Abstract
Recently, T2* imaging at 7 tesla (T) MRI was shown to reveal microstructural features of the cortical myeloarchitecture thanks to an increase in contrast-to-noise ratio. However, several confounds hamper the specificity of T2* measures (iron content, blood vessels, tissues orientation). Another metric, magnetization transfer ratio (MTR), is known to also be sensitive to myelin content and thus would be an excellent complementary measure because its underlying contrast mechanisms are different than that from T2*. The goal of this study was thus to combine MTR and T2* using multivariate statistics in order to gain insights into cortical myelin content.
Seven healthy subjects were scanned at 7T and 3T to obtain T2* and MTR data, respectively. A multivariate myelin estimation model (MMEM) was developed, and consists in (i) normalizing T2* and MTR values and (ii) extracting their shared information using independent component analysis (ICA). B0 orientation dependence and cortical thickness were also computed and included in the model.
Results showed high correlation between MTR and T2* in the whole cortex (r=0.76, p<10−16), suggesting that both metrics are partly driven by a common source of contrast, here assumed to be the myelin. Average MTR and T2* were respectively 31.0 +/− 0.3% and 32.1 +/− 1.4 ms. Results of the MMEM spatial distribution showed similar trends to that from histological work stained for myelin (r=0.77, p<0.01). Significant right-left differences were detected in the primary motor cortex (p<0.05), the posterior cingulate cortex (p<0.05) and the visual cortex (p<0.05).
This study demonstrates that MTR and T2* are highly correlated in the cortex. The combination of MTR, T2*, CT and B0 orientation may be a useful means to study cortical myeloarchitecture with more specificity than using any of the individual methods. The MMEM framework is extendable to other contrasts such as T1 and diffusion MRI.
Keywords: MTR, T2*, B0 orientation, myeloarchitecture, ICA, Brodmann
Introduction
Myeloarchitecture refers to the spatial organization of myelinated fiber in the central nervous system, including features such as their size, density orientation, and myelination (Flechsig, 1920; Vogt, 1911). The study of myeloarchitecture in the in vivo human cortex can provide further elements about the organization of the healthy and pathological cortex.
Previous studies have shown that T2* magnitude and phase images can reveal exquisite details of cortical microstructure, with enhanced contrast at ultra-high field strength (Duyn et al., 2007; Li et al., 2009, 2006). T2* is the effective transverse relaxation and is driven by microscopic and macroscopic field inhomogeneities, e.g. caused by susceptibility differences between tissues (Cohen-Adad, 2014). Of interest, T2* contrast is notably influenced by the size, density and orientation of myelinated fibers (Hwang et al., 2010; Lee et al., 2012; Pitt et al., 2010). Surface-based analysis of T2* revealed several features that correlate with myelin distribution in the cortex (Cohen-Adad et al., 2012, 2011; Deistung et al., 2013; Mainero et al., 2015). Similar observations were obtained from T1 (Dinse et al., 2013) and T1w/T2w (Glasser and Van Essen, 2011) measurements, further confirming the influence of myelin on T2* contrast. Despite its sensitivity to myeloarchitecture, T2* it is influenced by several confounds, such as the tissues iron level (Fukunaga et al., 2010), B0 field inhomogeneities (Hernando et al., 2012) and fibers orientation with respect to B0 (Cohen-Adad et al., 2012). Hence, combining T2* with another measure sensitive to myelin would increase the confidence in assessing the degree of myelination, as has been shown ex vivo (Tardif et al., 2012).
Magnetization Transfer (MT) imaging was shown to be sensitive to myelin content (Levesque and Pike, 2009; Schmierer et al., 2004) in white matter (WM) and thus would be an excellent complementary measure because its underlying contrast mechanisms are different than that from T2*. The MT effect results from the interaction between two kinds of hydrogen nucleus: protons in a liquid state associated with water molecules and protons in semisolid state associated with macromolecules. The macromolecular spins can be saturated by an off-resonance radio frequency (RF) pulse because they have a much broader absorption lineshape than the liquid spins. The preferential saturation of the macromolecular spins can be transferred to the liquid spins, depending on the rate of exchange (Levesque and Pike, 2009). This water spin saturation can then be detected with MRI (Henkelman et al., 2001). MTR is an index calculated using images with and without MT saturation pulse and was shown to correlate with myelin content (Henkelman et al., 2001; Schmierer et al., 2004). Recently, MTR was mapped in the cortex of MS patients (Chen et al., 2013; Derakhshan et al., 2014) and showed similarities between myelinated regions and high MTR values. However, MTR is only a semi-quantitative metric as it depends on sequence parameters, B1 profile and T1 relaxation (Berry et al., 1999; Pike Bruce, 1996).
Combining MTR with T2* thus appears to be a useful means to gain insight into cortical myelination because these two metrics are sensitive to myelin content but are based on different biophysical phenomena. MTR increases with myelin and T2* decreases with myelin.
