Matthias Serger1, Philipp Ehses1, Thomas Ulrich2, Malte Riedel2, Ruediger Stirnberg1, Nicolas Boulant3, Klaas Pruessmann2, and Tony Stoecker1,4
1German Center for Neurodegenerative Diseases (DZNE), Bonn, Germany, 2Institute for Biomedical Engineering, ETH Zurich and University of Zurich, Zurich, Switzerland, 3Commissariat à l’Energie Atomique, CNRS, NeuroSpin, BAOBAB, Université Paris-Saclay, Gif sur Yvette, France, 4Department of Physics and Astronomy, University of Bonn, Bonn, Germany
Synopsis
Keywords: Motion Correction, Motion Correction
Motivation: The quality of susceptibility weighted images may deteriorate under subject motion, especially at high fields, impairing further data analysis.
Goal(s): To mitigate motion artifacts through prospective motion correction(PMC) by employing 3D orbital navigators and real-time processing of a linear perturbation model.
Approach: Orbital navigators were integrated into a high-resolution 3D EPI sequence for rapid susceptibility-weighted imaging at 7T, and a real-time motion estimation pipeline was established. The impact of prospective correction for large instructed motion on the resulting images was investigated.
Results: Prospective motion correction successfully preserved the image quality of susceptibility weighted images, yielding results comparable to a scan without instructed motion.
Impact: The improvements in image quality
of the susceptibility weighted images underline the high potential
of a linear perturbation model with Orbital Navigators for precise and rapid
prospective motion correction in ultra-high field gradient echo imaging and
potentially many more applications.
Introduction
Head motion is a major challenge for susceptibility
weighted imaging (SWI) at high fields. When aiming for high resolutions, even
small involuntary motions can degrade image quality – particularly at long TE
optimal for SWI – and impede further analysis. Orbital Navigators (Onavs) with
a linear perturbation model have been shown to be a promising prospective
motion correction (PMC) method for highly precise and rapid geometry updates
with minimal calibration[1]. Here, Onavs have been integrated into a high-resolution
3D-EPI gradient echo sequence. Although such fast acquisitions reduce the impact
of intra-scan motion, images can still suffer due to the multi-shot acquisition,
especially if large or sudden movements occur during scanning. This work
demonstrates the benefit of the Onavs PMC method for SWI.Methods
A navigator trajectory[1,2] (k-space radius = 400
rad/m, TA = 2.3 ms) was integrated into a segmented whole-brain 3D-EPI [3] (0.6 mm3, FOV = 240 x 240 x 156 mm, 2
volumes, TR-shot = 40 ms, TAvol = 52s, 2x2z1 skipped-CAIPI
with segmentation factor 10, EPI factor = 20, TE = 22 ms) right after the water-selective
excitation pulse. A short pre-scan consisting of a reference navigator and
three rotated navigators was acquired to calibrate a linear perturbation model[1].
Due to the limited linearity of this model for large motions, the navigator
predictions were used to update its gradients and demodulation frequency to
stay in the frame of reference during prospective motion correction[2]. The
navigator data was sent in real-time to a server, which was used for processing
the data in order to calibrate the model first (~ 60 ms) and subsequently sent
motion updates to the scanner. The scan geometry was updated in real-time[4]
before every EPI shot and the processing on the server was fast enough (~ 3 ms)
to apply motion updates in every shot.
One healthy subject was scanned at a MAGNETOM 7T Plus
scanner (Siemens Healthineers, Erlangen, Germany) equipped with a 32 channel Rx
(1Tx) head coil (Nova Medical Inc, Wilmington,
Delaware). The subject was instructed to keep the head still during the
first volume acquisition and to move the head slightly at a certain time in the
subsequent volume acquisition (approximately during k-space center
acquisition). This experiment was repeated with and without PMC. For a rough
estimation of the noise standard deviation of the motion parameters, the volume
with small involuntary motions was high-pass filtered (5 Hz).
For each case, SWIs were calculated from the online
reconstructed magnitude and phase images using the CLEAR-SWI method[5].
Subsequently, minimum intensity projections (MIP) across 12 sagittal slices
(7.2mm) were computed.Results
Fig. 1 compares the prospectively corrected magnitude
images to its uncorrected counterparts without (top) and with (bottom)
instructed motion. The image quality is not degraded by PMC when the subject
holds still. However, it significantly improves for the motion case. Fig. 2
shows motion trajectories for the corrected and uncorrected scan, demonstrating
that the instructed motion was similar in both scans. The motion parameter noise
was in the order of 18 mdeg and 50 µm. Figure 3 shows the frequency spectrum of
the motion parameters. The peaks appear at 2.5 Hz and at higher harmonics for all
motion parameters.
Fig. 4 shows axial views of the SWIs and the derived MIPs
for all cases. The two times magnified views highlight particularly strong
motion artifacts and their mitigation by PMC.Discussion and Conclusion
The reduction in motion artifacts in both magnitude and
SWI images underlines that employing 3D Orbital Navigators with a linear
perturbation model is an appropriate motion correction method for
high-resolution EPI. Although the navigator was not updated during the
uncorrected scan, motion parameters between both experiments show high similarity,
indicating that the linear range of the model was not exceeded. The precision
in the motion updates is reduced by apparent noise that is, however, not purely
random but seems to be dominated by eddy currents (repeating with the in-plane
segmentation factor every 400ms). Such eddy currents can be corrected for in
the future to achieve single-digit µm precision, as previously reported for
this method[2]. Since Onavs have also proven to be capable of measuring and
correcting B0 fields up to the 1st order[6], image quality could be further
increased by implementing dynamic shimming which would be especially useful in
SWI applications and other long TE scans. In conclusion, this work demonstrates
the benefit of PMC with an Onav-based linear perturbation model for SWI
applications. Acknowledgements
This work received financial support from the European
Union Horizon 2020 Research and Innovation program under grant agreement 885876
(AROMA).References
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