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Optimisation of multi-compartment relaxometry myelin water imaging (MCR-MWI)
Kwok-Shing Chan1 and José P. Marques1
1Donders Institute for Brain, Cognition and Behaviour, Radboud University, Nijmegen, Netherlands

Synopsis

In this study, we optimise the variable flip angle acquisition protocol for GRE-based myelin water imaging using MCR model. We show numerically and via in vivo imaging that MCR-MWI can be performed with as few as 3 flip angles and still be able to achieve similar measurement performance as with 7 flip angles. We also conduct an analysis to investigate the usefulness of an image denoising method to improve MWI. Preliminary results suggest that MCR-MWI is very robust to noise and higher resolution data is needed to have a better insight.

Introduction

Myelin water imaging (MWI) using multi-echo gradient echo (mGRE) sequence to probe myelin in white matter (WM) is getting more attention because of its simple implementation and high scan time efficiency1-4. MGRE MWI requires fitting the signal decay with a 3-pool model which is a poorly-conditioned problem5. Recently, it was demonstrated that a variable flip angle (VFA) mGRE acquisition scheme combined with multi-compartment relaxometry (MCR-MWI) provided a more robust MWI measurement and insured convergence of the fitting process6. In the initial MCR-MWI implementation, the VFA scheme included 7 flip angles to ensure a variety of T1-weighting was introduced, which inevitably lengthened the scan time. In this study, we set out to investigate (1) if the acquisition time can be shortened by reducing the number of flip angles without affecting the robustness of MCR-MWI, and (2) if we can incorporate image denoising methods to further improve MWF estimation.

Methods

Numerical Simulation
Monte Carlo simulations were conducted to study the effect of reducing the number of flip angles on MCR-MWI robustness. A 3-pool WM signal was simulated using MCR6 and hollow cylinder models7 using the same parameters as shown in 6 Simulation #4 of Table 1. Gaussian noise was added to the signal to simulate moderate SNR for each flip angle (SNRTE0=57 when α=20°, same noise level for all data). Data fitting was performed using all 7 flip angles and all subsets among the 7 flip angles, from data comprised only 5 to 2 flip angles. The process was repeated 4000 times such that statistical analysis can be performed.

Simulated measurement accuracy and precision were accessed by examining the bias and standard deviation (SD) of the MWF fitting, normalised by the values from using 7 flip angles:
$$bias=\frac{|\overline{MWF_{2,3,4,5FA}}-MWF_{ground truth}|}{|\overline{MWF_{7FA}}-MWF_{ground truth}|} [Eq.1]$$
$$precision=\frac{SD(MWF_{2,3,4,5FA})}{SD(MWF_{7FA})|} [Eq.2]$$
where $$$MWF_{ground truth}$$$ is the MWF in simulated signal, $$$MWF_{2,3,4,5FA}$$$ is the fitted MWF with different flip angle subsets and $$$MWF_{7FA}$$$ is the fitted MWF using all 7 flip angles. Since it is unlikely the bias and precision of a subset can outperform full dataset, values derived from Eqs.1&2 were thresholded to 1 if they were lower than 1. A performance metric was derived to determine the optimum subset of flip angle combination that can produce a similar performance as using full dataset:
$$performance = bias \times precesion [Eq.3]$$
In vivo imaging
VFA mGRE data acquired at 3T (Siemens, Erlangen) for the previous MCR-MWI study were processed retrospectively6. In short, 8 healthy subjects were scanned with a monopolar 3D mGRE, TR/TE1/ΔTE/TE12=46/2.15/3.05/35.7ms, res=1.8mm iso., α=[5,10,20,30,40,50,70]°, GRAPPA=2 and TA=3.5mins. Additionally, higher resolution mGRE data was acquired from 2 of the 8 subjects: monopolar 3D mGRE, TR/TE1/ΔTE/TE12=46/2.15/3.03/35.48ms, GRAPPA=3, res=1.4mm iso., α=[5,10,20,30,40,50,70]° and TA=4.5mins. Tissue classification mask was obtained from MP2RAGE data as previous described6.

MCR-MWI fitting was performed using data from the optimal flip angle set determined from the simulations, corresponding to the optimum solutions of α=[10,20,70]°, [5,10,70]° and [10,20,50]°.

Group histogram analysis was performed on the MWF estimated using the 1.8mm isotropic GRE data across all subjects.

Additionally, the high-resolution GRE data were processed with MP-PCA8 with a 5x5x5 kernel size applied independently to each flip angle prior data fitting. MCR-MWI was applied on both denoised and original data to observe the impact on MWF reconstruction.

Results and Discussion

Numerical simulation
Similar accuracy compared to using 7 flip angles can be achieved with as fewer as using only 3 flip angles, whereas significant bias is observed when using 2 flip angles (Figs1&2). The optimum precision progressively decreased with data reduction (~1.4SD of 7 flip angles when 3 flip angles were used). From a simplistic data average perspective, the SD would be expected to increase by 1.5 for the 3-flip-angle scenario, suggesting an increased efficiency of this protocol.

In vivo imaging
Fig.3 shows the 1.8mm isotropic MWF maps. The MWF maps derived from full dataset (Fig.3a) and the top three subsets of 3 flip angles (Fig.3b-d) share similar contrast, with patch-like differences can be found across the brain (blue arrows), which are likely to due to image artefacts related to movement between acquisitions. Group-averaged MWF histograms of both global WM and grey matter (GM) from the 3-flip-angle dataset are slightly shifted to the left when compared to those of full dataset (Fig.4), potentially caused by the artefact related bias shown in Fig.2 or unbalanced MT9. Both tissues have a broader spectrum when using the 3-flip-angle dataset, as predicted by the simulations.