However, mapping T2* and MTR in the cortex is challenging because the cortical ribbon is thin, highly convoluted and its geometry varies across individuals. Cortical surface-based analysis allows robust visualization of MRI measurements across the entire cortex and enables the calculation of spatial statistics at a population scale (Dale et al., 1999; Derakhshan et al., 2014; Fischl, 2012; Fischl et al., 1999; Glasser and Van Essen, 2011). Other confounds exist that can affect cortical mapping studies. Namely, (i) the effect of cortical thickness, which can introduce variable amount of partial volume effect and (ii) the angle between coherently-oriented myelinated fibers in the cortex and the direction of the main magnetic field (B0) (Cohen-Adad et al., 2012). Multivariate statistics, such as Independent Component Analysis (ICA) can decompose multivariate signal into independent signals coming from independent sources (Bingham and Hyvärinen, 2000; Hyvärinen and Oja, 2000; Xie and Wu, 2006). Here, ICA would be an adequate candidate for probing the existence of shared information between T2*- and MTR-derived signal related to myelin content, while taking into account confounding factors (thickness, B0 orientation).
The goals of the present study were: (i) to map T2* at 7T and MTR at 3T in the healthy in vivo human cortex using surface-based analysis and (ii) to combine T2* and MTR using a multivariate model in order to extract the shared information related to myelin.
Material and Methods
A. Data acquisition
Healthy subjects (N=7, gender = 4F and 3M, age = 36 +/− 5 years) were recruited. Subjects were scanned with a 7T whole-body scanner (Siemens Healthcare, Erlangen, Germany) to measure T2* and with a 3T scanner (Siemens TIM Trio) to measure MTR. We chose not to perform the MTR protocol at 7T due to the less homogeneous B1 profile and SAR limitations. Both scanners were equipped with a 32-channel coil. Parameters values at 7T were: 2D gradient-echo, TR = 2020 ms, TE = 6.34+3.2n [n=0,…,11] ms, resolution = 0.33×0.33×1 mm3, acquisition time (TA) was 20 min (10 min/slab * 2 slab). Parameters for the 3T magnetization transfer contrast were: Spoiled gradient echo sequence: 3D FLASH (Fast Low-Angle Shot), TR/TE = 30/2.49 ms, matrix = 192×192, resolution = 1.2×1.2×1.2 mm3, with (mt_on) and without (mt_off) MT pulse. The MT pulse is a Gaussian envelope with pulse duration = 9984μs and frequency offset = 1200 Hz. The acquisition time (TA) of each FLASH volume was 7:45 min. In addition to the MTR protocol, a T1-weighted image was acquired at 3T for cortical surface reconstruction using a magnetization-prepared rapid acquisition with multiple gradient echoes (MEMPR) (van der Kouwe et al., 2008). Parameters were: TR/TI=2530/1200 ms, TE=[1.7, 3.6, 5.4, 7.3] ms, flip angle (α)=7°, FOV=230×230 mm2, resolution=0.9×0.9×0.9 mm3, bandwidth=651 Hz/pixel, scan time=6.5min. The reason for doing surface reconstruction from 3T data is that this protocol has been thoroughly validated (Dale et al., 1999; Govindarajan et al., 2014; Postelnicu et al., 2009; van der Kouwe et al., 2008), in comparison with the 7T MEMPR protocol, from which the less homogeneous B1+ profile can produce errors in segmentations.
B. Data processing
Figure 1 shows an overview of the data processing pipeline. Pre-processing steps included: (i) computing MTR and T2*. (ii) registering MTR and T2* volumes to the cortical surface model, (iii) sampling the obtained values within the cortex, (iv) calculate the cortical thickness and (v) computing the angle between B0 field and the vector normal to the cortical surface. Processing was done with FreeSurfer (http://surfer.nmr.mgh.harvard.edu) and custom-made scripts written in MATLAB.
T2* data were first corrected for background inhomogeneities as described in (Cohen-Adad et al., 2012), then T2* was estimated using monoexponential fitting. A gross alignment was first performed between the averaged first 4 echoes of the T2*-weighted volume and the T1weighted volume (at 3T) following the protocol described in (Govindarajan et al., 2014) Then, a fine alignment of the T2*-weighted volume to the surface was estimated using the boundary-based registration method (BBR, 9 degrees of freedom), which is based on the local intensity gradient and was shown to have high robustness and accuracy (Greve and Fischl, 2009). Then, the registration matrices were applied to the T2* volume. More details can be found in (Cohen-Adad, 2014). All registrations were visually inspected. For pre-processing of MTR data, both volumes with (mt_on) and without (mt_off) the Gaussian MT pulse were registered to the 3T T1-weighted volume using the function mri_robust_register available in FreeSurfer (Reuter et al., 2010). The mt_off volume was registered to the surface using bbregister (12 d.o.f.). The resulting affine matrix was then applied to the MTR volume. Once both mt_on and mt_off were registered to the cortical surface, MTR was computed as follows:
(1) |
Figure 1 shows the MTR registrations steps. Once registered to the individual surface, MTR and T2* were sampled at the mid distance between the pial and the white matter surface (50% depth) as done in (Cohen-Adad, 2014). The mid-cortical distance was chosen in order to minimize partial volume effect. Cortical thickness (CT) map was calculated using the normal distance between both pial and white matter surfaces previously segmented by freesurfer. B0 orientation dependence was estimated using the angle θz between the normal vector of the surface and the B0 field direction (Cohen-Adad et al., 2012). MTR, T2*, CT and B0 orientation data were then spatially normalized to the existing common space (fsaverage) available in FreeSurfer V4.2. Spatial normalization was performed using a spherical averaging procedure as described in (Fischl et al., 1999). For each subject, the cortical manifold was projected onto the target surface (fsaverage) and assigned a normal vector field with a consistent orientation.
