Several successful iterative approaches have recently been proposed for parallel-imaging reconstructions of variable-density (VD) acquisitions, but they often induce substantial computational burden for non-Cartesian data. Here we propose a generalized variable-FOV PILS reconstruction 3D VD Cartesian and non-Cartesian data. The proposed method separates k-space into non-intersecting annuli based on sampling density, and sets the 3D reconstruction FOV for each annulus based on the respective sampling density. The variable-FOV method is compared against conventional gridding, PILS, and ESPIRiT reconstructions. Results indicate that the proposed method yields better artifact suppression compared to gridding and PILS, and improves noise conditioning relative to ESPIRiT, enabling fast and high-quality reconstructions of 3D datasets.
The proposed variable-FOV (var-FOV) method comprises three stages of processing for non-Cartesian data: individual-coil gridding reconstructions, frequency-dependent FOV restriction, and sensitivity-weighted coil combination. First, data from each coil are gridding reconstructed within the full FOV. Afterwards, the gridded image for each coil is filtered into N separate images, each corresponding to a different band of spatial frequencies in k-space. For example, for the 3D variable-density stack-of-spirals sampling trajectory in Figure 1, the kx-ky plane is divided into 2 annuli (inner and outer),and the kz direction is also divided into 2 annuli (central versus peripheral kz regions). When these divisions are considered together, they yield 4 non-overlapping bands of spatial frequency in k-space. The reconstruction FOV (FOVrecon) for each band is then restricted in accordance with the average sampling density within the band. In the final stage, coil sensitivities are estimated from the densely-sampled central part of k-space8. Based on these sensitivity estimates, coil-combination weights are then calculated separately for each frequency band, considering the varying FOVrecon. The individual-coil images are then linearly combined with these weights. The reconstructed image is: $$$P=\sum_{b=1}^F\sum_{i=1}^CK_{bi}W_{bi}$$$ , where $$$K_{bi}=S_{bi}M_{bi}$$$ and $$$W_{bi}=M_{bi}D_i^*/\surd{}(\sum_{i=1}^CM_{bi}{\left\vert{}D_i\right\vert{}}^2)$$$ . For frequency band b and coil i, Sbi denotes the initial image obtained via gridding-reconstruction, Mbi denotes the windowing function that restricts FOVrecon, and Wbi denotes the coil combination weight. Di represents the coil-sensitivity estimate for coil i obtained from central k-space data.
The var-FOV method was demonstrated on 3D GRE acquisition of the knee (0.5 mm isotropic) and a T1-weighted acquisition of the brain (1mm isotropic). The datasets were resampled on 3D stack-of-spirals trajectories of varying acceleration factors (R). FOVacq was designed to linearly decrease from 10 cm to (5, 3, 1) cm for the knee and 18 to (9, 4, 2) cm for the brain. The trajectories had R = (2.6, 3.2, 4.1) and (10,8,6) interleaves for the knee, and R = (2.5, 3.7, 4.2) and (12, 8, 7) interleaves for the brain. The reconstructed images have matrix size of (320x320x220) and (240x240x240), for knee and brain respectively. SOS reconstructions were obtained via sum-of-squares combination of gridding reconstructions within the full FOV. PILS reconstructions were obtained via a sum-of-squares combination after individual-coil reconstructions were restricted to FOVrecon supported by the highest sampling density in the trajectory. ESPIRiT reconstructions were obtained using a kernel size of [6, 6, 6], a Tykhonov parameter of 0.01 for sensitivity estimation, and an eigenvalue threshold of 0.001.
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