Srikant Kamesh Iyer1, Brianna Moon2, Rishab Kumar3, and Walter R.T Witschey1
1Radiology, University of Pennsylvania, Philadelphia, PA, United States, 2Bioengineering, University of Pennsylvania, Philadelphia, PA, United States, 3Biochemistry and Molecular Biophysics, University of Pennsylvania, Philadelphia, PA, United States
Synopsis
This abstract presents a novel data driven
approach for high quality QSM reconstructions without the use of complex and
computationally intensive reconstruction models. The purpose of this approach
is to develop a reconstruction technique which does not depend on the use of
spatial priors from the magnitude image to remove artifacts and reduce blurring
of edges. In our proposed formulation, the data fidelity term is updated based
on the deviation of the estimated susceptibility map from the measured local
field. With the proposed fidelity-loss adaptive reconstruction formulation, removal
of artifacts was achieved without causing smoothing of sharp features.
Introduction
Quantitative susceptibility mapping (QSM) is a technique that can
quantify tissue magnetic properties and provide valuable information about
hemorrhagic stroke [1,2] and impaired tissue oxygen consumption [2]. Reconstruction
of magnetic susceptibility maps from the tissue field is a challenging
ill-posed inverse problem. Most popular techniques use a combination of
weighted least squares fidelity constraint and regularization constraints such
as total variation (TV) [3] or total generalized variation (TGV) [4,5]. An exponential data fidelity
model is sometimes used to further improve the quality of the reconstruction.
This leads to slow and computationally complex reconstruction models. The
purpose of this work was to develop a data driven QSM reconstruction algorithm
that can faithfully reconstruct fine features and maintain sharp edges. The
proposed Loss Adaptive Dipole Inversion (LADI) technique is a novel application
of the constrained TV formulation that does not need to estimate the location
of edges in the susceptibility maps or the nonuniform distribution of noise in
the phase data. The advantage of this technique compared to algorithms that use
a priori edge information is that our algorithm is unaffected by mismatch
between the edge prior and estimated susceptibility map. We compare the
performance of LADI to several CS based algorithms in for applications such as
neuroimaging and hemorrhagic myocardial infarction.Methods
The constrained reconstruction formulation
that we aim to minimize is $$_{min\chi}||\triangledown\chi||_{1}; S.T. ||M_{Bin}(F^H DFχ-ϕ)||^{2}\leq \sigma^{2}$$(1).
Here MBin
is a binary mask, D is the magnetic
dipole kernel represented in the frequency domain, χ is the susceptibility distribution, F is the Fourier operator, FH
the inverse Fourier operator, ϕ is
the tissue phase and σ is the noise
standard deviation. By using the Bregman iterations [6], Eq. (1) can be reduced
to $$_{min\chi}\lambda||\triangledown\chi||_{1}+\frac{\mu}{2} ||M_{Bin}(F^H DFχ-ϕ)||^{2}$$ and $$\phi^{k+1}=\phi^{k}+(ϕ-F^H DFχ^{k})$$The iterative update
of ϕ is equivalent to the
“adding-noise-back” step [6], which helps ensure better data fidelity to the
measured local tissue field, while preventing smoothing of edges and fine
features in the image due to data regularization. We compare the results from LADI
to thresholded k-space division (TKD) [3], closed form L2 [3], morphology enabled dipole inversion (MEDI) [4,7] and a rapid
implementation of non-linear MEDI with TGV constraints (FANSI) [4]. COSMOS
phantom [5] and cardiac QSM data acquired in a large animal model of
hemorrhagic myocardial infarction was used to compare the reconstructions. Visual
inspection of images for presence of artifacts, metrics such as RMSE [5], SSIM
[5], HFEN [5], mutual information [4] and quantification of mean
susceptibilities from ROI’s were used for to compare the different
reconstructions.
Results
A comparison of the reconstructions from COSMOS
phantom are shown in Fig (1). TKD reconstructions suffered from large streaking
artifacts (SSIM=0.75,RMSE=73.1,HFEN=66.7) while in closed form L2
reconstructions, removal of artifacts was achieved at the cost of smoothing of
edges (SSIM=0.81,RMSE=70.1,HFEN=68.3). FANSI and LADI had
slightly better performance with respect to global error quality metrics(Table I); though
sharp features such as veins were better preserved in LADI (location shown by arrow
in Fig 1). Overall, LADI (corr coeff=0.81) and FANSI (corr coeff=0.79) performed
better at matching COSMOS (corr coeff=0.77). ROI based comparison from five
different regions in the brain (Table II) showed that FANSI and LADI were able
to match COSMOS better than MEDI reconstructions. A comparison of the reconstructions
from the hemorrhagic myocardial infarction data is shown in Fig 2. LADI and
FANSI reconstructions had a good balance of feature preservation and artifacts
removal, and the dark artifacts seen in MEDI, TKD and closed form L2 was well
mitigated. Discussion
The proposed LADI technique does not need to estimate the location of
edges in the susceptibility maps or the nonuniform distribution of noise in the
phase data. The major advantage of LADI algorithm compared to algorithms that
use a priori edge information is that our algorithm is unaffected by mismatch
between the edge prior and estimated susceptibility map. Hence blurring of
edges that could occur in existing MEDI and non-linear MEDI based formulation is
avoided. The results from the COSMOS phantom and the cardiac QSM data showed
that the proposed model is robust to variations in data quality. LADI formulation
can be easily accelerated by incorporating the Split Bregman based variable
substitution techniques in [3,4].Conclusion
We developed a data driven approach for high quality QSM
reconstructions. LADI had better image quality metrics compared to MEDI and
performed as well as FANSI-TGV, one of the current state-of-the-art
reconstruction models. Ease of implementation, high image quality and robustness
to different data types are the important features of the proposed LADI
technique.Acknowledgements
This work is
supported by R00-HL108157, McCabe Foundation, and W.W. Smith Foundation.References
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