Mean and inter-subject standard deviation (SD) maps were calculated for MTR, T2*, CT and B0 orientation. Then, Pearson’s coefficient was calculated vertex-wise between each pair of the following parameters: MTR, T2*, CT and B0 orientation.
C. Multivariate Myelin Estimation Model (MMEM)
Here we propose a method to merge the myelin-related information contained in MTR and T2* into a single metric. The framework works as follows: Firstly, multilinear regressions were performed using predictors of myelin content (MTR and T2*) and confounding covariates (cortical thickness, which can introduce variable amount of partial volume effect, and B0 orientation dependency). Secondly, independent component analysis (ICA) is used to combine MTR- and T2*-derived signal related to myelin.
The detailed steps of the MMEM are represented in Figure 2. Firstly, two maps were estimated using multilinear regressions: one using the regressors MTR, CT and B0 orientation (ME_MTR) and one using the regressors T2*, CT and B0 orientation (ME_T2*). ME_MTR and ME_T2* maps respectively represent MTR and T2* values corrected for partial volume effect and fibers orientation. Notice that constant regressors such as age and gender were in the constant term of the regression because the MMEM was performed independently for each subjects and the resulting map was normalized under a common dynamic range (explained below). ME_MTR and ME_T2* maps were calculated using equations (2) and (3):
(2) |
(3) |
where a, b, c, d and e are the resulting parameters of the multilinear regressions. θz is the angle between the surface’s normal vector and the B0 magnetic field direction. The estimation of B0 orientation dependency was based on the model presented in (Cohen-Adad et al., 2012; Lee et al., 2011) but rearranged in a linear form to be used in a linear regression. More specifically, the sine function from the orientation dependency model was broken down into a linear sum of sine and cosine (see equation 1,2 and Supplementary Material S1 for the whole derivation). In order to merge MTR and T2* within the same framework, both linear regressions were performed with a common dependent variable. This dependent variable was a binary map made of regions that are known to be highly (BA1, BA4 and BA42) and poorly myelinated (BA8 and BA9) (Annese et al., 2004; Glasser and Van Essen, 2011; Glasser et al., 2014; Laule et al., 2008; Nieuwenhuys, 2013; Vogt, 1911). BA3 was not considered because of the thinness of the cortex in this region (mean CT=1.8mm) and hence strongly hampered by partial volume effect. The regions of high and low myelin content were arbitrarily set to 70% and 30%. It is however important to keep in mind that these arbitrary values were only chosen for adjusting the dynamics of both metrics (i.e. ME_MTR and ME_T2*), on a subject-by-subject basis, in order to explore the relative distribution of myelin-related values throughout the entire cortical ribbon. Secondly, the shared information between ME_MTR and ME_T2* was extracted using ICA decomposition, for each subject. ICA was chosen because (i) it is an unsupervised data-driven algorithm and is therefore free from arbitrary priors, (ii) it outputs mathematically independent components (as opposed to PCA) and (iii) the ‘so-called’ first component represents the shared information from ME_MTR and ME_T2* with the highest variance, which is assumed to represent myelin. This assumption is based on previous studies demonstrating the sensitivity of T2* and MTR to myelin content (Cohen-Adad et al., 2011; Deistung et al., 2013; Levesque and Pike, 2009; Mainero et al., 2015; Schmierer et al., 2004). The hypothesis being that the first component of the ICA was a more specific indicator for myelin content than a single metric taken separately. This hypothesis was further confirmed by simulations (see Supplementary Material S2) and comparison with previous histology works (Braitenberg 1962). The final multivariate myelin estimation was calculated from the principal independent vector of the ICA’s separating matrix (V1) and the matrix (X) containing ME_MTR and ME_T2* data (equation 4). This map was named Combined Myelin Estimation (CME).
(4) |
The robustness of the ICA decomposition was qualitatively checked for each subject by plotting the ICA’s vectors on the original set of data. The ICA’s first component map was then computed for each subject separately. Lastly, the ICA’s first component map were averaged across subjects.
The PALS-B12 Brodmann atlas (Van Essen, 2005) was used for interrogating sub-region of the cortex defined by their cyto-architecture. This choice was driven by previous studies showing homogenous myeloarchitecture within functional areas (Abdollahi et al., 2014; Bock et al., 2009; Geyer and Turner, 2013; Glasser and Van Essen, 2011; Glasser et al., 2014; Nieuwenhuys, 2013; Sereno, 1991).
Results
A. MTR, T2*, CT and B0 orientation mapping
MT and T2* data were successfully acquired in 6 out of 7 subjects. Visual inspection revealed excessive motion in one subject for the MT data. Hence only 6 subjects were used for subsequent analyses.
Figure 3A shows maps of 3T MTR, 7T T2*, CT and B0 orientation averaged across subjects. MTR map shows high values (>32%) notably in the primary motor cortex (BA4), in the primary somatosensory cortex (BA1, BA2 & BA3), in the somatosensory association cortex (BA5 & BA7), in the posterior cingulate cortex (BA31 & BA23), in the visual cortex (BA17, BA18 & BA19) and in the auditory cortex (BA42). However, some ‘strip’ patterns of lower MTR are observed in these regions, notably in the central sulcus (~BA3) and in the calcarine fissure. The CT map also highlights a ‘strip’ pattern in BA3 and shows some regions of low cortical thickness (< 2mm) around the calcarine sulcus. These regions are also highlighted by the CT map by showing thin cortical thickness (between 1 and 2mm). In the frontal cortex MTR is notably low. T2* map shows an overall similar pattern but with an opposite tendency. Low values (<25ms) are visible in the primary motor cortex, the primary somatosensory cortex and in the visual cortex whereas T2* is high (~35ms) in the frontal lobe. The CT map shows lower cortical thickness in BA3, BA17 and BA18 as previously shown (Clarkson et al., 2011; Cohen-Adad et al., 2012).
