Thara Nallamothu1,2, Haben Berhane1,2, Liliana Ma1, Justin Baraboo1,2, Daniel C. Lee3, Daniel Kim1, Phillip Greenland4, Michael Markl1,2, Rod Passman3, and Mohammed S.M. Elbaz1
1Radiology, Northwestern University, Chicago, IL, United States, 2Biomedical Engineering, Northwestern University, Chicago, IL, United States, 3Medicine (Cardiology), Northwestern University, Chicago, IL, United States, 4Preventative Medicine, Northwestern University, Chicago, IL, United States
Synopsis
Eddy
current corrections are essential in preprocessing 4D flow data due to
differing offset errors in each flow component leading to spatiotemporal inaccuracies
in the velocity vector-field. Current automated optimization methods may
require training data, have limited generalizability to different scan
protocols, are sensitive to wraparound errors, and do not account for complex spatiotemporal
errors. We introduce a self-calibrating method to optimize eddy current corrections
and detect wraparound errors by using our recent 4D flow-field disparity signature
technique that stochastically encodes the entire spatiotemporal profile of paired
vector disparities and show feasibility and generalizability to two different
4D flow protocols.
Introduction
Eddy
current offset correction is an essential step in preprocessing 4D flow data for
accurate flow quantification. Differing offset errors in each velocity encoding
direction induce disparate spatiotemporal inaccuracies in the 4D flow velocity
vector-field components. Limitations of available eddy current correction
methods include 1) manual methods can be time-consuming and observer-dependent;
2) automated methods (e.g., deep learning) may require large training data and
have limited generalizability to different scan protocols; 3) independent
optimization of each velocity component and time step does not fully account
for complex spatiotemporal errors 4) sensitivity to FOV wraparound errors. To
address these limitations, we propose a semi-automated self-calibrating method
(no training data) to simultaneously optimize eddy current corrections and
detect wraparound errors. The proposed method uses a recently developed 4D
flow-field disparity signature technique1,2 as a spatiotemporal vector-field
optimization metric. The signature technique stochastically encodes the profile
of pairwise vector disparity of the entire 3-directional velocity field. We
hypothesize that disparate spatiotemporal eddy current errors over the velocity
directions result in altered flow-field disparity signatures that would further
diverge in case of wraparound errors. In this study, we aimed to show the method’s
feasibility and generalizability to two different 4D flow protocols (CS and
GRAPPA). Methods
Our IRB-approved
study included 98 subjects: 64 atrial fibrillation patients scanned using a
PEAK-GRAPPA 4D flow protocol in a sagittal orientation (Non-CS) and 34 healthy
volunteers scanned using a compressed sensing (CS) 4D flow protocol in a
coronal orientation (Table 1).
Eddy current
correction: Static
tissue regions over all the slices were defined as voxels with temporal standard
deviation below a static tissue threshold ($$$\tau$$$). A 3D linear regression correction
was applied according to [3].
Optimization
of eddy current correction using 4D flow-field disparity signature
technique: A rough 2D
ROI containing flow was manually selected and propagated over all slices and
time frames (Fig. 1). The 4D flow-field disparity signature was computed as a
probability density function of ~30 million pairwise angular disparities (Θ)
over the spatiotemporal ROI1,2 (Fig. 1). The eddy
current correction and resulting signature were iteratively computed with
increasing $$$\tau$$$ with step size of 0.001. Root mean square error (RMSE)
was computed between successive signatures. Criteria for signature convergence to
optimal threshold $$$\tau_{auto}$$$ were RMSE<1% for 10 successive
iterations.
Wraparound
error detection:
Presence of wraparound artifact was defined as non-monotonic sequence of RMSE between
signatures prior to $$$\tau_{auto}$$$. Linear change point analysis4
was applied to the RMSE sequence. Non-monotonicity criteria were defined by the
presence of a segment with a positive slope or an increase in RMSE over 3
iterations (Fig. 2a).
Validation: Ground-truth for wraparound errors was
determined manually by a blinded visual inspection of 4D flow magnitude slices.
4D Flow Images were processed using
and
a manually optimized threshold $$$\tau_{manual}$$$. Manual corrections were computed within
FOV bounds that exclude regions with wraparound errors from static tissue.
