Noam Omer1, Neta Stern1, Tamar Blumenfeld-Katzir1, Meirav Galun2, and Noam Ben-Eliezer1,3,4,5,6
1Department of Biomedical Engineering, Tel-Aviv University, Tel-Aviv, Israel, 2Department of Computer Science and Applied Mathematics, Weitzman institute of science, Rehovot, Israel, 3Department of Orthopedics, Shamir Medical Center, Zerifin, Israel, 4Sackler Faculty of Medicine, Tel-Aviv University, Tel-Aviv, Israel, 5Sagol School of Neuroscience, Tel-Aviv University, Tel-Aviv, Israel, 6Center for Advanced Imaging Innovation and Research (CAI2R), New-York University Langone Medical Center, New York, NY, United States
Synopsis
Multicomponent T2 analysis (mcT2)
yields a voxel-wise distribution of T2 values, which can be used to
estimate sub-voxel information such as myelin content. Producing such data,
however, remains challenging due to the large ambiguity in the T2 space.
We present a data-driven approach for mcT2 analysis, which learns the
anatomy in question and identifies microscopic tissue-specific features as a
preprocessing step. It then utilizes them for analyzing each voxel locally
using a designated optimization scheme. Experiments in human brain data show reproducible myelin content estimations at clinical settings
without any prior assumptions.
Introduction
Quantification of myelin content in the white matter (WM) is essential for
studying developmental processes and neurodegenerative diseases1-3.
Direct assessment of myelin, however, is highly impractical on clinical
MRI scanners due to the limit on achievable resolutions. This limitation is circumvented
by modeling WM T2-signals as a weighted average over three tissue compartments:
intra/extra-cellular water and myelin water4. This signal model can
cast into a linear matrix form: $$S=Ew+H\ \ \ \small(1)$$where $$$S$$$ is the experimental signal comprised of time-points, $$$E$$$ is a simulated dictionary
of single-T2 signals expected in the
tissue, $$$w$$$ is an unknown weights
vector representing the relative fractions of the
elements in $$$E$$$, and $$$H$$$ is an unknown noise vector. Such modeling
allows to match each signal with a
distribution of T2 relaxation times (T2-spectrum)
and use the obtained spectrum to quantify the myelin water fraction (MWF)
– a proxy of myelin content2,5-6. Notwithstanding its
advantages mcT2 analysis faces major challenges, leading to a lack of a gold standard technique7. The
key challenge, in this case, is the ambiguity, which arises due to the large
number of possible T2 combinations resulting in a highly ill-posed
problem8-10.
Recently, we introduced a new data-driven algorithm for mcT2
analysis. Assuming the existence of only
a finite number of microstructural compartmentations, the algorithm first applies statistical tests to identify a
series of global mcT2 features in the anatomy in question. It then
uses these to analyze voxel-specific signals using a designated optimization
scheme. Unlike spatially local approaches8,11, the statistical power
produced by this global approach endows the analysis with additional robustness,
which stabilizes the localized optimization scheme. Preliminary validations of
the algorithm’s accuracy were presented on two and three-compartment phantoms12. We
present here a complete version of the algorithm including validations on in vivo brain WM.Methods
mcT2 Algorithm
i. Generate a
broad mcT2
dictionary containing all possible combinations of multi-T2
distributions by superimposing sets of simulated single-T2
signals generated by the echo-modulation algorithm13,14.
ii. Calculate the statistical
correlation between dictionary elements ($$$d$$$) and experimental signals ($$$e$$$) in the anatomy in question ($$$\small\tt \color{navy} {Fig.1a}$$$). This provides
a pairwise score $$$Pr(d,e)$$$, which is normalized to
[0…1] ($$$\small\tt \color{navy} {Fig.1b}$$$) and
subsequently raised to the power of $$$\beta$$$ to prioritize mcT2 signals with
higher statistical correlation ($$$\small\tt \color{navy} {Fig.1c}$$$).