Figure 3B shows maps of SD across subjects for the respective metrics. MTR SD is fairly homogenous and small in the whole cortex (~1.5%). T2* SD also exhibits fairly small values across the cortex (~2.5ms), however extreme values are found in the lower brain region, likely due to inhomogeneous B0 field at 7T. These fairly small SD maps for MTR and T2* suggest that the two metrics have centered and narrow distributions across subjects and hence the averaged maps are representative of the population studied here. Cortical thickness SD and B0 orientation SD were fairly large on a voxel-by-voxel basis (average SD was respectively 0.47mm and 17.4°), suggesting that there is an inter-subject variability in the morphology of the cortex, e.g., thickness, location and orientation of different gyri/sulci.
Table 1 summarizes the whole brain statistics (mean, inter subject SD and coefficient of variation (COV)). COV coefficients are calculated by performing the ratio between the inter-subjects SD and the mean across the whole cortex. COV are displayed percentage. Inter-subject SD and COV are fairly small for all metrics as previously seen on the maps.
Table 1.
LH | MTR [%] | T2* [ms] | CT [mm] | RH | MTR [%] | T2* [ms] | CT [mm] |
---|---|---|---|---|---|---|---|
Mean | 31.04 | 32.16 | 2.61 | Mean | 31.02 | 32.03 | 2.60 |
SD | 0.34 | 1.42 | 0.053 | SD | 0.41 | 1.39 | 0.061 |
COV [%] | 1.1 | 4.4 | 2.0 | COV [%] | 1.3 | 4.3 | 2.3 |
B. Pearson’s correlations between MTR and T2*
Figure 4 shows the Pearson’s correlations between MTR and T2*. Different colors are showing the vertices density in order to better visualize scatter’s shape. To reduce the high-frequency noise in the correlation space (MTR vs. T2*) a 2-dimensional smoothing of 10 points was achieved before computing the Pearson’s correlation. Strong correlations were observed in the right (r=−0.77) and left (r=−0.75) hemispheres. The colormap reveals higher density in the center of the scatter showing a 2D Gaussian tendency well defined at the center of the distributions.
We also assessed the whole cortex correlation between T2* & CT ; T2* & B0 orientation ; MTR & CT and MTR & B0 orientation. Table 2 shows their corresponding Pearson’s correlation coefficient. We can see that in the whole cortex, correlations with B0 orientation are fairly low.
Table 2.
LH | Thickness | B0 orientation | RH | Thickness | B0 orientation |
---|---|---|---|---|---|
MTR | r = −0.19 p < 10−16 |
r = 0.18 p < 10−16 |
MTR | r = −0.24 p < 10−16 |
r = 0.14 p < 10−16 |
T2* | r = 0.52 p < 10−16 |
r = −0.13 p < 10−16 |
T2* | r = 0.42 p < 10−16 |
r = −0.05 p < 10−8 |
C. Distribution graph
The distribution graph (Figure 5) is a qualitative way to visualize spatial correlations between MTR, T2*, CT and B0 orientation for assessing the feasibility to combine these four metrics using a linear model (first step of the MMEM). First, we compared the shape of MTR, T2*, CT and B0 orientation across all 164,000 vertices. Vertices of the mean T2* map (in red) were sorted in the ascending order. The same index distribution was then used to display MTR (blue), CT (magenta) and B0 orientation (green) values. For clarity, values were smoothed along the abscissa (100-point window). Inter subjects SD have also been plotted for each vertex. We chose to sort T2* values instead of MTR due to the larger number of artefactual vertices in the T2* data, leading to extremely low or high values, related to field inhomogeneity and/or surface registration (Cohen-Adad, 2014). Only the right hemisphere values are plotted for more clarity. Similar trends are observed between left and right hemispheres.
In order to further explore the different trends between metrics, the distribution graph was divided into four ensembles of vertices:
Region 1 (light blue on figure 5): Vertices hampered by strong artifacts on T2* data caused by signal dropout (T2*<24ms). This region contains less than 2% of all cortical vertices.
Region 2 (dark blue): Vertices for which MTR and T2* are correlated. Interestingly, these vertices are mainly located in the gyri adjacent to the central sulcus and the calcarine fissure. There are some dark blue areas that neighbor light blue areas in the lower brain region, and these vertices are likely affected by artifacts due to poor shimming in this region. However, we believe that the same pattern observed in other vertices (e.g., visual and motor cortex) is genuine. This region contains less than 2% of all vertices.
Region 3 (yellow): Vertices where MTR and T2* are anti-correlated (R-squared > 0.90). This region contains more than 96% of all vertices.
Region 4 (red): Vertices with high T2* values (>40ms), notably in anterior cingulate cortex (BA24 & BA32). These vertices are possibly affected by surface misregistration.
