Abstract
16
In Pang, Aquino et al. (2023)1, we presented multiple lines of evidence to indicate that brain 17
geometry plays a previously under-appreciated role in shaping dynamics. Mansour et al. raise 18
concerns about one specific analysis, in which we showed that eigenmodes derived from the 19
geometry of the human cortex can reconstruct diverse activity maps generated with functional 20
magnetic resonance imaging (fMRI) better than eigenmodes derived from connectomes 21
estimated with diffusion MRI (dMRI). Here, we address their concerns and show how our 22
findings and conclusions remain valid. 23
24
Introduction
25
Mansour et al. motivate their work by claiming that our findings have “been widely interpreted 26
to mean that geometry imposes stronger constraints on cortical dynamics than connectivity”. 27
This interpretation rests on an artificial and inaccurate dichotomy between brain geometry and 28
connectivity, as detailed in the extensive supplementary material (Section S8) of our original 29
article1 showing the precise mathematical relation between geometry and connectivity, and our 30
follow-up piece further explaining why the dichotomy is incorrect2. To clarify, geometric 31
eigenmodes assume a specific form of connectivity in which cortical locations are coupled 32
through an isotropic, distance-dependent kernel, such that connectivity between any two points 33
decays as an approximately exponential function of their physical separation. This assumption 34
follows the well-known exponential distance rule (EDR) demonstrated empirically to dominate 35
the connectomes of diverse species3–8. Geometric eigenmodes thus account for the effects of 36
both cortical geometry and EDR-like connectivity. In contrast, connectome eigenmodes do not 37
directly account for geometry. Connectomes are dominated by EDR-like connectivity4,9, but 38
they also account for the effects of topologically complex connections that are not incorporated 39
in an EDR approximation4,10. 40
41
The stronger performance of geometric eigenmodes in our original analysis1 indicated that 42
geometric eigenmodes, and the connectivity approximation that they entail, are sufficient to 43
account for diverse fMRI activity maps, despite the simplicity of the model. We thus concluded 44
that geometric eigenmodes “provide a more compact, accurate, and parsimonious 45
.CC-BY-NC-ND 4.0 International licensemade available under a
(which was not certified by peer review) is the author/funder, who has granted bioRxiv a license to display the preprint in perpetuity. It is
The copyright holder for this preprintthis version posted August 23, 2024. ; https://doi.org/10.1101/2024.08.21.608487doi: bioRxiv preprint
2
representation of [the brain’s] macroscale activity than alternative connectome-based models” 46
and that “the comparatively poor performance of connectome eigenmodes indicates that 47
topologically complex connections that exist beyond a simple EDR afford minimal further 48
benefit in obtaining eigenmodes that can accurately explain spatiotemporal patterns of cortical 49
activity as measured with fMRI” (p572)1. 50
51
Mansour et al. focus almost exclusively on our specific comment about the “comparative 52
performance of connectome eigenmodes”, citing it multiple times. They report a thorough set 53
of analyses to address this “comparatively poor performance” by showing that, when dMRI 54
data are processed using a specific pipeline of “state-of-the-art connectome reconstruction 55
techniques”, the accuracy of the connectome and geometric models becomes approximately 56
equal. We applaud their efforts to identify a dMRI processing regime that improves the 57
accuracy of the connectome model. However, we disagree with their conclusion that the 58
“evidence presented to support the comparative proposition that “eigenmodes derived from 59
brain geometry represent a more fundamental anatomical constraint on dynamics than the 60
connectome” may require reconsideration.” Below, we explain why their findings only 61
strengthen our original claims. 62
63
Geometric eigenmodes are more parsimonious than connectome eigenmodes 64
Mansour et al. consider five dMRI processing steps that can mitigate “biases and inaccuracies” 65
associated with “high-resolution connectome mapping ”. Each of these steps requires 66
investigator-dependent choices between alternative approaches that substantially influence 67
connectivity estimates and model accuracy, as thoroughly detailed in Mansour et al.’s 10 multi-68
panel supplementary figures (their Figs. S1–10). For instance, their two different methods for 69
gyral bias correction yield connectomes with quite different architectures (Figs. 1–2 and their 70
Fig. S1), neither of which completely address the gyral bias that was suggested to contaminate 71
our original connectome (Fig. 2b). This simple methodological variation is sufficient to reduce 72
the correlation between the two resulting connectivity matrices to 0.46, despite the source data 73
being otherwise identical. This major discrepancy in connectivity weights, caused by a single 74
processing choice, underscores the fragility of the resulting connectomes (as suggested in our 75
