Stefano Casagranda1, Christos Papageorgakis1, Feriel Romdhane2, Eleni Firippi1, Timothé Boutelier1, Laura Mancini3,4, Moritz Zaiss5, Sotirios Bisdas3,4, and Dario Livio Longo2
1Department of Research & Innovation, Olea Medical, La Ciotat, France, 2Institute of Biostructures and Bioimaging (IBB), National Research Council of Italy (CNR), Torino, Italy, 3Lysholm Department of Neuroradiology,, University College of London Hospitals NHS Foundation Trust, London, United Kingdom, 4Institute of Neurology UCL, London, United Kingdom, 5Department of Neuroradiology, University Clinic Erlangen, Friedrich-Alexander Universität Erlangen-Nürnberg (FAU), Erlangen, Germany
Synopsis
This work
provides a new denoising methodology for multi-acquisition magnetic resonance images
(MRI) based on principal components analysis (PCA). We are proposing a new
principal component selection criterion that identifies spatial information in
the extracted component coefficients, leading to a better preservation of anatomical structures and
pathological information. In addition, our adaptive filtering step allows us to
further denoise the MRI data, rejecting persistent spatial noise from the
extracted component coefficients. In our investigations
the proposed method outperformed the eigenvalue based selection criteria on Amide
Proton Transfer weighted CEST data.
Introduction
Principal Component Analysis (PCA) is a non-parametric
technique originally designed to reduce the dimensionality of a given dataset,
while retaining the essence of the data1,2. It extracts a new set of variables,
called Principal Components (PCs) which are ordered based on the variability of
the original data each
component explains, i.e. their associated eigenvalues.
PCA has
been successfully used for denoising purposes in multi-acquisition MRI, usually
reconstructing the original dataset selecting the signal-related components and
rejecting noise-related components. For example, in3, three eigenvalues-based methods
are presented (Malinowski, Nelson and Median criteria) and thereafter
investigated for their applicability to denoising of in vivo Chemical Exchange Saturation Transfer (CEST) MRI data4.
Other methods exist5,6 but many rely on
the eigenvalues associated with the extracted principal components for the
selection of the signal-related components. However, such methods risk discarding anatomical structures
and pathological information hidden in the noise of the extracted components,
especially if those areas are small, as eigenvalues measures blindly the variance of
components regardless if it is noise or relevant clinical information.
A Z-Spectrum for a given voxel in the CEST data
can be expressed as:
$$\mathbf{Z_i}=\overline{z_{i}}+\sum_j\alpha_{ ij}\mathbf{v_j}$$
where $$$\overline{z_{i}}$$$ is the mean value of the Z-Spectrum, $$$\mathbf{v_j}$$$ is a principal component and $$$\alpha_{ ij}$$$ is the coefficient of $$$\mathbf{v_j}$$$ of voxel $$$i$$$.
Collecting all coefficients $$$\omega_{ij}$$$ of a component $$$j$$$ in the same
order of the Z-Spectra in the CEST acquisitions, we obtain the PC related image (or volume) of the $$$j^{th}$$$ component (see Figure1).
Methods
Technical Solution:
Our proposed method, called Component Analysis based on Standard-deviation Attenuation (CASA) criterion is based on the decrease of the variance of a PC related image after a smoothing
filter is applied on it, as detailed in the following steps (see Figure2):
1) PCA
is performed to obtain the PC
related images. The standard deviation of the
voxels of the full image or within a segmented region (for example excluding
background voxels) is computed for each of the $$$N$$$ PC related images to form the
vector $$$\sigma^a=[\sigma^a_{1},\sigma^a_{2},\sigma^a_{3},…\sigma^a_{N}]$$$. Then a Gaussian smoothing filter of a factor $$$\Sigma$$$ is applied to each component and standard deviation is recomputed on the
smoothed PC related
images to
obtain $$$\sigma^b=[\sigma^b_{1},\sigma^b_{2},\sigma^b_{3},…\sigma^b_{N}]$$$, where $$$\sigma^a_{i}>\sigma^b_{i}$$$. The rate of decrease of
standard deviation is then computed, for each component, as $$$\sigma^r =(\sigma^a -\sigma^b) / \sigma^a$$$,
where $$$0<\sigma^r_{i}<1$$$, $$$\forall i$$$. Components whose $$$\sigma^r_{i}$$$ rate is on the plateau of the curve are rejected (see Figure2).
