Tomasz Pieciak1, Maryam Afzali2,3, Antonio Tristán-Vega1, and Santiago Aja-Fernández1
1Laboratorio de Procesado de Imagen (LPI), Universidad de Valladolid, Valladolid, Spain, 2Leeds Institute of Cardiovascular and Metabolic Medicine, University of Leeds, Leeds, United Kingdom, 3Cardiff University Brain Research Imaging Centre (CUBRIC), School of Psychology, Cardiff University, Cardiff, United Kingdom
Synopsis
The orientationally-averaging or the so-called power-averaging is a common approach to reduce the impact of macroscopic anisotropy in diffusion MRI (dMRI). This paper analytically derives two new closed-form unbiased orientationally-averaging diffusion MRI signal estimators and shows that the noise-related bias could be significantly suppressed with these new findings. The new formulas might be applied to retrospectively orientationally-averaged dMRI signals with minimal computational effort.
Introduction
The orientationally-averaging is a common approach used to reduce the impact of macroscopic anisotropy in diffusion MRI (dMRI)1,2,3,4. The orientationally-averaged dMRI signals have been successfully practised in tissue characterization, including estimation of the diffusivities parallel and perpendicular to axon13, the T2 relaxation time of intra‐axonal water14 and free-water fraction volume16, white matter segmentation17, or as regularization priors for kurtosis estimation18. The orientationally-averaged signal is typically calculated as the average of diffusion-weighted signal over the samples in the $$$\mathbf{q}$$$-space domain, driving to unwanted noise-induced bias due to a positive skewness of Rician distribution, being de facto the standard statistics used in dMRI6,7. This paper analytically proposes two new closed-form unbiased orientationally-averaging dMRI signal estimators and shows that the noise-related bias could be significantly suppressed. The new formulas might be applied to a retrospectively orientationally-averaged dMRI with minimal computational effort.Methods and materials
The orientationally-averaged signal: The orientationally-averaged diffusion-weighted MRI signal can be calculated as the weighted mean over the $$$\mathbf{q}$$$-space domain samples 2,3,4,14
$$\overline{S}(b)=\sum_{i=1}^{N_g}w_i S(\mathbf{g}_i, b),\ \ \ 0\le w_i\le 1$$
with $$$S(\mathbf{g}_i, b)$$$ being the sample acquired in $$$i$$$-th gradient direction at a specific $$$b$$$-value, and $$$N_g$$$ being the total number of gradient directions defined over the shell $$$b$$$, and $w_i$ is the normalized weight used to compensate the non-uniformity of gradients distribution over the sphere, or via the spherical harmonics (SH) decomposition of the signal2,15
$$\overline{S}(b)=C_{00}\left\{S(\mathbf{g},b)\right\}=\frac{1}{\sqrt{4\pi}}\int_{S}S(\mathbf{g},b) d \mathbf{g}$$
where $$$C_{00}\left\{S(\mathbf{g},b)\right\}$$$ is the zeroth-order
SH decomposition of the signal, or alternatively using the Mean Apparent Propagator MRI coefficients2,5.
Unbiasing orientationally-averaged signal: Calculating the orientationally-averaged signal might introduce a noise-related bias due to a positively-skewed Rician distribution being a typical statistical model assumed in dMRI6, 7,13. Assuming the samples $$$\left\{S(\mathbf{g}_i,b)\right\}_{i=1}^{N_g}$$$ are independent and non-identically Rician distributed, i.e. $$$S(\mathbf{g}_i,b)\sim \mathrm{Rice}(A(\mathbf{g}_i, b),\sigma(b))$$$ with the noise-free amplitude $$$A(\mathbf{g}_i,b)$$$ and non-centrality parameter $$$\sigma(b)$$$ defined for each $$$b$$$-value independently, we can define the asymptotic expansion of the expectation operator of the signal8, $$$\mathbb{E}\{S(\mathbf{g},b)\}=\sigma(b)\sqrt{2x}+\frac{1}{2}\sqrt{\frac{2}{x}}+\mathcal{O}\left(x^{-3/2}\right)$$$ with $$$x=\frac{A^2(\mathbf{g}, b)}{2\sigma^2(b)}$$$ and $$$\mathcal{O}(\cdot)$$$ being the decay of the corresponding term as fast as the function argument. Starting from give asymptotic expansion of the expectation operator, we analytically derive two new unbiased orientationally-averaged diffusion-weighted MRI signal estimators:
$$\overline{S}_{\mathrm{unbiased}}^{(1)}(b)=\sum_{i=1}^{N_g}w_iS(\mathbf{g}_i,b)-\frac{1}{2}\widehat{\sigma}^2(b) \left( \sum_{i=1}^{N_g}w_i S(\mathbf{g}_i,b)\right)^{-1}=\overline{S}(b)-\frac{1}{2} \frac{\sigma^2(b)}{\overline{S}(b)}$$
$$\overline{S}_{\mathrm{unbiased}}^{(2)}(b)=\frac{1}{2} \left(\sum_{i=1}^{N_g}w_iS(\mathbf{g}_i,b)+\left(\sum_{i=1}^{N_g}w_i S(\mathbf{g}_i,b)-\sqrt{2}\sigma(b)\right)^{1/2} \left(\sum_{i=1}^{N_g}w_i S(\mathbf{g}_i,b)+\sqrt{2}\sigma(b)\right )^{1/2}\right) \\
= \frac{1}{2} \left( \overline{S}(b) + \left( \overline{S}(b) - \sqrt{2}\sigma(b) \right )^{1/2} \left( \overline{S}(b) + \sqrt{2}\sigma(b) \right )^{1/2} \right)$$
where $$$\sigma(b)$$$ is the noise level measured in a voxel-wise manner under a specific $$$b$$$-value. The parameter $$$\sigma(b)$$$ can be estimated from all samples available in a voxel, i.e. $$$\widehat{\sigma}(b) = \varphi(\left\{S(\mathbf{g}_1),\ldots,S(\mathbf{g}_{N})\right\})$$$ with $$$\varphi(\cdot)$$$ being the operator used to obtain the noise level (e.g. median absolute deviation9, random matrix theory based method10) or taking into account a spatial neighbourhood of the sample11,12.
