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Frequency-dependent diffusion-relaxation multidimensional MRI of the human brain
Jessica TE Johnson1, Thomas J Ross2, Yihong Yang2, Daniel Topgaard3, and Dan Benjamini1
1National Institute on Aging, Baltimore, MD, United States, 2National Institute on Drug Abuse, Baltimore, MD, United States, 3Lund University, Lund, Sweden

Synopsis

Keywords: Microstructure, Diffusion/other diffusion imaging techniques

Using an integrative acquisition and processing pipeline that joins concepts from oscillating gradients, tensor-valued encoding, and diffusion-relaxation correlation, we comprehensively explored microstructure and local chemical composition in the human brain. Using both frequency-dependent and tensorial aspects of the encoding spectrum b(ω), we designed an in vivo, whole brain, 40-min 7D D(ω)-R1-R2 distribution acquisition protocol at 2mm isotropic resolution. Scanning eleven healthy participants, we demonstrated frequency/time-dependent changes of diffusion-relaxation correlations measures in the human brain. Finally, intra-scan test–retest repeatability of a range of reconstructed parametric maps was investigated.

Introduction

Diffusion-relaxation correlation NMR1-5 maximizes the amount of encoded chemical and microstructural information by probing relaxation and diffusion mechanisms simultaneously. Over the past decade, these methods were combined with spatially resolved measurements6-8 and applied ex- and in vivo.9-14 Recently, acquisition schemes with free gradient waveforms exploring both the frequency-dependent and tensorial aspects of the encoding spectrum b(ω) have enabled estimation of nonparametric distributions of frequency-dependent diffusion tensors.15

We have incorporated the concepts of diffusion tensor distributions,16-18 tensor-valued encoding,19-21 Monte Carlo inversion,22,23 and frequency-dependent diffusion tensors15 into a single framework. Building on previous 7D D(ω)-R1-R2 “massively multidimensional” MRI ex vivo study,24 we adapt this method to a 40 min whole brain in vivo acquisition protocol at 2 mm isotropic resolution, perform brain imaging on healthy participants, and asses test-retest reliability.

Methods

Eleven healthy participants (ages 37.8±11.0 years, 7 women) were scanned on a 3T system (MAGNETOM Prisma, Siemens Healthcare AG, Erlangen, Germany) with a 32-channel head coil. A subset of three participants were scanned twice, a few weeks apart, to allow assessment of test-retest reliability. Data were acquired using a single-shot spin-echo EPI sequence modified for tensor-valued diffusion encoding.25 Numerically optimized26 linear, planar, and spherical b-tensors were employed with b-values ranging between 0.1 and 3ms/µm2. Here we augment the data acquisition scheme with exploration of the ω-dimension of b(ω) in the range of 6.5-21.5Hz centroid frequencies to allow decoupling of frequency-dependent diffusion components. Sensitivity to R1 and R2 was achieved by acquiring data with different combinations of repetition- and echo times (Figure 1).

The data were first preprocessed using the TORTOISE package,27-29 and subsequently processed in Matlab R2019b (MathWorks, Natick, MA) using the 7D Monte Carlo inversion algorithm24 as implemented in the multidimensional diffusion MRI toolbox.30 The components of the inversion, i.e., axial and radial diffusivities [D||,D], azimuthal and polar angles [Θ,Φ], longitudinal and transversal relaxation rates [R1,R2], along with high frequency isotropic diffusivity D0, and axial and radial transition frequencies, $$$\Gamma_{||}$$$ and $$$\Gamma_{\bot}$$$,15 were sampled in the ranges 0.05$$$\leq$$$D||//0$$$\leq$$$5µm2/ms,0$$$\leq$$$Θ$$$\leq$$$p,0$$$\leq$$$Φ$$$\leq$$$2p,0.2$$$\leq$$$R1$$$\leq$$$2s-1,1$$$\leq$$$R2$$$\leq$$$30s-1,0.01$$$\leq\Gamma_{\bot/||}\leq$$$10000s-1.

The dimensions of the D(ω)-R1-R2 distributions in the primary analysis space [D||,D,Θ,Φ,D0,G||,G,R1,R2] were evaluated at selected values of ω within the narrow 6.5-21.5Hz window actually probed by the gradient waveforms, giving a set of ω-dependent distributions in the [D||(ω),D(ω),Θ,Φ,R1,R2] space. For each value of ω, the results are visualized as ω-independent distributions by projecting D||(ω) and D(ω) to the dimensions of isotropic diffusivity Diso(ω) and squared normalized anisotropy DΔ2(ω),24 and mapping means, variances, and covariances over relevant dimensions and sub-divisions (“bins”) of the distribution space, roughly corresponding to white matter (WM), gray matter (GM), and CSF. Following conventions often used to display results from oscillating gradient encoding,31 the effects of restricted diffusion were quantified by a finite difference approximation of the rate of change of the diffusivity metrics with frequency within the investigated window, which in our case was 21.5Hz and 6.5Hz.

