Qiang Yu1, David Reutens1, Javier Urriola1, Surabhi Sood1, and Viktor Vegh1
1Centre for Advanced Imaging, University of Queensland, Brisbane, Australia
Synopsis
Focal cortical dysplasias (FCD) are developmental malformations of the
cerebral cortex that are often highly epileptogenic. When medications fail to
control seizures, surgical removal of dysplastic epileptogenic tissue may be
curative. But, in 20-40% of patients current MRI scans cannot identify FCD
affected brain regions. Building on the anomalous nature of diffusion and magnetic
susceptibility of tissue, we aimed to improve in vivo identification of FCD in the brain. We found the combination of
anomalous diffusion model parameters and tissue magnetic susceptibility can be
used to differentiate FCD from healthy tissue in the brain.
Introduction
Focal cortical dysplasias (FCD) are developmental malformations of the
cerebral cortex that are often highly epileptogenic. They are characterised by
abnormal cortical architecture, with disruption of the normal organisation of
the cortex into well-defined layers and grey-white matter blurring.
Approximately 75% of patients with FCD develop epilepsy and surgical removal of
dysplastic epileptogenic tissue may be curative if medications fail to control
seizures.1 The ability to accurately detect and localise the
epileptogenic tissue to be resected is vital for surgical success. Patients
with clearly definable lesions on MRI have a 60-80% chance of seizure freedom
after surgery versus a 30-40% success rate for MRI-negative patients.2-5
However, visual analysis of conventional MRI scans is normal in 20-40% of FCD
patients.6 Hence, it is essential to develop MRI-based methods which
can delineate abnormal tissue in focal epilepsy patients with FCD. We aimed to
bridge this gap by exploiting the properties of anomalous diffusion and by
studying the magnetic susceptibility characteristics of tissues. Such an
approach has not been explored to date in focal epilepsy and FCD.Methods
Ethics was granted by the Royal Brisbane and
Women’s Hospital and the University of Queensland’s human research ethics
committees, Brisbane, Australia. Two consenting focal epilepsy patients were
recruited for the study. A 7 T Siemens whole body MRI research scanner (Siemens
Healthcare, Erlangen, Germany) was used to acquire data. Diffusion-weighted
data: bipolar planar diffusion imaging pulse sequence with 2 mm3 and 1.5 mm3 isotropic
resolution, seven b-values between 0 and 3,000 s/mm2 in steps of 500 s/mm2.
3D gradient recalled multiple-echo non-flow-compensated data: 0.75 mm3
isotropic resolution using 9 echo times starting from 4.98 ms and in steps of 3.13 ms.
Total scan time to acquire data was 45 minutes per participant, which included the
acquisition of standard clinical scans.
We opted to use the
fractional motion (FM) model as the parameters of this model have been
demonstrated to be sensitive to tissue microstructure variations.7 The
FM model describes the MRI signal in terms of the statistical properties of
water diffusion:
$$S(b)=S_0exp\left[-\eta Db^{\alpha/2}\left(\Delta-\frac{\delta}{3}\right)^{-\alpha/2}\Delta^{\alpha+\beta}\delta^{-\alpha}\right].$$
Here, $$$D$$$ is the anomalous diffusion coefficient, $$$\eta$$$ is a
dimensionless number required to maintain nominal unit for $$$D$$$ in
$$$\mu$$$m2/ms. The parameter $$$\alpha$$$ governs the variance of diffusion
increments and parameter $$$\beta$$$ measures the correlation properties of
increments. $$$\Delta$$$ is the time between the two pulses and $$$\delta$$$ is
the gradient duration. A nonlinear least squares algorithm
(Levenberg-Marquardt) in MATLAB® was used to solve for $$$D$$$,
$$$\alpha$$$ and $$$\beta$$$ by fitting the acquired data. Magnetic susceptibility
was calculated from gradient recalled multiple-echo non-flow-compensated data
using STI Suite V2.2.8 Brain regions shown in Figure 1 were
segmented using FreeSurfer.9 Figure 2 shows regions-of-interest(ROIs) located
in healthy and dysplastic grey matter used to assess changes in parameter $$$\alpha$$$ and
magnetic susceptibility.
Results
An example of a spatially resolved map of $$$\alpha$$$ and $$$\beta$$$
is shown in Figure 3. These parameters elucidate clear grey-white matter
contrast in the healthy human brain. Figure 4 shows that with increasing echo
time, $$$\alpha$$$ from the FM model and magnetic susceptibility of tissue are
able to differentiate FCD from normal brain and cortical grey matter regions (compare
average GM to average FCD) in our two participants. Figure 5 highlights that $$$\alpha$$$ is
smaller in all healthy grey matter ROIs (red markers) in comparison to the
dysplastic grey matter regions (blue markers) for the two patients.Discussion
Parameter $$$\alpha$$$ may be influenced by the magnetic susceptibility
of tissue,10 and the apparent magnetic susceptibility varies with
echo time.11 This suggests that magnetic environment and diffusion
signal formation are likely to be linked. Region-by-region analysis of the
brain cortex provides sufficient sensitivity to changes due to FCD, and
importantly, this approach eliminates the need to segment the brain into specific
regions.Conclusion
The combination of $$$\alpha$$$ from the FM model and tissue magnetic
susceptibility respectively mapped from diffusion-weighted and gradient
recalled echo MRI data appears to be spatially selective for dysplastic grey
matter brain regions. Such an approach of combining different modality MRI data
can lead to improved sensitive to microstructural variations and potentially be
used to distinguish small dysplastic cortical grey matter areas from healthy cortical
grey matter.Acknowledgements
Professor David Reutens and Dr Viktor Vegh acknowledge the Australian
Research Council for the award of a Discovery Project Grant (DP140103593). Aiman
AI Najjar and Nicole Atcheson from the Centre for Advanced Imaging, University
of Queensland, for helping with data acquisition.References
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