Parallel Imaging: How & Why It Moved So Quickly to Product
Rita G. Nunes1
1Instituto Superior Técnico, Universidade de Lisboa, Portugal

Synopsis

The aim of this talk is to introduce the basic concepts of Parallel Imaging and to discuss what made it such a successful technique. Parallel imaging took advantage of the availability of multichannel coil arrays to accelerate exams. It has had a major impact in MRI, quickly becoming available on standard scanners and being used in every day routine clinical practice.

Outcome/Objectives

To provide the context for the initial developments required for parallel imaging;
To explain the basic parallel imaging methods, their advantages, and pitfalls;
To provide practical examples of the impact of this technique.

Abstract

Although essential for Parallel Imaging, multi-channel array coils were initially introduced for other reasons. The main motivation for using them was to increase the signal-to-noise ratio (SNR) of the images. The use of small coil elements, closer to the region of interest and with a more localized coil sensitivity, enables measurement of the same signal whilst limiting the sample volume which contributes to the received noise. Having an array of small elements makes it possible to keep the spatial coverage of a larger coil with the SNR benefits of a small coil. In 1990, Roemer et al. demonstrated that a nearly-optimal SNR can be obtained by combining the individual coil images by using the sum-of-squares approach1; this approach had the advantage of not requiring calibration of the coil sensitivities.

A few years later, in 1993, it was suggested that coil encoding could partially replace gradient encoding allowing to speed up image acquisition at the cost of some SNR loss but at the time the demonstrations were limited to phantom experiments2. In 1997, Sodickson et al. presented the first in vivo demonstration with a compelling example of a cardiac imaging application3. This was a game-changer since shortening the image readout was essential to make single-shot cardiac imaging feasible and made the community realize that the potential benefits of parallel imaging could in some cases surpass the downside of an SNR penalty. Although the suggested reconstructed algorithm (SMASH) relied on being able to synthesize Fourier spatial harmonics through a linear combination of the coil sensitivities3, and for that reason, it is only compatible with very specific coil geometries (i.e. linear arrays), it paved the way for other approaches.

Soon afterward, an alternative formulation (SENSE) was introduced by Pruessmann et al. who realized that utilizing the image domain representation for both the coil sensitivities and the under-sampled data was a lot simpler and allowed for much more flexibility regarding coil requirements4. By using a Cartesian regular under-sampling strategy, it was possible to break the large reconstruction problem into the inversion of many small encoding matrices connecting the groups of aliased image pixels. SENSE became the method of choice, quickly becoming available as a commercial product that could be applied in clinical practice. SENSE enabled to shorten scan times for multi-shot sequences and had a large impact also on single-shot EPI, reducing the duration of the readout window and hence the level of geometric distortions in functional and diffusion MR images.

The SENSE formulation was later extended to allow for more general under-sampling schemes, including Non-Cartesian trajectories, where each pixel will be overlapped with many others5. The inversion of a much larger encoding matrix is then required but it can be carried out efficiently through iterative algorithms (e.g. conjugate gradients); this enables to make use of fast implementations of equivalent operators (e.g. fast Fourier transform), without explicitly having to build or invert the full encoding matrix.
A drawback of SENSE is that it requires explicit calibration of the coil sensitivity maps. Although it provides an optimal reconstruction when this is feasible, alternative methods have since been developed which do not present this limitation. GRAPPA6 is a k-space-based method that estimates a reconstruction kernel from fully-sampled calibration data. This method is also widely available and enables very fast reconstructions: the estimated kernel implicitly contains coil sensitivity information and can be applied to individual coil k-space data to populate missing k-space positions; after reconstructing the individual coil images, these are combined using Roemer’s1 sum-of-squares approach.

Parallel Imaging is now used on the majority of MRI acquisitions. The idea of using coil information to encode spatial position has since been applied to separate slices in simultaneous multi-slice (SMS) acquisitions7 and has also made it possible to accelerate single-shot EPI scans8, with a major impact in both functional9 and diffusion MRI10 studies.

Acknowledgements

Fundação para a Ciência e a Tecnologia (SFRH/BD/120006/2016, PTDC/EMD-EMD/29686/2017) and Programa Operacional Regional de Lisboa 2020 (LISBOA-01-0145-FEDER-029686).

References

[1] Roemer PB, Edelstein WA, Hayes CE, Souza SP, Mueller OM. The NMR phased array. Magn Reson Med. 1990; 16:192–225.

[2] Carlson J W, Minemura T. Imaging time reduction through multiple receiver coil data acquisition and image-reconstruction. Magn. Reson. Med. 1993; 29:681–8.

[3] Sodickson DK, Manning WJ. Simultaneous acquisition of spatial harmonics (SMASH): Fast imaging with radiofrequency coil arrays. Magn Reson Med. 1997; 38:591–603.

[4] Pruessmann KP, Weiger M, Scheidegger MB, Boesiger P. SENSE: Sensitivity encoding for fast MRI. Magn Reson Med. 1999; 42:952–962.

[5] Pruessmann KP, Weiger M, Börnert P, Boesiger P. Advances in sensitivity encoding with arbitrary k-space trajectories. Magn Reson Med. 2001; 46:638–651.

[6] Griswold MA, Jakob PM, Heidemann RM, Nittka M, Jellus V, Wang J, Kiefer B, Haase A. Generalized autocalibrating partially parallel acquisitions (GRAPPA). Magn Reson Med. 2002; 47:1202–1210.

[7] Larkman DJ, Hajnal JV, Herlihy AH, Coutts GA, Young IR, Ehnholm G., Use of multicoil arrays for separation of signal from multiple slices simultaneously excited, J Magn Reson Imaging. 2001; 13:313-7.

[8] Nunes RG, Hajnal JV, Golay X, Larkman DJ. Simultaneous slice excitation and reconstruction for single shot EPI. In: Proceedings of the 14th annual meeting of ISMRM, Seattle, Washington, USA, 2006. 293.

[9] Moeller S, Yacoub E, Olman CA, Auerbach E, Strupp J, Harel N, Ugurbil K. Multiband multislice GE-EPI at 7 Tesla, with 16-fold acceleration using partial parallel imaging with application to high spatial and temporal whole-brain fMRI. Magn Reson Med 2010; 63:1144–1153.

[10] Setsompop K, Gagoski BA, Polimeni JR, Witzel T, Wedeen VJ, Wald LL. Blipped-controlled aliasing in parallel imaging for simultaneous multislice echo planar imaging with reduced g-factor penalty. Magn Reson Med. 2012; 67:1210-24.

Further Reading:

[11] Larkman DJ, Nunes RG. Parallel magnetic resonance imaging. Phys Med Biol. 2007; 52:R15-55.

[12] Hamilton J, Franson D, Seiberlich N. Recent advances in parallel imaging for MRI. Prog Nucl Magn Reson Spectrosc. 2017; 101:71-95.

Proc. Intl. Soc. Mag. Reson. Med. 30 (2022)