The main purpose of this graph was to identify vertices where a linear relationship between MTR and T2* can be tested without introducing too much bias. Based on these results, the combination into a unique framework for estimating myelin content (MMEM, see below) will be performed on region #3.
D. Multivariate myelin estimation model (MMEM)
Multilinear regression
Table 3 shows results of the linear models defined in Figure 2 and equations 2,3. These results show that myelin estimation is proportional to MTR and is inversely proportional to T2*, as was expected (Cohen-Adad et al., 2011; Schmierer et al., 2004). Secondly, we notice that MTR accounts for about 54% of the ME_MTR metric and T2* accounts for about 38% of the ME_T2* metric, whereas cortical thickness and B0 orientation have lesser influence (6% and <1%, respectively). Thirdly, we notice a fairly low inter-subject variability for the fittings coefficients of the constant part (a), the MTR or T2* part (b) and the cortical thickness part (c), that suggest a fairly good robustness of the model. However we notice a high variability of d and e parameters. We believe this is related to the fact that even though T2* is modulated by B0 orientation with respect to cortical surface (Cohen-Adad et al., 2012), this modulation is fairly low compared to that in the white matter. Evidences are found in gray/white matter comparative studies from (Sati et al., 2012). Moreover, it is possible that there is an inter-subject variability in the morphology of the cortex, e.g., orientation of coherently-aligned cortical fibers. Again, our model is performed in a subject by subject basis, and thus is not affected by the morphological inter-subject variability.
Table 3.
a [%] | b [%] | c [%] | d [%] | e [%] | |
---|---|---|---|---|---|
ME_MTR | −39.1 ± 1.9 | 54.2 ± 0.4 | −6.2 ± 1.7 | −0.14 ± 0.4 | −0.05 ± 0.13 |
ME_T2* | 54.4 ± 2.0 | −37.6 ± 2.9 | −6.0 ± 2.5 | 0.33 ± 0.33 | 0.05 ± 0.12 |
Independent Component Analysis (ICA)
The second step was to perform an ICA for each subject, in order to find a transformation matrix that optimizes the extraction of the common information contained in ME_MTR and ME_T2* (Hyvärinen and Oja, 2000; Xie and Wu, 2006). However, performing an ICA with large data vector (~164,000 vertices) is poorly robust. Therefore, a graphical validation of each ICA result (one per subject) was made. This graphical validation was useful to assess the result of each ICA’s and the inter-subject consistency between results.
Figure 6A shows results of ICA for each subject. Pink arrows are the two vectors of the separating matrix W found by the ICA (Hyvärinen et al, 2000). Figure 6B represents the projection of the ME_MTR and ME_T2* data into the space defined by the two vectors of the ICA’s separating matrix. These graphs are useful to assess the non-correlation (r<0.06) of the resulting set of data.
The inter-subject variability of ICA results is fairly low (First vector direction = 58±4° and angle between both vectors = 112±5°), justifying the relevance of computing an average map of principal components across subjects.
Combined Myelin Estimation (CME)
Figure 7 shows the average map of the Combined Myelin Estimation (CME). This map was computed from the first component of the ICA using equation (3) and averaged across subjects. The CME represents the common entity contained by ME_MTR and ME_T2*, i.e., the source shared between ME_MTR and ME_T2* that is mathematically independent from the rest of the acquired signal. Therefore, CME is thought to reflect the cortical myelin content with greater specificity than MTR or T2* alone. The mean and SD of CME across the cortex was 50.3±0.7. Overall, we notice a high myelin estimation (yellow/red) in the primary motor cortex BA4=74±3% (here, % refers to the CME metric, and ±3% refers to the SD across subjects) and in the primary somatosensory cortex (BA1=67±7%, BA2=59±4% and BA3=63±13%). Moreover, a high myelin estimation is also observed in the visual cortex (BA17=67±5% & BA18=68±6%) and the auditory cortex (BA42=57±10%). These results are consistent with previous study (Annese et al., 2004; Glasser and Van Essen, 2011; Glasser et al., 2014; Laule et al., 2008; Nieuwenhuys, 2013; Vogt, 1911).
CME maps comparisons
Figure 8A shows a side-by-side comparison of CME, ME_MTR and ME_T2* on the inflated cortical surface. Major differences between ME_MTR and ME_T2* are indicated with white circles (plain and dashed). In the medial view of ME_T2*, one can observe a higher signal in the visual cortex than that in the ME_MTR (plain-circle). Inversely, the ME_T2* map shows a lower signal in the precuneus areas (small-dashed-circle) and superior frontal cortex (middle-dashed-circle) compared to that in the ME_MTR map. In the lateral view of the ME_MTR map, one can observe a higher signal in the somatosensory association cortex (small-dashed-circle) and in the angular gyrus (plain-circle), compared to that in the ME_T2* map. Figure 8B,C show correlations between the myelin estimations metrics and histology values from (Braitenberg 1962), which are based on optical attenuation measures in an ex vivo human cortex stained for myelin. The Pearson’s correlation coefficients of: ME_MTR vs. Histology, ME_T2* vs. Histology and CME vs. Histology, were respectively 0.71 (p-value < 0.05), 0.69 (p-value < 0.05) and 0.77 (p-value < 0.01). These correlations suggest that CME is a more specific marker for cortical myelin content than ME_MTR or ME_T2* taken separately.
