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
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[2] Carlson J W, Minemura
T. Imaging time reduction
through multiple receiver
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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,
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Tesla, with 16-fold acceleration using partial parallel imaging with
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[10] Setsompop K, Gagoski BA, Polimeni
JR, Witzel T, Wedeen VJ, Wald LL. Blipped-controlled aliasing in parallel
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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.