2880

Optimized Density Compensation Function for Filtered Backprojection and Compressed Sensing Reconstruction in Radial k-space MRI
KyungPyo Hong1, Amanda L DiCarlo1, Aggelos K Katsaggelos1,2,3, Florian A Schiffers3, Cynthia K Rigsby1,4, Hassan Haji-Valizadeh5, and Daniel Kim1,6
1Radiology, Northwestern University Feinberg School of Medicine, Chicago, IL, United States, 2Electrical and Computer Engineering, Northwestern University, Evanston, IL, United States, 3Computer Science, Northwestern University, Evanston, IL, United States, 4Medical Imaging, Ann & Robert H. Lurie Children's Hospital of Chicago, Chicago, IL, United States, 5Internal Medicine, Cardiovascular Division, Beth Israel Deaconess Medical Center and Harvard Medical School, Boston, MA, United States, 6Biomedical Engineering, McCormick School of Engineering, Northwestern University, Evanston, IL, United States

Synopsis

While conventional density compensation function(DCF) performs sufficiently well for filtered backprojection(FBP) and radial k-space MRI when the Nyquist sampling condition is met and/or evenly-spaced view angles are used, it may perform poorly when sub-sampling and/or irrational-view angles are used. We propose an optimized DCF for the aforementioned conditions by calculating the density weights based on geometric properties of radial k-space sampling in a discrete environment, regardless of scan conditions such as data sizes and view angles. Compared with standard DCF, the optimized DCF produces higher signal-to-noise ratio(SNR) in FBP (phantom) and more accurate flow metrics in 48-fold accelerated, phase-contrast MRI.

Introduction

Density compensation function (DCF) is an essential component to account for non-uniform data sampling in filtered backprojection (FBP)1 and radial k-space MRI. The original DCF was analytically derived as a Jacobian determinant in an analog environment; it is an “invariant v-shaped” high-pass filter with zero at the center, which results in reduced signal-to-noise ratio(SNR) and increased streaking artifacts.2 A standard DCF performs sufficiently in a discrete environment when the Nyquist sampling condition is met and samples are evenly distributed. The standard DCF, however, may perform sub-optimally in highly-accelerated radial k-space MRI or when irrational-view angles are used. In this study, we sought to develop an optimized DCF based on geometric properties of radial k-space sampling in a discrete environment, regardless of scan conditions (e.g., sub-sampling factor, view angles), and evaluate its performance with FBP in phantom and compressed sensing(CS) reconstruction of 48-fold accelerated real-time phase-contrast(PC) MRI in patients with congenital heart disease(CHD).