E. Analyses within Brodmann Areas
Figure 9A shows the CME map with an overlay of the PALS-B12 Brodmann Areas (BA). This figure shows a fair adequation between variations of CME and BA borders, for instance in BA1, BA2, BA3 and BA4 (primary motor and primary somatosensory cortex, green arrows), in BA17, BA18, BA19 (visual cortex, blue arrows) and in BA42 (auditory cortex, yellow arrow). However, in several areas (for instance BA22 or BA39) CME is quite heterogeneous, suggesting to divide these regions in smaller areas if we aimed to build a more accurate myelo-architectural atlas.
Figure 9B shows the CME map averaged within each BA and Figure 9C shows the mean BA values, as well as the inter-subject SD and the intra-area SD. In comparison with the SD across the entire cortex (26.5%), the intra-area SD is fairly low (in average 11.9%). We also note that the inter-subject SD is low, with an average coefficient of variation of 25% (here the average COV was calculated by computing the COV for each area, and then averaging all COVs across areas).
Figure 10 shows bar graphs representing mean and intersubject SD values of the different metrics used in the model (CME, MTR, ME_MTR, T2*, ME_T2*) within Brodmann regions. This graph shows the inter-hemispheric differences across (CME, MTR, ME_MTR, T2* and ME_T2*). Overall, we observe a fairly good right-left reproducibility, except in some regions as described hereafter. The CME map shows significant hemispheric differences in BA4 and BA31 (more myelin estimated in RH, p<0.05) and in BA17 and BA23 (more myelin estimated in LH, respectively p<0.05 and p<0.01).
Discussion
This study presented a novel approach to combine MTR and T2* in the in vivo human cortex, with the goal of studying cortical myeloarchitecture. We proposed to use a multivariate model to extract myelin-related information shared by both metrics. The model takes into account cortical thickness and B0 orientation and is flexible, i.e., other metrics such as T1 and diffusion data can be added. In the following, we discuss the sensitivity and specificity of MTR and T2* to detect myelin content, the multivariate model and ICA decomposition for combining MTR and T2* and the resulting maps, limitations and perspectives.
Sensitivity and specificity of MTR and T2* for quantifying myelin content
MT reflects the relative density of macromolecules, such as lipids or proteins. Since myelin has a lipid-protein structure (~80% lipids and ~20% protein), MT is able to provide indirect measure of myelin content. The MT phenomenon is complex and some of its underlying physical mechanisms are still unknown (Kim and Cercignani, 2014). Overall, the MT effect induces reduction of signal in tissues with large amount of MT, such as those with high concentration in macromolecules (e.g., lipids). For example, MT ratio (MTR) was shown to correlate well with myelin content in the white matter (Schmierer et al., 2004). Recently, MTR was shown to be sensitive to cortical demyelination in multiple sclerosis patients (Chen et al., 2013; Derakhshan et al., 2014). However, MTR is only a semi-quantitative metric and has several confounds. Firstly, B1 inhomogeneities related to RF transmission induce variabilities on the MT pulse power, which affect MTR measures. Secondly, MTR values depend on the sequence parameters (Berry et al., 1999). Thirdly, MTR values are affected by T1 relaxation (Pike Bruce, 1996). Despite the longer acquisition time, quantitative MT (Levesque and Pike, 2009) provides more accurate estimation of myelin content.
T2* is the effective transverse relaxation time and is therefore affected by (i) mesoscopic field inhomogeneities, which result from susceptibility differences between tissues (parenchyma, deoxygenated blood, bone, cartilage, etc.) and (ii) macroscopic field inhomogeneities, which arise from magnetic field imperfections, air–tissue boundaries, or ferromagnetic objects (e.g., metal clips, implants, dental prosthesis). The latter are characterized by large-scale gradients that cause enhanced signal decay in gradient echo images and thus apparent decrease in T2* that can confound the underlying biology. Furthermore, the specificity of T2* contrast to myelin content is hampered by fiber orientation in the white matter (Lee et al., 2011) and in the cortex (Cohen-Adad et al., 2012), tissue iron level (Lee et al., 2012; Stüber et al., 2014), blood vessels (Spees et al., 2001), blood oxygen level (Li et al., 1998). Note that in this study, the effect of blood vessel was minimized by excluding large blood vessels using manual masks. Also, capillary blood should only contribute minimally to the T2* contrast, as reported by Lee et al. (Lee et al., 2012).
Combining MTR and T2* using ICA
The main goal of this study was to gain specificity in myelin mapping by combining T2* and MTR. Here, ICA decomposition was chosen to extract shared information between MTR and T2* that represents myelin content. The ICA offers the advantage of recovering sources of interest (here: myelin content) from observed mixtures, making it well suited for the brain data analysis because of the multifaceted origin of MTR and T2* contrasts. Here we used the fast-fixed point algorithm presented by Hyvärinen et al (Bingham and Hyvärinen, 2000). This algorithm transforms the observed data to the linear combination of source signals (or independent components) which are non-gaussian and mutually independent. The output of the ICA is a separating matrix, which is represented by two vectors defining a new basis of independent components. Results of the ICA on our MTR and T2* data showed a fairly low inter-subject variability of the directions of the first vector (58±4°), which is assumed to represent myelin content. This low variability suggests stability of the decomposition process with respect to the spatial distribution of myelin-related source. Note that the current ICA framework is modular and the model would benefit from complementary sources of contrast sensitive to myelin content, such as T1 (Bock et al., 2009; Dinse et al., 2013; Sereno, 1991), T1w/T2w (Glasser and Van Essen, 2011), phase images (He and Yablonskiy, 2009) and diffusion data. While adding more metrics will likely increase the sensitivity and specificity to myelin, it is important to keep in mind that some metrics can share variance due to a shared MR contrast mechanism and/or artifactual contribution. For example, MTR contrast is partly driven by T1. In this study we chose to acquire T2* and MTR. The rationale behind acquiring these two contrasts was to show a proof-of-concept for combining two myelin mapping techniques with very different biophysical properties: susceptibility-related effect for T2* and macromolecular-related magnetization transfer effect for MTR.
