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3D Free-Breathing Ungated Spiral bSSFP Functional Cardiac Imaging Using a Deep Image Prior
Jesse Ian Hamilton1,2, Gastao Lima da Cruz1, and Nicole Seiberlich1,2
1Radiology, University of Michigan, Ann Arbor, MI, United States, 2Biomedical Engineering, University of Michigan, Ann Arbor, MI, United States

Synopsis

Keywords: Machine Learning/Artificial Intelligence, Cardiovascular, deep learning; spiral; real-time CMR

Motivation: Real-time imaging methods are useful for patients with limited breathhold capacity or arrhythmias, but are typically limited to 2D scans that prevent evaluation of wall motion in 3D over the heart.

Goal(s): The goal of this project is to develop a technique for 3D real-time (free-breathing ungated) cine imaging.

Approach: The proposed method combines a highly undersampled 3D stack-of-spirals trajectory with a deep image prior reconstruction, which does not require ground truth training data.

Results: Real-time 3D imaging is demonstrated in healthy subjects with temporal resolutions of 36ms per volume at 1.5T and 58ms per volume at 0.55T.

Impact: Real-time 3D imaging could enable streamlined cardiac MRI exams, with whole-heart 3D cine images obtained in 10s without breathholds or gating. This technique may also simplify quantification compared to 2D real-time methods, since motion is synchronized over all partitions.

Introduction

Real-time imaging methods are useful for patients with limited breathhold capacity or arrhythmias but are typically limited to 2D scans. Different slices are collected at different points in time, precluding evaluation of wall motion in 3D over the entire heart. Additionally, measuring ventricular volumes and ejection fraction (EF) can be labor-intensive, as images at diastole and systole must be identified for each slice separately. This study develops an approach for 3D real-time bSSFP cine imaging using self-supervised deep learning, with feasibility in healthy subjects demonstrated at <60ms and <40ms temporal resolution per volume at 0.55T and 1.5T, respectively.

Methods

Acquisition: Data were acquired using 3D stack-of-spirals sampling with 48 interleaves.1 The 3D k-space was filled by collecting all partitions before rotating the spiral by the golden angle (Figure 1a).2 Interleaved R=2 undersampling was applied along the partition direction, and each volume was reconstructed using only one interleaf and all acquired partitions, resulting in a net acceleration of R=96.

Reconstruction: A Time-and-Partition Dependent Deep Image Prior (DIP) reconstruction was developed that extends the Time-Dependent DIP by Yoo et al. for 2D dynamic imaging.3,4 A convolutional neural network (CNN) was used to generate time-resolved 3D images without ground truth training data. To improve efficiency, 2D (rather than 3D) convolutions were used by parameterizing the time index i and partition index j on a low-dimensional manifold (Figure 1b). A point on the manifold was input to the CNN to generate a 2D image; this was repeated for all time frames and partitions to obtain time-resolved 3D images. The manifold consisted of Fourier basis functions as follows, with lower-frequency sinusoids favoring smooth changes and higher-frequency sinusoids recovering rapid motion, with $$$N_t$$$ time frames and $$$N_z$$$ partitions.
$$z_i = [sin(\pi i/N_t), cos(\pi i/N_t),sin(2\pi i/N_t),cos(2\pi i/N_t),...,sin(L_t\pi i/N_t),cos(L_t\pi i/N_t)]$$ $$z_j=[sin(\pi j/N_z), cos(\pi j/N_z),sin(2\pi j/N_z),cos(2\pi j/N_z),...,sin(L_z\pi j/N_z),cos(L_z\pi j/N_z)]$$
$$$L_t$$$ and $$$L_z$$$ determined the highest frequency sinusoids and were set using $$$L_t=\lfloor log_2(N_t) \rfloor=8$$$ and $$$L_z=\lfloor log_2(N_z) \rfloor=4$$$. The final manifold sample $$$z_{ij}$$$ was obtained by concatenating $$$z_i$$$ and $$$z_j$$$. Training (Figure 1c) was performed in mini-batches of one 3D volume by calculating the forward encoding model, including coil sensitivities and gridding.5 The MSE loss was computed with respect to acquired k-space data to optimize the CNN weights. Training was performed de novo after each scan for 500 epochs and required 26 hours on a GPU.

Experiments: Short-axis cardiac data were collected in five healthy subjects at 1.5T (MAGNETOM Sola, Siemens Healthineers, Erlangen, Germany). Real-time 3D spiral data were obtained with 16 partitions, 300x300mm2 FOV, 2.2x2.2x8.0mm3, and TR/TE=4.5/1.4ms. 288 time-resolved 3D images were collected over 10.4s at a temporal resolution of 36ms per volume. Additionally, real-time 2D spiral data were collected using a Time-Dependent DIP4 reconstruction (34ms/frame, R=6). A 2D breathheld ECG-gated Cartesian cine scan with 25 phases was acquired for reference. LVEF values were compared using Bland-Altman6 plots after manual contouring. To demonstrate translatability on a commercial low-field system, two subjects were scanned at 0.55T (MAGNETOM Free.Max), where lower gradient performance resulted in temporal resolutions of 50ms for 2D and 58ms (per volume) for 3D real-time scans.