own original analysis1) and poses a difficult challenge for the construction of a reliable basis 76
set, particularly given the priority that Mansour et al. assign to the analysis of weighted 77
connectomes. 78
79
Notably, this critical choice of gyral bias correction is only one in a sequence of decisions 80
required in their connectome reconstruction pipeline. These decisions yield a parameter space 81
comprising many plausible processing steps that can result in very different connectomes11,12. 82
It is difficult to ascertain how one should choose between these different processing options. 83
Mansour et al. use the geometric eigenmodes as a benchmark for optimizing their set of 84
choices. This approach is vulnerable to overfitting the data to obtain a desired result. It is 85
unclear how well this optimized set of choices generalizes to independent data. 86
87
Geometric eigenmodes obviate the need to navigate this analytic “garden of forking paths ”. 88
They are derived using robust and widely accepted pipelines for reconstructing cortical 89
surfaces from T1-weighted scans13. In fact, the end point of the geometric eigenmode pipeline 90
is the starting point of the connectome eigenmode pipeline, which requires acquisition of an 91
additional MRI modality and the construction of a complex sequence of processing steps based 92
on numerous choices. Mansour et al.’s analysis shows that, at best, a specific subset of these 93
choices yields a basis set that matches, but never substantially surpasses, the accuracy of the 94
geometric eigenmodes (their Figs 1, S2, S4–10, and S12). The fact that equivalent performance 95
.CC-BY-NC-ND 4.0 International licensemade available under a
(which was not certified by peer review) is the author/funder, who has granted bioRxiv a license to display the preprint in perpetuity. It is
The copyright holder for this preprintthis version posted August 23, 2024. ; https://doi.org/10.1101/2024.08.21.608487doi: bioRxiv preprint
3
is the best result for the connectome approach, despite the large parameter space explored by 96
Mansour et al., is strong evidence for the superior parsimony of the geometric basis set. Their 97
analysis thus strengthens our conclusion that geometric eigenmodes offer a sufficient and 98
parsimonious account of fMRI data . Future innovations in dMRI processing may further 99
improve the performance of connectome eigenmodes, but the gain in model performance 100
should be of a sufficient magnitude to justify the added complexity and problematic reliability 101
of the connectome model. 102
103
Topologically complex connections make a negligible contribution to reconstruction 104
accuracy 105
The ability to account for the specificity of brain connectivity, and particularly of the 106
topologically complex, often long-range, connections that cannot be explained by an EDR , is 107
the primary motivation for using connectome eigenmodes. However, Mansour et al.’s own 108
findings show that removal of longer-range connections (i.e., >16 mm) has a minimal effect on 109
the reconstruction accuracy of connectome eigenmodes, whereas removal of short -range 110
connections has a much larger impact (their Fig. S12). This result, when taken with their finding 111
of approximately equivalent performance of the geometric and “state-of-the art” connectome 112
eigenmodes, strengthens our original claim that an isotropic, EDR -like connectivity 113
approximation is sufficient to reconstruct diverse activity patterns mapped with fMRI and that 114
topologically complex connectivity (i.e., connectivity not readily captured by an EDR -like 115
approximation) makes a minimal contribution. Mansour et al.’s demonstration that removal of 116
short-range connections has a larger impact on reconstruction accuracy also supports our 117
original claim that local, short -range connections, which facilitate continuous propagation of 118
waves of excitation through the cortex, are important for understanding fMRI activity1. As we 119
acknowledged in our original article 1, topologically complex connections undoubtedly play 120
important roles for brain function but their effects may not be easily revealed by traditional 121
fMRI paradigms. 122
123
“State-of-the-art” dMRI processing increases the similarity between connectome and 124
geometric eigenmodes 125
If long-range connections make a negligible contribution to model accuracy, what drives the 126
performance improvement of “state-of-the-art” connectome eigenmodes? The answer to this 127
question is found in Figs 2 and S11b of Mansour et al., which show that their processing 128
strategy increases the alignment of the connectome eigenmodes to the geometric eigenmodes. 129
This increased similarity occurs because their additional processing steps accentuate the local 130
homogeneity and EDR -like dependence of the connectome ––the two key elements of the 131
connectivity approximation upon which the geometric approach relies. For instance, their Figs 132
S3f–g show how local homogeneity and the EDR dependence are dramatically enhanced by 133
connectome spatial smoothing. In Fig. 3a, we additionally demonstrate that their gyral bias 134
correction truncates the tails of the vertex connectivity strength distribution relative to the 135