In automated cases with successful
wraparound error detection, the computation was similarly bounded. One iteration of velocity anti-aliasing
was performed. Left atrial
(LA) Peak ($$$v_{peak-auto}$$$,
$$$v_{peak-manual}$$$) and
mean ($$$v_{mean-auto}$$$, $$$v_{mean-manual}$$$) velocities were computed over
the cardiac cycle and compared using Bland-Altman, coefficient of variation
(CoV), intraclass correlation (ICC).
Intra-observer
variability: To assess
sensitivity of the algorithm to the only manual input (choice of ROI, Fig. 1
step 2), the analysis of all cases was repeated using a newly defined ROI resulting
in a new automated threshold $$$\tau_{auto2}$$$. $$$v_{peak-auto}$$$ vs. $$$v_{peak-auto2}$$$
and $$$v_{mean-auto}$$$ vs. $$$v_{mean-auto2}$$$
agreement was tested between data corrected using $$$\tau_{auto}$$$ versus $$$\tau_{auto2}$$$. Results
Wraparound
error detection in the 34 CS cases, all of which were wraparound-free, had an
accuracy of 73.5%. Of the 64 Non-CS cases, accuracy was 75%, sensitivity was 74%
and specificity was 78.6% (Fig. 2b).
As summarized
in Figure 3, there was excellent agreement between $$$v_{peak-auto}$$$ and $$$v_{peak-manual}$$$ in wraparound
error and wraparound-free Non-CS cases and in wraparound-free CS cases. There
was similarly excellent agreement between($$$v_{mean-auto}$$$
and $$$v_{mean-manual}$$$.
Intra-observer variability
analysis of manual ROI selection, summarized in Figure 4, showed excellent
agreement between $$$v_{peak-auto}$$$
and $$$v_{peak-auto2}$$$
in both protocols, in cases with or without wraparound
error. There was similarly excellent agreement between $$$v_{mean-auto}$$$ and $$$v_{mean-auto2}$$$.Discussion and Conclusions
Using a recently
introduced 4D flow-field disparity signature to encode the entire
spatiotemporal three-directional velocity vector-field, we developed a
self-calibrating method for optimizing eddy current corrections and
simultaneously identifying wraparound errors. The results demonstrated
generalizability of the method, showing excellent agreement in LA peak and mean
velocity vs. the manually optimized, in two 4D Flow MRI protocols (CS, GRAPPA) with
different scan parameters as well as in the cases with identified wraparound
artifact. We found high LA
velocity agreement in most undetected wraparound cases, suggesting that smaller
wraparound region errors may have had minimal impact on the eddy current
correction in these cases.
In one error case with
severe deviation, the error was undetected, and the image may be uncorrectable.
LA velocity showed excellent agreement between values of the only manual input
(ROI selection). Future work will focus on automated adjustment of the
wraparound error region, as well as expanding to different eddy current correction
schemes and 4D flow scan protocols.Acknowledgements
This research is supported in part by the Transformational Project Award AHA 20TPA35490311 from the American Heart Association (AHA).References
[1] Elbaz M.S.M.,
Malaisrie C., McCarthy P., Markl M. (2021) Stochastic 4D Flow Vector-Field
Signatures: A New Approach for Comprehensive 4D Flow MRI Quantification. In: de
Bruijne M. et al. (eds) Medical Image Computing and Computer Assisted
Intervention – MICCAI 2021. MICCAI 2021. Lecture Notes in Computer Science, vol
12905. Springer, Cham. https://doi.org/10.1007/978-3-030-87240-3_21
[2] Nallamothu
T, DiCarlo A, Lee D, Kim D, Arora R, Markl M, Greenland P, Passman R and Elbaz
M. (2021) Novel Stochastic 4D Flow Signatures of time-resolved 3D left atrial
flow-field alterations in atrial fibrillation. In Proceedings: 29th Scientific
Meeting, International Society for Magnetic Resonance in Medicine (ISMRM).
2021.
[3] Walker, P. G.,
Cranney, G. B., Scheidegger, M. B., Waseleski, G., Pohost, G. M., &
Yoganathan, A. P. (1993). Semiautomated method for noise reduction and
background phase error correction in MR phase velocity data. Journal of
magnetic resonance imaging : JMRI, 3(3), 521–530.
[4] Killick, R.,
Fearnhead, P., Eckley, I.A. (2012) Optimal detection of changepoints with a
linear computational cost. Journal of the American Statistical Association. 107(500),
1590–1598.