Methods

Optimized DCF: While each radial spoke samples uniformly-spaced discrete data points along the radial direction, the spacing along the circumferential direction between neighboring discrete points varies with the radius in the polar coordinate system (Figure-1a). We propose a new concept that the spacing along both the circumferential and radial directions is uniform such that $$$arc\;length\:(\triangle{L})=r\triangle{\theta}=\triangle{r}=1$$$ (Figure-1b), which is also a minimal spacing to avoid overlaps between samples at a given radius. Using this concept as a criterion, we propose to calculate the degree of overlap between two neighboring samples at a given radius. Specifically, a DCF at $$$r$$$ of $$$i^{th}$$$ radial spoke (i.e., $$$DCF_{i}^{r}$$$) can be calculated to be inversely proportional to the sum of density weights ($$$c_{ij}^{r}$$$) between all neighboring points including itself, as described in Figure-1c.
Phantom Experiment for FBP: We scanned a T1MES phantom3 on a 1.5T MRI system (Aera,Siemens), using a gradient echo pulse sequence with radial k-space sampling with the following imaging parameters: field-of-view (FOV)=288x288 mm2, reconstruction matrix=192x192, slice thickness=8 mm, TE/TR=1.5/3.3 msec, receiver-bandwidth=1002 Hz/pixel, flip angle=15°, 600 radial spokes (i.e., full Nyquist condition), readout duration=2 sec, and dummy scan (2 sec). We separately acquired two data sets using regular-view angle=0.3° and tiny-golden-view angle=32.034°.4
In-vivo Experiment for CS: 48-fold accelerated, real-time PC data of 17 pediatric patients with CHD (10 males; mean age=11.3±3.2 years) were obtained from a previous study5 approved by our institutional review board. MRI scans included standard clinical 2D PC MRI with Cartesian k-space sampling (i.e., clinical PC) and real-time 2D PC MRI with radial k-space sampling (i.e., radial PC) at up to four locations (aortic valve, pulmonic valve, left-pulmonary artery, right-pulmonary artery; N=60 vascular planes in total). For the relevant imaging parameters of clinical PC, please see reference.5 The relevant imaging parameters for 48-fold accelerated, radial PC were: FOV=288x288 mm2, reconstruction matrix=192x192, in-plane resolution=1.5x1.5 mm2, slice thickness=6 mm, receiver-bandwidth=745 Hz/pixel, flip angle=12°, TE/TR=1.8/4.17 msec, prospective ECG-triggering, free-breathing scan time=3.34 sec (835-msec of dummy scan+2.50 sec) leading to 300 continuous radial spokes per plane, and golden-view angles=111.2461°.4 Velocity-encoding strength was matched to the clinical PC (150-400 cm/sec). For additional details, please see reference.5
Image Reconstruction: All image reconstructions were separately performed using GPU-based non-uniform fast Fourier transform (NUFFT)6 with standard and optimized DCF on a GPU workstation (Tesla V100, NVIDIA) equipped with MATLAB (R2020b,MathWorks). Auto-calibrated gradient delay correction was performed on all k-space data using the RING method.7 For the phantom data reconstruction, FBP was performed using multi-coil NUFFT. For the patient data reconstruction, we binned 300 radial spokes to achieve 4 radial spokes per frame (33.4-msec temporal resolution) and employed a radial CS framework8 using two orthogonal sparsity transforms of temporal total variation (TVt) and temporal principal component analysis (PCAt) with identical normalized regularization weight (α)=0.0075 (relative to the maximum signal), as shown in Figure 2.
Image Analysis: For phantom data, we measured SNR. For in-vivo data, we quantified the forward-flow volume, backward-flow volume, and peak-velocity per location by manually drawing regions-of-interest in Matlab. For radial PC, we analyzed the first full-heartbeat in all subjects.
Statistical Analysis: We conducted linear-regression and Bland-Altman analyses on forward-flow volume, backward-flow volume, and peak-velocity to assess the degree of association and agreement, respectively, between clinical and radial PC datasets. p<0.05 was considered statistically significant.

Results

Figure 3a compares the mean DCF of 600 radial spokes between standard vs. optimized DCF. As shown in Figure 3b, the resulting FBP images of the phantom using optimized DCF produced 11 to 18% higher SNR than standard DCF for both regular and irrational-view angles. Figure 4 shows representative magnitude (zero-filled NUFFT and CS reconstruction) and phase-difference images in a pulmonary-valve plane, and the corresponding plots of mean velocity. Radial PC with optimized DCF produced higher dynamic range of mean velocity (i.e., less temporal blurring) than that with standard DCF. As shown in Figure 5, compared with clinical PC as reference, the levels of association and agreement in forward-flow volume, backward-flow volume, and peak-velocity were better for optimized DCF than standard DCF.

Discussions

This study demonstrates that optimized DCF produces higher SNR in FBP(phantom) and more accurate peak-velocity, forward-flow volume, and backward-flow volume in 48-fold accelerated radial PC MRI. Future work includes extending the optimized DCF for 3D radial scans.

Acknowledgements

This work was supported in part by the following grants: National Institutes of Health (R01HL116895, R01HL138578, R21EB024315, R21AG055954, R01HL151079) and American Heart Association (19IPLOI34760317).

References

1. Shepp LA, Logan BF. The Fourier reconstruction of a head section. IEEE Transactions on Nuclear Science 1974;21(3):21-43.