High-resolution MCR-MWI results derived from 3 flip angles (Fig.5b) are noticeably noisier than the full dataset counterpart (Fig.5a,c), apart from the similar bias in frontal WM shown in Fig.2. Incorporating MP-PCA denoising does not provide any significant improvement to the results of using 3 flip angles (Fig.5c,e).

Conclusions

MCR-MWI is possible with at least 3 flip angles without significantly degrading the performance, allowing acquisition time to be reduced to ~40% in the original implementation.

MCR-MWI using 3 flip angles with MP-PCA denoising did not show significant improvements, yet this could be due to the robustness of MCR-MWI to noise. Higher-resolution data or higher accelerated data will be acquired in the future to fully investigate the potential of denoising methods in more demanding SNR conditions.

Acknowledgements

This work is part of the research programme with project number FOM-N-31/16PR1056/RadboudUniversity, which is financed by the Netherlands Organisation for Scientific Research (NWO).

References

1. Gelderen, P. van et al. Nonexponential T2* decay in white matter. Magnetic resonance in medicine 67, 110–117 (2011).

2. Nam, Y., Lee, J., Hwang, D. & Kim, D.-H. Improved estimation of myelin water fraction using complex model fitting. Neuroimage 116, 214–221 (2015).

3. Shin, H.-G. et al. Advances in gradient echo myelin water imaging at 3T and 7T. Neuroimage 188, 835–844 (2018).

4. Alonso-Ortiz, E., Levesque, I. R. & Pike, G. B. Impact of magnetic susceptibility anisotropy at 3 T and 7 T on T2*-based myelin water fraction imaging. Neuroimage 182, 370–378 (2018).

5. Lee, J. et al. So You Want to Image Myelin Using MRI: An Overview and Practical Guide for Myelin Water Imaging. J Magnetic Reson Imaging Jmri (2020) doi:10.1002/jmri.27059.

6. Chan, K.-S. & Marques, J. P. Multi-compartment relaxometry and diffusion informed myelin water imaging – promises and challenges of new gradient echo myelin water imaging methods. Neuroimage 221, 117159 (2020).

7. Wharton, S. & Bowtell, R. Gradient echo based fiber orientation mapping using R2* and frequency difference measurements. Neuroimage 83, 1011–1023 (2013).

8. Does, M. D. et al. Evaluation of principal component analysis image denoising on multi-exponential MRI relaxometry. Magnetic resonance in medicine 81, mrm.27658-3514 (2019).

9. Teixeira, R. P. A. G., Malik, S. J. & Hajnal, J. V. Fast quantitative MRI using controlled saturation magnetization transfer. Magnetic resonance in medicine 81, 907–920 (2019).

Figures

Fig. 1: Monte Carlo simulations derived measurement performance from using (top to bottom) only 5 flip angles to 2 flip angles with all possible combinations. It is clear that generally both accuracy (low bias) and precision improved when the combinations comprising small flip angles (5° and 10°) and large flip angles (50° and 70°). The dashed line indicates the reference performance to using data of 7 flip angles. Having the performance value close to 1 means the subset has similar performance as using data of all 7 flip angles.

Fig. 2: Top 5 subsets of the 7 flip angles were tested in the numerical simulations. Texts highlighted in blue and red indicate the best and worst performers among the top 5. When reducing the number of flip angles, similar accuracy as fitted with all 7 flip angles can be achieved as fewer as using 3 with the progressive expense of measurement precision. Even the best performer of using 2 flip angle shows a significant increase of bias, though the precision is similar to using 3 flip angles. Left panels show the corresponding options among the steady-state signals.

Fig. 3: Example of MWF on 2 axial slices on 1 subject using data from (a) 7 flip angles and (b-d) top 3 performed subsets of using 3 flip angles. All sets of data produced MWF maps with similar contrast globally, and noise appearance followed the pattern suggested by the simulations. (c) Substantial differences to the full dataset result can be found as patches across the brain, depending on which flip angles were used, which is likely to be caused by the artefacts in the data and potential unbalanced MT effect (blue arrows).

Fig. 4: Group-averaged MWF histograms on WM and GM across 8 subjects using 1.8mm isotropic data from (a) 7 and (b) 3 flip angles. Both WM and GM histograms of using 3 flip angles have a slight left shift when compared to those of using 7 flip angles, possibly caused by the artefact related bias shown in Fig.3, and potentially unbalanced MT effect among the data. Histograms broadening can also be observed when fitting used 3 flip angles. This is in line with the decrease of measurement precision in the numerical simulations shown in Figs.1&2.

Fig. 5: Compare to the results of using 7 flip angles (a), high-quality MWF and other quantitative parameters can still be obtained using data from only 3 flip angles on 1.4mm isotropic data (b), though the noise in these maps is more pronounced when compared to the 1.8mm isotropic MWF in Fig.3. (c) Bias caused by artefacts is also more noticeable in the high resolution maps because of the longer scan time. (d) Results with MP-PCA denoising only show negligible differences compared to those without denoising.

Proc. Intl. Soc. Mag. Reson. Med. 29 (2021)
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