Results

Figures 2 and 3 show 2D and 3D real-time images from the same subject at 1.5T. Respiratory and cardiac motion are synchronized over all partitions for the 3D scan, enabling evaluation of motion over the entire LV, unlike the 2D scan, where each slice is imaged at a different point in time. Bland-Altman plots in Figure 4 compare LVEF from 2D and 3D real-time methods with the 2D reference scan. The mean bias and 95% limits of agreement were -0.9% (-8.2%, 6.4%) for 3D real-time vs the 2D reference. Figure 5 presents 2D and 3D real-time images from one subject acquired at 0.55T.

Discussion

The study demonstrates the feasibility of 3D real-time functional cardiac imaging by combining a highly undersampled stack-of-spirals trajectory with a deep image prior. This technique may enable streamlined exams, as whole-heart 3D cine images could be obtained without breathholds or gating in a 10-second scan. This technique may simplify volume and EF measurements since motion can be evaluated synchronously over the entire heart. Future studies will explore whether real-time 3D imaging can improve LVEF reproducibility over 2D real-time techniques, where changes in slice positions during free-breathing may lead to differences in LVEF values. Initial results at 0.55T suggest this technique could be deployed on low-field scanners, potentially improving access to cardiac MRI in lower-resource settings. Future work will include validation in additional subjects, including patients with arrhythmias.

Acknowledgements

Siemens Healthineers; NIH/NHLBI R01HL163030, R01HL153034, and R01HL163991

References

1. Hargreaves B. Variable-Density Spiral Design Functions. 2005. http://mrsrl.stanford.edu/~brian/vdspiral/.
2. Winkelmann S, Schaeffter T, Koehler T, Eggers H, Doessel O. An optimal radial profile order based on the Golden Ratio for time-resolved MRI. IEEE Trans Med Imaging. 2007;26(1):68-76. doi:10.1109/TMI.2006.885337.
3. Ulyanov D, Vedaldi A, Lempitsky V. Deep Image Prior. In: Proceedings of the IEEE Computer Society Conference on Computer Vision and Pattern Recognition. IEEE Computer Society; 2018:9446-9454.
4. Yoo J, Jin KH, Gupta H, Yerly J, Stuber M, Unser M. Time-Dependent Deep Image Prior for Dynamic MRI. IEEE Trans Med Imaging. 2021;40(12):3337-3348. doi:10.1109/TMI.2021.3084288
5. Fessler J, Sutton B. Nonuniform fast Fourier transforms using min-max interpolation. IEEE Trans Signal Process. 2003;51(2):560-574.
6. Bland JM, Altman DG. Statistical methods for assessing agreement between two methods of clinical measurement. Lancet Lond Engl. 1986;1(8476):307-310.

Figures

Figure 1: (A) Data are acquired using a stack-of-spirals trajectory with interleaved R=2 partition undersampling. One volume is reconstructed from 1 (out of 48) spiral arms and all acquired partitions. (B) Time and partition indices are parameterized on a low-dimensional manifold, which is sampled and input to a 2D CNN to generate an image. This process is repeated for all partitions and time frames to generate time-resolved 3D images. (C) The CNN is trained by favoring consistency between generated images and acquired k-space data using the forward MRI encoding model.

Figure 2: Free-breathing ungated 2D spiral multislice bSSFP images acquired in a healthy subject at 1.5T and reconstructed using a time-dependent deep image prior. Note the asynchronous motion between slices due to the sequential acquisition of each slice. Relevant imaging parameters include 2.2 x 2.2 mm2 spatial resolution, 8 mm slice thickness, 300 x 300 mm2 FOV, and 34 ms temporal resolution (R=6, 8 out of 48 spiral interleaves per frame).

Figure 3: Free-breathing ungated 3D spiral bSSFP images acquired in a healthy subject at 1.5T and reconstructed using a time- and partition-dependent deep image prior. Unlike the 2D multislice real-time images, respiratory and cardiac motion are synchronized over all partitions as the entire 3D volume is acquired every time frame. Relevant imaging parameters include 2.2 x 2.2 x 8.0 mm3 spatial resolution, 300 x 300 mm2 FOV, 36 ms temporal resolution per volume, R=48 in-plane (one interleaf) and R=2 through-plane (8 acquired partitions) for a total acceleration factor of R=96.

Figure 4: Bland-Altman plots comparing LVEF measurements at 1.5T between a 2D breathheld and ECG-triggered Cartesian cine scan and (A) 3D spiral real-time images reconstructed using a time- and partition-dependent deep image prior, and (B) 2D spiral real-time images reconstructed using a time-dependent deep image prior. The solid red line indicates the mean bias. The dotted red lines indicate the 95% upper and lower limits of agreement.

Figure 5: Spiral bSSFP images from one subject at 0.55T are shown using (A) 2D real-time imaging at a temporal resolution of 50ms using a time-dependent deep image prior reconstruction, and (B) 3D real-time imaging at a temporal resolution of 58ms per volume with a time- and partition-dependent deep image prior reconstruction.

Proc. Intl. Soc. Mag. Reson. Med. 32 (2024)
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DOI: https://doi.org/10.58530/2024/1372