2) Before the signal reconstruction a smoothing filter or denoising method can be applied on the retained PCs (PC related images). The strength of the applied filter is proportional to the amount of information that the $$$i^{th}$$$ component carries expressed in $$$\sigma^r_{i}$$$, as $$$w^r_{i}=(\sigma^r_{i}-\sigma^r_{1})/(\sigma^r_{plateau}-\sigma^r_{1})$$$ (see Figure2). This allows to optimize the filtering method based on the amount of noise and information present in each component.
3) The retained component coefficients are projected back in the original space and used for the denoised data reconstruction.
Carrying out only the first and third step, we call the method “CASA basic”, and “CASA advanced” when all three steps are applied.
Patient data acquisition and postprocessing:
Imaging clinical data on a glioma patient were acquired on a 3T whole-body MRI system (MAGNETOM Prisma; Siemens Healthcare, Erlangen, Germany) with a 64-channel Head/Neck coil. A 3D snapshot-GRE CEST protocol7 (MPI03) was used to acquire WASAB18 and Amide Proton Transfer weighted4 (APTw) data with parameter details listed in Figure3. Data were motion corrected with SimpleElastix9. Olea Sphere 3.0 (Olea Medical, La Ciotat, France) was used to compute B0/rB1 map from WASAB1 and correct the APTw-Z-Spectra.
Synthesized data:
A simulated brain phantom was generated starting from the clinical APTw dataset with its same 3D resolution. The Z-Spectra were fitted with the Bloch-McConnel equations modified to include the exchange terms with a five pools model10,11, using MATLAB (parameters in Figure3). The phantom (ground truth) Z-Spectrum volumes were computed at 25 equally-spaced offsets from -6ppm to 6ppm (step=0.5ppm).
The phantom was corrupted by several percentage levels of Rician noise (0.25%,0.5%,1%,3% of the maximum intensity for each Z-Spectra) in frequency domain. The phantom data were PCA denoised using both CASA methods, Malinowski, Nelson and Median selection criteria. MTRasym12 (at 3.5ppm) maps were computed on the ground truth and on various denoised data. These maps were used for comparison.Results
Data quality analysis using Peak signal-to-noise ratio (PSNR), Structural Similarity Index (SSIM), Correlation and Mean Square Error (MSE) have been used to evaluate the goodness of the various denoising methods.
The results in Figure4 shows that for all noise levels "advanced CASA" metric leads to the best results (highest PSNR/SSIM/Correlation and Lowest MSE). Figure5 shows the MTRasym maps of ground truth, data corrupted by various noise levels, and after PCA denoising with "advanced CASA" criterion.Discussion and Conclusion
A new PCA denoising methodology has been proposed for multi-acquisition MRI data, optimized to preserve anatomical structures and pathological information. The advanced version of the proposed method led to the best results between the different evaluated PCA denoising methods on CEST APTw multi-volume acquisitions. An additional investigation should be performed to compare the advanced CASA method with other PCA denoising methods in the literature5,6.Acknowledgements
The research leading to these results has received
funding from AIRC MFAG 2017 ‐ ID. 20153 project – P.I. Longo Dario Livio.
This project has received funding from the European Union’s
Horizon 2020 research and innovation programme under grant agreement No 667510
and the Department of Health’s NIHR-funded Biomedical Research Centre at
University College London. SB and LM are supported by the National Institute of
Health Research Biomedical Research Council, UCL Hospitals NHS Trust.References
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