Abstract

Measuring fibre dispersion in white matter with diffusion magnetic resonance imaging (MRI) is limited by an inherent degeneracy between fibre dispersion and microscopic diffusion anisotropy (i.e., the diffusion anisotropy expected for a single fibre orientation). This means that estimates of fibre dispersion rely on strong assumptions, such as constant microscopic anisotropy throughout the white matter or specific biophysical models. Here we present a simple approach for resolving this degeneracy using measurements that combine linear (conventional) and spherical tensor diffusion encoding.To test the accuracy of the fibre dispersion when our microstructural model is only an approximation of the true tissue structure, we simulate multi-compartment data and fit this with a single-compartment model. For such overly simplistic tissue assumptions, we show that the bias in fibre dispersion is greatly reduced (~5x) for single-shell linear and spherical tensor encoding data compared with single-shell or multi-shell conventional data. In in-vivo data we find a consistent estimate of fibre dispersion as we reduce the b-value from 3 to 1.5 ms/μm2, increase the repetition time, increase the echo time, or increase the diffusion time. We conclude that the addition of spherical tensor encoded data to conventional linear tensor encoding data greatly reduces the sensitivity of the estimated fibre dispersion to the model assumptions of the tissue microstructure.

Highlights

  • Diffusion magnetic resonance imaging (MRI) is commonly used to reconstruct in-vivo white matter tracts and estimate connectivity between brain regions

  • We investigate the bias incurred in the fibre dispersion estimate when fitting a single-compartment model (i.e. eqs. (4) and (13)) to data simulated from a two-compartment tissue with varying “intra-axonal” signal fractions

  • The single-compartment model assumes that microscopic anisotropy remains constant across b-values, which is invalid for this data generated from two compartments

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Summary

Introduction

Diffusion MRI is commonly used to reconstruct in-vivo white matter tracts and estimate connectivity between brain regions. A wide variety of methods have been proposed to deconvolve the diffusion MRI signal to extract these main fibre orientations (Basser et al, 2000; Tuch, 2004; Anderson, 2005; Behrens et al, 2007; Tournier et al, 2007; Descoteaux et al, 2007; Dell’Acqua et al, 2007, 2010). Most are based on spherical deconvolution (Dell’Acqua and Tournier, 2018), where the diffusion signal S is modelled as the convolution between the fODF and a single-fibre response function R:

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