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Multishot Dual Polarity GRAPPA: Robust Nyquist Ghost Correction for multishot EPI
This study introduces multishot dual-polarity GRAPPA (msDPG), a novel method for correcting Nyquist ghosts in multishot echo-planar imaging (EPI). msDPG significantly improves image fidelity, enabling high-resolution imaging on advanced MRI scanners.
Area of Science:
- Magnetic Resonance Imaging (MRI)
- Image Reconstruction
- Medical Physics
Background:
- Nyquist ghosts are artifacts in echo-planar imaging (EPI) that degrade image quality.
- Multishot EPI techniques are susceptible to these artifacts, especially on scanners with high-performance gradients or at ultra-high fields.
- Existing correction methods like linear phase correction (LPC) have limitations in addressing complex ghosting patterns.
Purpose of the Study:
- To develop a robust Nyquist ghost correction method specifically for multishot EPI.
- To address challenging ghosting artifacts encountered in advanced MRI systems.
- To enhance the fidelity and resolution of multishot EPI acquisitions.
Main Methods:
- Developed multishot dual-polarity GRAPPA (msDPG) by extending dual-polarity GRAPPA (DPG) to multishot readouts.
- Employed tailored DPG kernels to correct high-order phase differences not handled by LPC.
- Integrated advanced regularizers for physiologic inter-shot phase variation correction and proposed a calibration refinement method.
Main Results:
- msDPG demonstrated superior ghost correction compared to LPC, reducing the ghost-to-signal ratio (GSR) by over 50% in phantom and in vivo experiments.
- Achieved lower noise amplification than conventional DPG, particularly with large in-plane acceleration.
- Enabled high-fidelity, submillimeter diffusion imaging with regularized reconstruction.
Conclusions:
- The proposed msDPG method offers robust Nyquist ghost correction for multishot EPI.
- This technique facilitates high-fidelity submillimeter imaging, overcoming limitations of previous methods.
- msDPG is particularly effective on scanners with high-performance gradients and at ultra-high field strengths.
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