iii. Sum the scores of each dictionary
element across all voxels to form a global, element-specific,
probability score $$$Pr(d) $$$ ($$$\small\tt \color{navy} {Fig.1d}$$$).
iv. Identify the set of $$$L$$$ dictionary elements with highest scores and denote
them as $$$\widehat{E}$$$ ($$$\small\tt \color{navy} {Fig.1e}$$$). Then
substitute the term $$$Ew$$$ in Eq. (1) and express the signal as a weighted sum of mcT2 motifs. $$S= \widehat{E}\widehat{W}+H\ \ \ \small(2)$$ where $$$\widehat{W}$$$ is the unknown weights of each mcT2 motif in $$$\widehat{E}$$$.
v. Cast Eq. (2) as the following minimization problem:$$argmin_{\widehat{W}}(\phi)=\frac{1}{2}||\widehat{E}\widehat{W}-S||_2^2+\lambda_{Tik}|\widehat{W}||_2^2+\lambda_{L1}|\widehat{W}||_1\ \ \ \ s.t.\ \widehat{W}_i\geq0,\ \sum\widehat{W_i}=1\ \ \ \small(3)$$ Here $$$\lambda_{Tik}$$$ and $$$\lambda_{L1}$$$ are Tikhonov and L1 regularization weights. The inequality
constraints ensure that is non-negative and forces its sum to be unity, as expected in case
of T2 spectrum.
vi. Solve Eq. (3) using MATLAB’s quadratic programming optimizer (Mathworks, Natick, Massachusetts, USA).
MRI scans
In vivo brain scans were performed on a 3 Tesla whole body
MRI scanner (Prisma, Siemens Healthineers) using a 24-channel head coil. To
test reproducibility, three identical multi-echo spin-echo scans were performed
for the same subject, during one scan session. Experimental parameters were:
FOV=200x210 mm2, matrix
size=216x180, Naverages=1,
TR=3000 ms, TE=10, 20,...,200 (NTE’s=15), slice thickness=3 mm, acquisition-bandwidth=210 Hz/Px.
mcT2 analysis
Three WM segments were investigated: the
genu corpus callosum (GCC), splenium of corpus
callosum (SCC) and a cortical segment (CSEG). Segments data were analyzed with a mcT2
dictionary containing 64 elements, logarithmically spaced between 1-800 ms, and
fraction resolution of 0.05 for T2’s$$$\leq$$$40 ms and 0.1 for T2’s$$$>$$$40. Spatially global statistical analysis was done using $$$\beta$$$=104 and $$$L$$$=30 . Eq. (3) was solved using MATLAB’s solver with $$$\lambda_{Tik}$$$=10-2 and $$$\lambda_{L1}$$$=103. Mean and standard deviations (SD)
of MWF values (T2$$$\leq$$$40)2 were calculated, along with the geometric
mean of the remaining T2-spectrum (T2>40)15.Results
$$$\small\tt \color{navy} {Fig.2}$$$ presents MWF maps of the three WM segments. MWF values for the CSEG and SCC ranged between 8-13% and 10-16% respectively, while
the GCC values ranged between 5-14%. Segment specific mean and SD of MWF values
are delineated in $$$\small\tt \color{navy} {Table\ 1}$$$. These values
demonstrate a consistent range of MWF values with similar means and relatively
low SDs of 1.4% (GCC), 0.5% (SCC), and 1.0% (CSEG), across scans. The geometric
means and SDs were also consistent
between scans ($$$\small\tt \color{navy} {Table\ 1}$$$).Discussion & Conclusion
This study presents the first use
of global mcT2 analysis approach on clinical data. Our results
show that the proposed method can reproducibly probe MWF in the WM tissue at in
vivo scan settings and, thereby allowing to track
microscopic myelin-related processes. The results further demonstrate that learning
global tissue features prior to performing voxel-based mcT2 analysis
stabilizes the optimization scheme and efficiently overcomes the ambiguity in
the T2-space without the need to assume the number of sub-voxel tissue
compartments.Acknowledgements
ISF Grant 2009/17
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