Maria Aristova1, Alireza Vali2, Alex Barker2, Ali Shaibani3, Sameer Ansari4, Matthew Potts5, Babak Jahromi5, Michael Hurley4, Susanne Schnell2, and Michael Markl2
1Biomedical Engineering, Northwestern University, Chicago, IL, United States, 2Radiology, Northwestern University, Chicago, IL, United States, 3Radiology, Neurosurgery, Northwestern University, Chicago, IL, United States, 4Neurointerventional radiology, Northwestern University, Chicago, IL, United States, 5Neurosurgery, Northwestern University, Chicago, IL, United States
Synopsis
To optimize dual-venc 4D Flow
MRI parameters for flow assessment in brain arteriovenous malformations, we
conducted an in-vitro optimization analysis and compared it to in-vivo data
from a patient with complex AVM. Using k-t acceleration factors of 2-5 and
about 2-10 voxels across the imaged vessels, we quantified the agreement with the
ground truth flow and geometry. We applied a flow distribution network graph
concept to characterize flow conservation as an additional quality metric. Data
indicated that approximately 5 voxels across imaged vessels are needed,
consistent with results from previous publications.
Introduction
Dual-venc 4D Flow MRI1 requires trade-offs
between spatial resolution, temporal resolution, field of view (FOV) and acceleration,
where optimal parameter combinations are highly application-dependent. Dual-venc 4D Flow MRI uses two
velocity encodings (low and high venc)
within one acquisition to achieve a large dynamic velocity range and velocity
to noise ratio. Hemodynamic
characterization of brain arteriovenous malformations (AVM) requires the large
dynamic velocity range and VNR of dual-venc, large FOV and high spatial
and temporal resolution, for accurate flow quantification in the main arteries and veins, which can be as small as 3mm. Previous work2 established minimum 4-5
voxels across a vessel for accurate quantification, but at 3T and with dual-venc, this guideline merits further exploration. We
applied kt-accelerated, dual-venc 4D
Flow in-vitro with known steady flow in a branched network of parallel flow
channels, and explored the parameter space of spatial resolution and k-t acceleration
factor to identify 4D Flow scan parameters enabling flow quantification within 10%
of ground truth, and internal flow conservation within 10%. In this context, we
present hemodynamic metrics and flow network analysis of a complex AVM.Methods
An in-vitro flow phantom contained flow along all spatial dimensions in
4, 6 and 8mm diameter channels (Fig.1). Water with 2mM gadolinium (Ernst angle3 =18°) circulated via a steady
flow pump (Micropump, USA) and was also used to fill the phantom shell as a static eddy
current correction reference. Total inlet flow was regulated via PID feedback
control implemented in LabView (National Instruments, USA) and a flow meter (OMEGA,
USA). The phantom was imaged at 3T (Skyra: Siemens, Germany) using dual-venc 4D Flow MRI with high-venc values set to avoid velocity aliasing (settings:
Fig.1B). Using in-house-developed software (Fig.2), data were corrected for phase
offset errors and noise. A phase-contrast angiogram was calculated and segmented.
~20 analysis planes/vessel segment were
used to obtain velocity profile, net flow and vessel diameter. Flow
distribution network graphs (FDNG: Fig.2) were constructed, tracking vessel
connectivity and flow conservation. For each spatial resolution and acceleration
factor combination, we computed net flow and diameter measurement error from
known values, static tissue velocity noise, and flow network mass conservation.
The methods were applied to a patient with complex bithalamic AVM (female-10yo:
Fig.1B), imaged at 1.5T (Aera: Siemens, Germany). Velocity noise and flow conservation
were characterized and a FDNG was extracted (Fig.2B).Results and Discussion
Results
indicate complex interactions between acceleration factor, spatial resolution
and number of voxels across the imaged vessel, which all impact the overall
image quality and quantification accuracy. Percent flow quantification error (Fig.3A)
depends on all these factors. For (1.2mm)3 resolution at all R, the error
is <10%, potentially balancing noise (more significant at higher resolution) and partial volume
effects (more significant at lower resolution). Scan conditions with <10% error have >5
voxels across each vessel at all R (Fig.4A), consistent with previous findings.
However, the resolution appears to dominate over the number of voxels across a vessel.
Evaluating the impact of this metric likely requires a more finely differentiated
scan parameter space.
Both
of the scans with >10% quantification error in vessel diameter measurement had
2.5 voxels across the vessel (6mm channel at (1.2mm)3 resolution, R=2 and R=3 respectively: Fig.3B and 4B). Velocity noise in static tissue (Fig.3C) was <5%
for all but one in-vitro measurement (R=3 and 5 voxels across the vessel), but ~8% in-vivo,
potentially due to less accurate static tissue identification in-vivo, patient motion, or lower field strength.
In
FDNG analysis of in-vitro scans of the entire branched phantom system (Fig.3D), flow conservation error
increases monotonically with decreasing spatial resolution. More accelerated
scans have higher mass conservation error, but less sensitivity to voxel size. Both
scans with <10% flow conservation error ((0.8mm)3 spatial
resolution, R=2 and R=3 respectively), have ≥5 voxels across each vessel, consistent with results of flow quantification accuracy. In-vivo data for flow conservation across the AVM (8.4% error) met the 10% flow conservation error benchmark
despite being collected at R=5; however, flow conservation error across the confluence of sinuses and whole brain was higher, suggesting a need for further exploration of these metrics in-vivo, particularly in the venous system.
Conclusions
Results suggest an optimal spatial resolution, (1.2mm)3 and a
minimal number of 5 voxels across the vessel to minimize noise and maximize
quantification accuracy and consistency. Broadly, in-vivo data aligns with
in-vitro results and indicates dual-venc
4D flow applications in AVM are feasible. However, more refined exploration of
this parameter space is needed. Future work will consider impact of temporal
resolution for pulsatile flow. Acknowledgements
We
gratefully acknowledge funding from the following sources: AHA Scientist
Development Grant 16SDG30420005, NIH K25HL119608 and NIH R01HL115828.References
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