In silico data:
The
synthetic dMRI signal was generated under three scenarios: 1)
free-water diffusion with a fixed
diffusivity at $$$D_0=3.0\times10^{-3}\
\mathrm{mm}^2/\mathrm{s}$$$, 2)
restricted diffusion with parallel and perpendicular diffusivities at
$$$D_{||}=2.0\times10^{-3}\ \mathrm{mm}^2/\mathrm{s}$$$ and
$$$D_\perp=0.75\times10^{-3}\ \mathrm{mm}^2/\mathrm{s}$$$, and
3) a mixture
of free-water and restricted
diffusion with a volume fraction of $$$f=0.2$$$ and same parallel and perpendicular diffusivities. All signals were generated under $$$b=1000\ \mathrm{s}/\mathrm{mm}^2$$$ and 90 uniformly distributed gradient directions.
In vivo data: We use two publicly available datasets: 1) Sherbrooke diffusion MRI data acquired with a 1.5T Siemens scanner and delivered with DIPY tool19. The data consists of three shells at $$$(1000,2000,3500)\ \mathrm{s}/\mathrm{mm}^2$$$ and 64 gradient directions per a single shell, and 2) the Human Connectome Project (HCP) MGH20 data (subject 1016) acquired on a Siemens 3T Connectom scanner at four b-values $$$(1000,3000,5000,10000) \ \mathrm{s}/\mathrm{mm}^2$$$ with $$$(64,64,128,256)$$$ gradient directions, voxel resolution of $$$1.5 \ \mathrm{mm}^3$$$.
Data processing: To estimate the parameter $$$\sigma(b)$$$, we use a variance-stabilizing homomorphic filter11,12 applied over each gradient direction and aggregate them to a representative noise level using a mean operator across all gradient directions at the specified $$$b$$$. Orientationally-averaged signals are calculated using the SH expansion at the order of 2.Results
- Fig.1 displays the relative error (in %) and Fig.2 shows the bias of the orientationally-averaged dMRI signal obtained with three estimators, namely the standard one and two proposed under three scenarios: 1) free-water diffusion, 2) restricted diffusion and 3) combined diffusion with a free-water volume fraction of $$$f=0.2$$$.
- Fig.3 and Fig.4 visually inspects the orientationally-averaged dMRI signals in axial slices using two in vivo datasets with the estimators specified above, along with the absolute errors calculated between the standard approach and unbiased equivalents.
Discussion and conclusions
In this paper, we analytically derived two new unbiased orientationally-averaging estimators under the assumption of Rician statistics for dMRI data. Our study has led to the following conclusions:
- Proposed estimators significantly reduce the orientationally-averaging noise-induced bias due to aggregation of the samples from positive skewed Rician statistics.
- Under the high SNR of the dMRI data, i.e. $$$\widehat{\sigma}(b) \rightarrow 0$$$, the correction components in both estimators $$$\overline{S}_{\mathrm{unbiased}}^{(1)}(b)$$$ and $$$\overline{S}_{\mathrm{unbiased}}^{(2)}(b)$$$ rule out themselves, and consequently, the equations reduce to the standard formula.
- New signal estimators are easy to obtain directly or via the SH expansion, can be applied to retrospectively orientationally-averaged dMRI signals, and do not require any non-standard tools or algorithms to be used except for the noise level estimation.
Acknowledgements
The authors acknowledge Ministerio de Ciencia e Innovación of Spain with research grant RTI2018-094569-B-I00. Tomasz Pieciak acknowledges the Polish National Agency for Academic Exchange for the grant PN/BEK/2019/1/00421 under the Bekker programme and the Ministry of Science and Higher Education (Poland) under the scholarship for outstanding young scientists. Maryam Afzali acknowledges a Wellcome Trust Investigator Award (219536/Z/19/Z).References
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