Interpretations of the combined myelin estimation (CME) maps
The CME exhibited high values (>70%) in the primary motor cortex (BA4), in the primary somatosensory cortex (BA1, BA2 and BA3), in the visual cortex (BA17 & BA18) and in the auditory cortex (BA42). Contrariwise, the insula, the frontal and prefrontal cortex (BA8, BA9 & BA10) and the anterior cingulate cortex (BA24 & BA32) have low CME values (<30%). Seen as an indicator of myelin content, this pattern of CME across the cortex is in concordance with previous cortical myelin-oriented studies (Annese et al., 2004; Glasser and Van Essen, 2011; Glasser et al., 2014; Laule et al., 2008; Nieuwenhuys, 2013; Vogt, 1911). Moreover, the intra-regional standard deviation of the CME is low in comparison to that across the whole cortex. This suggests a fairly homogenous myelin estimate inside the putative cortical areas. This observation is consistent with previous studies showing homogeneous myeloarchitecture within functionally-defined areas. (Abdollahi et al., 2014; Bock et al., 2009; Geyer and Turner, 2013; Glasser and Van Essen, 2011; Glasser et al., 2014; Nieuwenhuys, 2013; Sereno, 1991).
The CME map was compared with existing myelin-related maps from the literature. The MR longitudinal relaxation time T1 has been shown to be closely related to myelin content in vivo (Dick et al., 2012; Koenig et al., 1990; Sigalovsky et al., 2006) and ex vivo (Mottershead et al., 2003; Schmierer et al., 2008, 2004) showing for example high correlation (r = 0.89) between T1 relaxation time and myelin content in fixed brain (Schmierer et al., 2008). Recently, (Sereno et al., 2013) have computed high resolution quantitative R1 (inverse of T1) maps from PDw and T1w images according to the formalism developed by Helms et al. (2008) and including a correction for imperfect RF spoiling (Preibisch and Deichmann, 2009) in order to obtain an accurate estimation of the cortical myelin content. Moreover, the ratio between T1w and T2w images has been shown to be an accurate estimate of the relative myelin content across cortex (Glasser and Van Essen, 2011; Glasser et al., 2014). Glasser et al. (2014) have demonstrated that T1w/T2w maps reveals an observer-independent map of the area boundaries for dozens of cortical areas in a population-average analysis. Figure 11 shows a side-by-side comparison between our CME maps and the cortical myelin estimations based on T1w/T2w from Glasser et al. (Glasser and Van Essen, 2011; Glasser et al., 2014) and R1 (inverse of T1) contrast from Sereno et al. (Sereno et al., 2013). Strong similarities are observed across maps, notably high myelin indices in the motor, visual and auditory cortices and low myelin indices in the anterior frontal cortex and in the temporal cortex. Small details are also shared by all contrasts, for example the middle-high spot located in the frontal lobe of the left hemisphere (green circle), the middle-high spot in the superior temporal cortex of the right hemisphere (green circle) and the bright spot in the lateral occipital cortex (near BA19). More interestingly, some discrepancies are observed for the CME map (red circles), i.e. regions of strong contrast previously not seen in other metrics. For example, we can observe a stronger signal in CME maps than in R1 or T1w/T2w maps in the pars triangularis area (dashed-red circle, near BA47) and in the superior parietal area (red circle, near BA7). Further work is needed to validate these findings with histology.
We chose to analyse our data with respect to cortical parcellation offered by the PALS-B12 atlas, which aims at representing homogeneous cytoarchitecture within the human cortex as proposed by Brodmann (Brodmann, 1909). Borders of these regions are defined by the variation of the cells organization and structure of the cortex and are thought to represent functional units (Barbier et al., 2002; Jacot-Descombes et al., 2012; Lanzilotto et al., 2013). In analogy to the present study, we observe that regions representing specific functions of the human body (primary motor, auditory, visual) overlap with regions where CME was high. However, there is not necessarily a direct correspondence between myelo- and cyto-architecture (Geyer et al., 2011). Other atlases are available in the literature, notably the myeloarchitectonic atlas of Nieuwenhuys et al. (Nieuwenhuys et al. 2014), which divides the cortex into 180 myeloarchitectonic areas. A qualitative side-by-side comparison revealed some similarities between this atlas and the CME map. For example, in the pars triangularis region the bright spot visible in CME map only (dashed-red circle in Figure 11C) seems to overlap with area 57–58 in the Nieuwenhuys atlas (red circle in Supplementary material S3). We notice that this bright spot is in accordance with a previous ex vivo monkey histology (Cruz-Rizzolo et al., 2011). Moreover, the motor cortex in the CME map exhibits a multiple-line pattern along the central sulcus, which is also visible in the Nieuwenhuys atlas. Moreover, the motor cortex in the CME map exhibits a multiple-line pattern along the central sulcus, which is also visible in the Nieuwenhuys atlas.
