Daniel Stäb1,2, Steffen Bollmann1, Christian Langkammer3, Kristian Bredies4, and Markus Barth1
1The Centre for Advanced Imaging, The University of Queensland, Brisbane, Australia, 2Department of Diagnostic and Interventional Radiology, University of Würzburg, Würzburg, Germany, 3Department of Neurology, Medical University of Graz, Graz, Austria, 4Institute for Mathematics and Scientific Computing, University of Graz, Graz, Austria
Synopsis
Ultra-high field whole brain
susceptibility mapping at an isotropic resolution of 1 mm was performed within
16 seconds using a 3D planes-on-a-paddlewheel (POP) EPI sequence. The
non-Cartesian readout scheme is created by rotating a standard EPI readout
train around its own phase encoding axis and provides higher flexibility for
echo time minimization than conventional 3D EPI. Morphologic images and
susceptibility maps obtained were comparable to those acquired with a
conventional 4 minute 3D GRE scan.Background
Quantitative
susceptibility mapping (QSM) provides novel insights into tissue composition
complementary to established contrasts and yields 10-fold-increased grey
matter/white matter contrast compared to magnitude imaging. As susceptibility
effects scale with the magnetic field QSM highly profits from scanning at
ultra-high field1.
Data are
conventionally acquired by Cartesian 3D spoiled gradient-echo (GRE) sequences. However,
high spatial resolutions come along with extensive measurement times, which can
be problematic in terms of head motion. Providing a significantly higher
sampling efficiency, Cartesian echo-planar-imaging (EPI) represents a fast
alternative to GRE but its application is limited by the gradient performance, geometric
distortions and signal dropouts.
The purpose of this
study was to perform QSM at 7T at an isotropic resolution of 1 mm. To achieve a
high sampling efficiency, minimize distortions and maximize the motion
robustness, we propose a non-Cartesian 3D EPI sequence with a
paddlewheel-shaped readout scheme2,3.
Methods
The planes-on-a-paddlewheel (POP)
trajectory is realized by rotating 2D EPI readout planes about the phase
encoding axis (Fig. 1a). Single planes on this paddlewheel are sampled at each
excitation, with the slab selection performed along the rotation axis.
The concept was evaluated in a healthy
volunteer (26, female). Measurements were performed on a 7 T whole body scanner
(Siemens Healthcare, Germany) with a gradient strength of 70 mT/m, slew rate of
200 mT/m/s and a 32 channel Tx/Rx head array (Nova Medical, USA). Images were
obtained at an isotropic resolution of 1 mm after 3rd order shimming
using the following acquisition parameters: FOV = 212 x 212 x 108 mm3,
330 projections, TR = 47 ms, TE = 24 ms, ES = 1.0 ms, flip angle = 13°, ramp
sampling, 10 measurements. A homogeneous azimuthal distribution of the planes
was achieved by employing an interleaved radial projection order (Fig. 1b). For
the correction of gradient delays and Nyquist ghosting three non-phase-encoded
navigator echoes were used. Parallel imaging with undersampling factor RPE
= 3 was applied along the phase encoding (PE) direction.
Post ramp sampling regridding, gradient delay
and Nyquist ghost correction was performed, and GRAPPA was employed to reconstruct
the missing phase encoding lines with the weight sets determined from a
separate 3-fold segmented full resolution reference scan. Gridding of the
non-Cartesian data was performed using the non-uniform fast Fourier transform
(NUFFT) software4.
For susceptibility mapping, a single-step QSM
method using total generalized variation5 (TGV) was employed for each coil channel phase
data individually. The brain mask for QSM was derived from the
root-sum-of-squares-combined magnitude data. Finally, QSM images were obtained
by calculating the mean of all channels. All QSM images were reconstructed using the same regularization
parameters for the TGV-QSM algorithm.
For comparison, conventional
imaging was performed using a 3D multi-echo GRE sequence with identical spatial
resolution (FOV = 212 x 212 x 120 mm3, TR = 29 ms, 7 echoes, TE1=
4.36 ms, ES = 2.86 ms, flip angle = 13°, GRAPPA with RPE = 3 and 16
additional calibration lines).
Results
The images obtained by the 3D
POP EPI sequence are free from reconstruction artifacts (Fig. 2a) and smaller anatomical
features of the brain can be delineated well. Both images and susceptibility
maps (Fig. 2b) are comparable to the corresponding 3D GRE data. As can be seen in
Fig. 2c, the image geometry is not significantly altered with respect to the 3D
GRE measurement.
The superimposed contours (red) were
calculated from the corresponding 3D GRE images after applying an affine
co-registration algorithm. No
deviations can be identified within the axial plane while slight distortions
are found along the phase encoding axis (arrows).
Figure 3 summarizes
susceptibility values obtained in three sub-cortical regions of interest. Mean
and standard deviation are not affected by the number of 3D POP EPI measurements
and are comparable to the values from 3D GRE.
Discussion
High resolution quantitative
susceptibility mapping was successfully performed at ultra-high field using 3D
POP EPI. With less than 16 seconds per volume, the proposed non-Cartesian
readout scheme is considerably faster than standard 3D multi-echo GRE imaging. The
radial nature of the readout is beneficial in terms of motion robustness and
provides high flexibility for further undersampling. Due to the smaller FOV in
the phase encoding direction and by employing parallel imaging with an
acceleration factor of R
PE = 3, low geometric distortions were achieved, also
in this most problematic dimension. The low variance of the susceptibility
values for multiple measurements indicates a high reproducibility of the
technique.
Acknowledgements
MB acknowledges funding from ARC Future Fellowship grant FT140100865.
The authors acknowledge the facilities of the National Imaging Facility at the
Centre for Advanced Imaging, University of Queensland.References
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