uncorrected case, yielding an approximately Gaussian shape in which there is a low probability 136
of finding vertices with substantially higher or lower connectivity than the mean . Thus, 137
regardless of any debate over whether gyral bias correction improves the biological plausibility 138
of vertex -wise connectivity estimates, it ultimately increases the homogeneity of those 139
estimates. Figure 3b also shows that the processing steps applied by Mansour et al. exaggerate 140
the distance-dependent decay of connectivity edge weight s by attenuating precisely those 141
longer-range connections that deviate from an EDR footprint (see also Fig. 1b). 142
143
These considerations indicate that the performance of connectome eigenmodes approaches 144
geometric eigenmodes when the former are made to look like the latter . This is done through 145
.CC-BY-NC-ND 4.0 International licensemade available under a
(which was not certified by peer review) is the author/funder, who has granted bioRxiv a license to display the preprint in perpetuity. It is
The copyright holder for this preprintthis version posted August 23, 2024. ; https://doi.org/10.1101/2024.08.21.608487doi: bioRxiv preprint
4
data processing steps that increase the convergence between empirical connectivity estimates 146
and the isotropic, EDR-like connectivity approximation that underpins the geometric model. 147
The findings of Mansour et al. thus align with our original results and support the fundamental 148
role of geometric eigenmodes and the connectivity approximation that they entail in shaping 149
fMRI activity maps. 150
151
Conclusions
152
Mansour et al. show that: (i) best-estimate connectome eigenmodes only ever match, but never 153
substantially surpass, the reconstruction accuracy of the geometric model ; (ii) long-range 154
connections make a minimal contribution to the performance of the connectome model ; and 155
(iii) the performance improvements of the connectome model are attributable to processing 156
steps that increase the similarity between empirical connectome s and the connectivity 157
approximation inherent in the geometric approach. These findings beg the question: why use 158
the more complex connectome model if it offers little added value beyond the simpler 159
geometric approach? 160
161
The answer to this question depends on the goals of the investigator, since both geometric and 162
connectome eigenmodes have distinct strengths and limitations. Geometric eigenmodes offer 163
a simple and parsimonious account of brain function as they are formally linked with the 164
biophysical model of dynamics provided by neural field theory 14–17. This link allows one to 165
associate each eigenmode with characteristic spatial and temporal frequencies, which can be 166
used to understand how different types of stimuli drive cortical dynamics18. However, a 167
Limitation
of the geometric approach is that it is not straightforward to integrate cortical and 168
subcortical eigenmodes into a single model. Connectome eigenmodes can account for both 169
cortical and subcortical connectivity and facilitate mappings between specific eigenmodes and 170
task activation patterns in specific circumstances (see Fig . S13 of Mansour et al.). However, 171
connectome eigenmodes are susceptible to myriad data processing choices and include 172
overlapping contributions from topologically complex connections , EDR -like connectivity, 173
and geometry that can be difficult to disentangle without additional analysis. Future work will 174
benefit from understanding the strengths and limitations of the two approaches, and developing 175
approaches to unify them. 176
177
178
Figure 1. Original Pang, Aquino et al. and reprocessed Mansour et al. connectomes . (a) Panels from 179
left to right show the original connectome used in our work , our connectome after performing Mansour et 180
al.’s gyral bias correction via regression, and the connectome preferred by Mansour et al. (b) Same as panel 181
.CC-BY-NC-ND 4.0 International licensemade available under a
(which was not certified by peer review) is the author/funder, who has granted bioRxiv a license to display the preprint in perpetuity. It is
The copyright holder for this preprintthis version posted August 23, 2024. ; https://doi.org/10.1101/2024.08.21.608487doi: bioRxiv preprint
5
a but the vertices are reordered according to their spatial locations from posterior to anterior. This reordering 182
shows how the connectome preferred by Mansour et al. attenuates long-range connectivity, thus converging 183
on the distance-dependent connectivity approximation inherent in the geometric approach. 184
185
186
Figure 2. Spatial maps of v ertex-level connectivity strength s for the original and reprocessed 187
connectomes. (a) Spatial map of the vertex connectivity strengths as depicted by Mansour et al. (b) Same 188
as panel a but the values are zscored , which attenuates the effect of outlying values and allows a clearer 189
visualization of the spatial structure in the map. For panels a and b, panels from left to right show results 190
using our original connectome, our connectome after performing Mansour et al.’s gyral bias correction via 191