It should be noted that CME is currently not calibrated on true myelin values. CME’s limits (0% to 100%) were defined based on regions with qualitatively low and high myelin content (Annese et al., 2004; Glasser and Van Essen, 2011; Glasser et al., 2014; Laule et al., 2008; Nieuwenhuys, 2013; Vogt, 1911). Such a calibration procedure is challenging because ex vivo measures of myelin content may not be accurate for in vivo assessment. Histology and immunohistochemistry techniques may suffer from non-uniformity (Cruz-Rizzolo et al., 2011; Culling, 2013). Moreover, optical density measurements of the stain do not provide an accurate measure of myelin density because it does not probe the quantity of myelin in a slice (Culling, 2013). (Stüber et al., 2014) introduced the PIXE technique recently using complex experimental setup. Furthermore, MR parameters change post mortem due to fixation. For instance, the correlation of MTR with myelin content is much stronger before fixation (Schmierer et al., 2008). Moreover, image registration is not easy in such studies, and spatial sampling is limited. Finally, more knowledge is required about the relationship between CME and true myelin content. For example, here we assumed linearity, but this has to be verified before calibration procedure.
Concerning the fiber orientation dependency, we are aware that various models have been proposed in the literature. For example, (Bender and Klose, 2010; Denk et al., 2011) have shown that the fiber orientation dependence can be well described using the term sin(theta)^2. We have therefore compared our model with the sin(theta)^2 model. Results were similar, with a square difference (averaged across all vertices) of 0.32 %2 for ME_MTR and 0.11 %2 for ME_T2*.
The correlations with histological work of Braitenberg (Braitenberg, 1962) suggest that CME is a more specific marker for cortical myelin content compared to ME_MTR or ME_T2* taken separately. We have also shown that ME_MTR and ME_T2* are more specific markers of myelin than MTR and T2* (see Figure 8). This type of comparison is however limited by several factors. Firstly, the Braitenberg dataset was only limited to a few regions. Secondly, the study of Braitenberg was hampered by imperfect tissue fixation and staining, which added potential biases in the measures.
Limitations and futures studies
T2* volumes were acquired with anisotropic voxels in order to maintain a high in-plane resolution (0.3×0.3 mm). Anisotropic voxels are subject to more inhomogeneous partial volume effect during the cortical sampling. In the future, EPI-Based multi-echo measurements (Zwanenburg et al., 2011) may sufficiently accelerate acquisition to allow use of isotropic voxels. MTR volumes were acquired with isotropic voxels, despite a somewhat low resolution (1.2mm) in comparison with the thickness of the cortex. Future studies could benefit from MT-prepared multi-echo EPI (Helms and Hagberg, 2005) in order to acquire faster MT-weighted images and potentially increase the spatial resolution thanks to the higher SNR efficiency of EPI sequences. However it is important to keep in mind that EPI measurement suffers from geometric distortions, which are difficult to perfectly correct using standard approaches (fieldmap-based or non-rigid alignment). Residual distortions would lead to imperfect registration to the cortical surface and hence lead to potentially wrong values when sampling along the cortical ribbon.
The MMEM used a normalization procedure based on regions that are known to be highly and poorly myelinated. Thus, the output of the MMEM does not give an absolute measure of myelin content, but rather an indicator of relative level of myelin compared to other brain areas. Furthermore, it could be argued the choice of regions for normalization purpose was not adequate, however the robustness of the resulting MMEM coefficients was fairly high. For example, when using only BA4 (high myelin) and BA9 (low myelin), the resulting coefficients were less than 1% different compared to the results presented in this study.
Validation is essential to these types of MRI studies. Although CME maps showed remarkably high spatial correspondence with previous in vivo and postmortem studies (Annese et al., 2004; Glasser and Van Essen, 2011; Glasser et al., 2014; Laule et al., 2008; Nieuwenhuys, 2013; Vogt, 1911) it remains essential to further compare MRI maps with full cortex histology samples stained for myelin. However, limitations exist with histological staining, as it does not necessarily represent quantitative measure of myelin content and is hampered by the attachment properties of the tissue (depends on preparation, fixation, etc.) (Jain et al., 1998; Pistorio et al., 2006).
The multivariate myelin estimation model has the potential to be useful in assessing early cortical changes in myelin in patients with neurodegenerative diseases such as multiple sclerosis.
Supplementary Material
Acknowledgments
We thank Benjamin De Leener, Tanguy Duval, Simon Lévy, Blanche Perraud, Nikola Stikov and Yves Goussard (Polytechnique Montreal), Pierre Bellec (Université de Montréal), Céline Louapre and Costanza Giannì (A. A. Martinos Center, Boston), Gaëlle Seret (Polytechnique Paris) and Jérémie Pilon (Danone Research) for helpful discussions. This work was supported by the National Multiple Sclerosis Society [FG 1892A1/1, 4281-RG-A-1], by the National Center for Research Resources [P41-RR14075], the Fonds de Recherche du Québec – Santé (FRQS), the Fonds de Recherche du Québec – Nature et Technologies (2015-PR-182754), the Quebec BioImaging Network (QBIN), the Natural Sciences and Engineering Research Council of Canada (NSERC) and the Polytechnique MEDITIS program.
Footnotes
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