\,\,\,\,\,\,\,$$$$$$x_{m}=x_{m-1}-\gamma A^{*}(Ax_{m-1}-y)$$$
$$$\,\,\,\,\,\,\,\,$$$$$$x_{m}=real(x_{m}\circ e^{i\cdot(-P_{m-1})})$$$
$$$\,\,\,\,\,\,\,\,$$$$$$x_{m}=DnCNN(x_{m})$$$
$$$\,\,\,\,\,\,\,\,$$$$$$x_{m}=x_{m}\circ e^{i\cdot P_{m-1}}$$$
$$$\,\,\,\,\,\,\,\,$$$$$$x_{m}=STH_{\sigma}(x_{m})$$$
$$$\,\,\,\,\,\,\,\,$$$$$$P_{m}=angle(x_{m})$$$
end
return $$$x_{n}$$$

Matrix $$$A$$$ represents the MRI operator including a 3D gridding procedure [4], initialized with the trajectory information and the coil sensitivities, which were estimated from the densely sampled central part of the 3D k-space using ESPIRIT [5]. $$$x_{0}$$$ was determined by a “naïve reconstruction” using a grid size of 256 x 256 x 256. $$$STH_{\sigma}$$$ applies a soft threshold in image space with a threshold of $$$\sigma$$$, which was determined empirically based on the noise level. A number of $$$n$$$ = 15 was chosen for the reconstruction of the ankle dataset, and $$$n$$$ = 13 for the head dataset. In the following, we refer to the proposed method as S3MOB (Speedy 3D MRI Of Bone). For comparison, conjugate gradient SENSE [6] was applied to the same datasets.

Results

Fig. 2 and Fig. 3 depict the reconstructions of ankle and head data for naïve gridding reconstruction, iterative SENSE, and the proposed S3MOB method with different numbers of acquired projections. With 56$$$\,$$$k projections, the naïve reconstruction results in a depiction of the ankle with low artifact level, good SNR and sharp edges (Fig. 2). Since the data is not fully sampled in the periphery of k-space, iterative SENSE could increase sharpness slightly, however at the cost of also increasing noise. This effect is more pronounced for higher acceleration factors. The application of S3MOB resulted in a good compromise between sharpness, SNR and artifact level. This is confirmed by the head data shown in Fig. 3. Bone microstructure could be resolved with good SNR, even with only 10.5$$$\,$$$k projections, corresponding to an acquisition time of 3:45$$$\,$$$min. Using an NVIDIA RTX A6000 GPU (48$$$\,$$$GB), the reconstruction time for S3MOB was between one (10.5$$$\,$$$k projections) and seven minutes (56$$$\,$$$k projections) for the presented examples.

Discussion & Conclusion

The proposed data-driven S3MOB technique represents a promising method to accelerate MRI in bony tissues. Next steps include training the denoising CNN specifically for the imaging task, studying the impact of the acceleration on quantitative imaging (T2*- or proton density mapping) as well as the combination with alternative means of acceleration, e.g. exploiting more efficient trajectories like FLORET [7].

Acknowledgements

Presented work was partially funded by the Interdisciplinary Center for Clinical Research in Würzburg under Research Grant F-437.

References

1. Ma, Y-J, Chen, Y, Li, L, et al. Trabecular bone imaging using a 3D adiabatic inversion recovery prepared ultrashort TE Cones sequence at 3T. Magnetic Resonance in Medicine 2020:1640–1651. https://doi.org/10.1002/mrm.28027.

2. Layton KJ, Kroboth S, Jia F, Littin S, Yu H, Leupold J, Nielsen JF, Stocker T, Zaitsev M. Pulseq: A rapid and hardware-independent pulse sequence prototyping framework. Magnetic Resonance in Medicine 2017:1544-1552 doi: 10.1002/mrm.26235.

3. Zhang, K, Zuo, W, Chen, Y, Meng, D, Zhang, L. Beyond a Gaussian Denoiser: Residual Learning of Deep CNN for Image Denoising. IEEE Transactions on Image Processing 2017:3142-3155 doi: 10.1109/TIP.2017.2662206.

4. MATLAB implementation of Non-Uniform Fast Fourier Transform in 3D. https://github.com/marcsous/nufft_3d. Accessed October 31, 2023.

5. BART Toolbox for Computational Magnetic Resonance Imaging, Version v0.7.00. https://mrirecon.github.io/bart/. Accessed October 31, 2023.

6. Pruessmann KP, Weiger M, Börnert P, Boesiger P. Advances in sensitivity encoding with arbitrary k-space trajectories. Magnetic Resonance in Medicine 2001:638-651. doi: 10.1002/mrm.1241.

7. Yoneyama, M, Azuma, M, et al. Volume isotropic 3D bone Imaging with broadband IR-prepared FLORET UTE and Fibonacci interleaved trajectory ordering. Proceedings of the International Society for Magnetic Resonance in Medicine 2023:0632.

Figures

Schematic representation of the utilized sequence. (A): Adiabatic pulse followed by seven projections with the central projection beginning at TI = 64 ms where magnetization of long T2 is supposed to reach zero crossing. Interval between two consecutive adiabatic IR pulses is TR = 150 ms. (B): Single excitation pulse and projection, τ = 4.1 ms denotes the time interval between two RF pulses. Ramp sampling and small TE = 50 µs are applied for optimal contrast. (C): 3D representation of radial koosh ball trajectory.

Sagittal slice from 3D reconstruction of the left ankle of a healthy volunteer using the different reconstruction methods and number of projections. While CG-SENSE was capable of increasing sharpness, which is evident in naïve reconstructions due to increasing gaps of the koosh ball trajectory in the periphery of k-space, noise is also considerably amplified. The proposed technique yields a comparably high SNR and low artifact level. For 28 k, resolution appears slightly inferior to the CG-SENSE reconstruction.

Transversal slice (top) and sagittal slice (bottom) from 3D reconstruction of the head of a healthy volunteer using the different reconstruction methods and number of projections. Overall, the proposed technique yields sharp depiction of the bone microstructure at reduced noise levels.

Proc. Intl. Soc. Mag. Reson. Med. 32 (2024)
1522
DOI: https://doi.org/10.58530/2024/1522