regression, and Mansour et al.’s preferred connectome. Panel b clearly shows that gyral bias is still 192
evident in the reprocessed connectomes and that the two correction strategies by Mansour et al. can lead 193
to highly divergent maps . These visualizations are preferable to the regression slopes and linear 194
correlations shown in Fig. S1b of Mansour et al., which will be biased by the outliers, heteroscedasticity, 195
and non -monotonicity evident in their scatterplots of the association between vertex connectivity 196
strength and curvature. 197
198
199
Figure 3. Vertex connectivity strength distributions and edge weight distance-dependencies for the 200
original and reprocessed connectomes. (a) Distribution of vertex connectivity strengths. (b) Edge weight 201
vs euclidean distance between vertices in semilogarithmic scale. For panels a and b, left to right shows results 202
using our original connectome, our connectome after performing Mansour et al.’s gyral bias correction via 203
regression, and Mansour et al.’s preferred connectome. The processing steps proposed by Mansour et al. 204
truncate the tails of the vertex connectivity strength distribution (panel a ) and attenuate the weights of 205
.CC-BY-NC-ND 4.0 International licensemade available under a
(which was not certified by peer review) is the author/funder, who has granted bioRxiv a license to display the preprint in perpetuity. It is
The copyright holder for this preprintthis version posted August 23, 2024. ; https://doi.org/10.1101/2024.08.21.608487doi: bioRxiv preprint
6
medium-to-long-range connections (between 50 and 100 mm) (panel b; see red arrows ). The processing 206
steps of Mansour et al. thus enforce a structure on the empirical data that more closely resembles the locally 207
isotropic, EDR-like connectivity approximation of the geometric model. 208
209
References
210
1. Pang, J. C. et al. Geometric constraints on human brain function. Nature 618, 566–574 211
(2023). 212
2. Pang, J. C. et al. Reply to: Commentary on Pang et al. (2023) Nature. 2023.10.06.560797 213
Preprint at https://doi.org/10.1101/2023.10.06.560797 (2023). 214
3. Henderson, J. A. & Robinson, P. A. Relations between the geometry of cortical gyrification 215
and white-matter network architecture. Brain Connectivity 4, 112–130 (2014). 216
4. Roberts, J. A. et al. The contribution of geometry to the human connectome. NeuroImage 217
124, 379–393 (2016). 218
5. Wang, X. J. & Kennedy, H. Brain structure and dynamics across scales: In search of rules. 219
Current Opinion in Neurobiology 37, 92–98 (2016). 220
6. Horvát, S. et al. Spatial Embedding and Wiring Cost Constrain the Functional Layout of 221
the Cortical Network of Rodents and Primates. PLOS Biology 14, e1002512 (2016). 222
7. Ercsey-Ravasz, M. et al. A Predictive Network Model of Cerebral Cortical Connectivity 223
Based on a Distance Rule. Neuron 80, 184–197 (2013). 224
8. Knoblauch, K., Ercsey-Ravasz, M., Kennedy, H. & Toroczkai, Z. The Brain in Space. in 225
Micro-, Meso- and Macro-Connectomics of the Brain (eds. Kennedy, H., Van Essen, D. C. 226
& Christen, Y .) 45–74 (Springer International Publishing, Cham, 2016). doi:10.1007/978-227
3-319-27777-6_5. 228
9. Theodoni, P. et al. Structural Attributes and Principles of the Neocortical Connectome in 229
the Marmoset Monkey. Cerebral Cortex 32, 15–28 (2022). 230
10. Betzel, R. F. et al. Generative models of the human connectome. NeuroImage 124, 231
1054–1064 (2016). 232
11. Oldham, S. et al. The efficacy of different preprocessing steps in reducing motion-233
related confounds in diffusion MRI connectomics. NeuroImage 222, 117252 (2020). 234
12. Gajwani, M. et al. Can hubs of the human connectome be identified consistently with 235
diffusion MRI? Network Neuroscience 1–25 (2023) doi:10.1162/netn_a_00324. 236
13. Fischl, B. FreeSurfer. NeuroImage 62, 774–781 (2012). 237
14. Robinson, P. A., Rennie, C. J. & Wright, J. J. Propagation and stability of waves of 238
electrical activity in the cerebral cortex. Physical Review E 56, 826–840 (1997). 239
15. Robinson, P. A. et al. Prediction of electroencephalographic spectra from 240
neurophysiology. Physical Review E 63, 021903 (2001). 241
16. Jirsa, V . & Haken, H. Field Theory of Electromagnetic Brain Activity. Physical 242
Review Letters 77, 960–963 (1996). 243
17. Wright, J. J. & Liley, D. T. J. Simulation of electrocortical waves. Biological 244
Cybernetics 72, 347–356 (1995). 245
18. Gabay, N. C., Babaie-Janvier, T. & Robinson, P. A. Dynamics of cortical activity 246
eigenmodes including standing, traveling, and rotating waves. Phys. Rev. E 98, 042413 247
(2018). 248
249
.CC-BY-NC-ND 4.0 International licensemade available under a
(which was not certified by peer review) is the author/funder, who has granted bioRxiv a license to display the preprint in perpetuity. It is
The copyright holder for this preprintthis version posted August 23, 2024. ; https://doi.org/10.1101/2024.08.21.608487doi: bioRxiv preprint
Text is read by the "Ask this paper" AI Q&A widget below.
Extraction quality varies by source — PMC NXML preserves structure
cleanly, OA-HTML may include some navigation residue, and OA-PDF can
have broken hyphenation. The publisher copy
(via DOI)
is the canonical version.