2. Crawford CR. CT filtration aliasing artifacts. IEEE Trans Med Imaging 1991;10(1):99-102.

3. Captur G, Gatehouse P, Keenan KE, Heslinga FG, Bruehl R, Prothmann M, Graves MJ, Eames RJ, Torlasco C, Benedetti G, Donovan J, Ittermann B, Boubertakh R, Bathgate A, Royet C, Pang W, Nezafat R, Salerno M, Kellman P, Moon JC. A medical device-grade T1 and ECV phantom for global T1 mapping quality assurance-the T1 Mapping and ECV Standardization in cardiovascular magnetic resonance (T1MES) program. J Cardiovasc Magn Reson 2016;18(1):58.

4. 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.

5. Haji-Valizadeh H, Feng L, Ma LE, Shen D, Block KT, Robinson JD, Markl M, Rigsby CK, Kim D. Highly accelerated, real-time phase-contrast MRI using radial k-space sampling and GROG-GRASP reconstruction: a feasibility study in pediatric patients with congenital heart disease. NMR Biomed 2020;33(5):e4240.

6. Knoll F, Schwarzl A, Diwoky C, Sodickson DK. gpuNUFFT-an open source GPU library for 3D regridding with direct Matlab interface. In: Proceedings of the 22rd Annual Meeting of ISMRM, Melbourne, Australia 2014. Abstract No. 4297.

7. Rosenzweig S, Holme HCM, Uecker M. Simple auto-calibrated gradient delay estimation from few spokes using Radial Intersections (RING). Magn Reson Med 2019;81(3):1898-1906.

8. Feng L, Grimm R, Block KT, Chandarana H, Kim S, Xu J, Axel L, Sodickson DK, Otazo R. Golden-angle radial sparse parallel MRI: combination of compressed sensing, parallel imaging, and golden-angle radial sampling for fast and flexible dynamic volumetric MRI. Magn Reson Med 2014;72(3):707-717.

Figures

Figure 1. Illustration of optimized DCF. (a) General spacing along the circumferential direction in polar coordinate system. (b) Proposed concept of discrete spacing along the circumferential direction, which is also a minimal spacing to avoid overlaps between samples at a given radius. (c) Formula to calculate optimized DCF. $$$\triangle{L}=arc\;length$$$; $$$\triangle{r}=discrete\;length$$$; $$$\theta=azimuthal\;angle$$$.

Figure 2. A schematic flowchart of the image reconstruction pipeline. The adaptive phased array method was performed on the time average images to self-calculate the coil sensitivity maps, and 300 radial spokes were binned into 4 radial spokes per frame. Coil sensitivity maps, multi-coil NUFFT with DCF, binned k-space data, and zero-filled images were used as inputs to the iterative CS algorithm using two regularizations of TVt and PCAt (conjugate gradient with backtracking line search). Phase difference was calculated, followed by performing background phase correction.

Figure 3. FBP with standard and optimized DCF using 600 (full Nyquist) radial spokes in T1MES phantom. (a) Comparison of mean density weight profiles of regular view (=0.3°) and tiny golden view angles (=32.034°) between standard (black) and optimized DCF (blue=0.3°; red=32.034°). (b) The resulting FBP images of the phantom: optimized DCF produced 11 to 18% higher SNR than standard DCF for both regular and irrational view angles. SNR was calculated as mean signal at the central vial divided by standard deviation of noise at the top left background. SNR=signal-to-noise radio.

Figure 4. Representative magnitude (zero-filled NUFFT, top row; CS reconstruction, middle row) and phase difference (bottom row) images at systole and diastole reconstructed by radial PC with standard DCF (first and second column) and optimized DCF (third and fourth column). The corresponding mean velocity profiles on pulmonary valve were plotted in fifth column.

Figure 5. Linear regression (first and second columns) and Bland-Altman (third and fourth columns) plots of radial PC with standard DCF (first and third columns) and radial PC with optimized DCF (second and fourth columns) against clinical PC in forward-flow volume (top row), backward-flow volume (middle row), and peak-velocity (bottom row). In Bland-Altman plots, the upper and lower limit-of-agreement (dashed line) were calculated by mean difference ± (1.96 × standard deviation of mean difference). The difference was calculated by radial PC minus clinical PC.

Proc. Intl. Soc. Mag. Reson. Med. 29 (2021)
2880