Parallel imaging is an MRI acceleration method that uses the spatial sensitivity of multi-channel receiver coils to undersample k-space and reconstruct full–field-of-view images, thereby shortening acquisition time without changing contrast weighting. It achieves this by reducing phase-encoding steps by an acceleration factor RRR and resolving the resultant aliasing using coil sensitivity information in the image domain (SENSE-type) or k-space interpolation (GRAPPA-type) during reconstruction.
Parallel imaging leverages independently digitized signals from multiple receiver coil elements with distinct spatial sensitivity profiles to provide additional localization information beyond conventional phase encoding. By exploiting these sensitivities, fewer phase-encoding lines are acquired, decreasing scan time proportionally to the acceleration factor RRR within SNR and geometry constraints.
| Aspect | SENSE (image-domain) | GRAPPA/SMASH/SPIRiT (k-space) |
|---|---|---|
| Core idea | Unfold aliased images using explicit coil sensitivity maps | Synthesize missing k-space lines using calibrated convolutional kernels across coils |
| Calibration | Requires accurate coil sensitivity estimation; separate reference or self-calibrated variants exist | Uses ACS lines; does not require explicit sensitivity maps |
| Pros | Direct control via regularization; efficient when maps are accurate | Robust to map errors; widely used in EPI and routine sequences |
| Cons | Sensitive to map errors and motion; FOV must match encoding | Kernel miscalibration can cause residual artifacts; ACS costs time |
Parallel imaging incurs an SNR penalty approximated by
$$ SNRR≈SNR0/(R g)\mathrm{SNR}_R \approx \mathrm{SNR}_0 / \big(\sqrt{R}\, g\big)SNRR≈SNR0/(Rg), $$
where ggg is the geometry factor describing noise amplification from coil geometry and conditioning of the reconstruction. Coil configuration, acceleration direction(s), and ACS quality strongly affect ggg and thus practical acceleration limits, with typical routine RRR values of 2–3 in 1D and modest 2D accelerations when coil coverage is favorable