Using a subset of three participants with repeat visits, test-retest variability (VAR) was calculated as percentage of difference in proportion to average of test and retest acquisitions (|scan1-scan2|/[[scan1+scan2]/2]) of whole-brain average values of seven parametric maps: E[Diso], E[DΔ2], E[R1], E[R2], fbin1, fbin2, and fbin3. In addition, we computed the intra class correlation coefficient for single measurement (ICC(3,1)) to evaluate the reliability of these measures.32-34

Results

Figure 2 shows experimental and fitted signals and corresponding 2D projections from full D(ω)-R1-R2 distributions in four representative voxels associated with WM in the corpus callosum, cortical GM, border of cortex and WM, and CSF in the ventricles. The distributions reflect the microstructural differences of the respective tissue type, e.g., comparable Diso yet high DΔ2 in WM compared with GM, and fastest relaxation in WM. Note the strong frequency dependency at the border of cerebral cortex and WM, where a highly anisotropic component at low frequency vanishes at 23Hz.

Figure 3 displays axial maps of global and bin-specific statistical descriptors of D(ω)-R1-R2 from a representative subject. The contrasts are in good agreement with previously published D-R1-R2 data.25 We observed spatial patterns of rate of frequency change of the diffusivity metrics, e.g., predominantly positive or negative values of Diso or DΔ2, respectively, in the occipital cortex. To get a more comprehensive description of the diffusion frequency dependencies in the brain, we used the earth mover’s distance (EMD)35 to quantify the voxelwise difference between 7D D(ω)-R1-R2 spectra at given diffusion frequency. Pairwise EMD values at 6 diffusion frequencies are summarized in a distance matrix, shown in Figure 4. Strongest frequency dependencies were observed in deep WM and cortical brain regions. Lastly, the ICC(3,1) and VAR values for repeatability and variability were generally high or low, respectively, for all measures (Figure 5).

Discussion

We showed that “massively” multidimensional diffusion-relaxation correlation MRI, which joins diffusion-relaxation correlation, time/frequency dependent diffusion, and tensor-valued encoding, is feasible on a clinical system at whole-brain 2mm isotropic resolution using a 40-min acquisition protocol. The resulting voxelwise nonparametric D(ω)-R1-R2 distributions provide unprecedented level of detail with respect to local chemical composition and microstructure. While we intend to carefully map brain regions and expand the diffusion frequency range in the future, our preliminary results show a clear pattern of frequency-dependent diffusion-relaxation correlation in the human brain.

Acknowledgements

This work was supported by the Intramural Research Program of the National Institute on Aging and the National Institute on Drug Abuse of the National Institutes of Health.

References

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Figures

Figure 1. Key experimental details. (A) Time-dependent effective gradients G(t) and (B) corresponding tensor-valued encoding spectra b(𝜔) for linear, planar, and spherical encoding at different echo times and centroid frequencies. (C) Acquisition protocol with repetition time TR, echo time TE, as well as b-tensor magnitude b, normalized anisotropy bΔ (planar: –0.5, spherical: 0, linear: 1), orientation (Θ, Φ), and centroid frequency, versus image acquisition index.

Figure 2. Representative voxels in the human brain. (a) S0 map with crosses indicating voxels locations. (b) Single-voxel attenuation profiles (colored circles) and their fits (black dots). (c) D(ω)-R1-R2 distributions for each voxel projected onto the 2D Diso-DΔ2, Diso-R1, and Diso-R2 planes for five frequencies in the range ω/2π=6-23Hz as indicated with the linear gray scale of the contour lines.

Figure 3. Parameter maps derived from voxelwise D(ω)-R1-R2 distributions. (a) S0 map displayed in gray scale, diagram with the division of the 2D Diso-DΔ2 projection into three bins (bin1,bin2,bin3), and the resulting signal fractions (fbin1,fbin2,fbin3) coded into RGB color. (b) Per-voxel means E[x], variances V[x], and covariances C[x,y] at frequency 6.5Hz. (c) Parameter maps of the rate of change with frequency, Δω/2π. (d) Bin-resolved maps of E[x] and Δω/2πE[x]. The brightness and color scales represent, respectively, the signal fractions and the values of each parameter.


Figure 4. Quantification of frequency-dependent diffusion-relaxation correlations via visualization of voxelwise pairwise earth mover’s distance (EMD) between different frequencies. Clear spatial patterns are visible, with the strongest frequency-dependent diffusion-relaxation correlations in deep WM and cortical brain regions.

Figure 5. Test-retest variability (VAR) and repeatability (ICC(3,1)) calculated from a subset of three participants with repeat visits. Whole-brain averages were used, and VAR and ICC(3,1) are shown for seven parametric maps: E[Diso], E[DΔ2], E[R1], E[R2], fbin1, fbin2, and fbin3. E[R2] yielded negative ICC, which is theoretically difficult to interpret, and therefore was set to zero.


Proc. Intl. Soc. Mag. Reson. Med. 31 (2023)
0679
DOI: https://doi.org/10.58530/2023/0679