Keywords
Neural communication, Functional connectivity, MEG, connectome 15
16
Abstract
17
Tracking signal propagation in nervous systems is crucial to our understanding of brain 18
function and information processing. Current methods for inferring neural communication 19
track patterns of sustained co-activation over time, making them unsuitable to detect discrete 20
instances of signal transmission. Here, we propose Event-marked Windowed Communication 21
(EWC), a new analytical framework to infer functional interactions arising from discrete 22
signalling events between neural elements, in otherwise continuous time series data. In 23
contrast to conventional measures of functional connectivity, our method utilises an event-24
based subsampling of neural time series, which allows it to capture the statistical analogue 25
of activity propagation. We test EWC on simulations of neural dynamics and show that it is 26
capable of retrieving ground truth motifs of directional signalling , over a range of model 27
configurations. Critically, we demonstrate that EWC’s subsampling approach affords profound 28
reductions in computation times, compared to established network inference methods such 29
as transfer entropy. Lastly, we showcase the utility of EWC to infer whole -brain functional 30
networks from MEG recordings. Networks computed using EWC and transfer entropy were 31
highly correlated (median r=0.821 across subjects), but EWC inference was approximately 6.5 32
times faster per epoch. In summary, our work presents a new method to infer signalling from 33
time series of neural activity at low computational costs. Our framework is flexible and can be 34
applied to activity time series captured by diverse functional neuroimaging modalities, 35
opening up new avenues for the study of neural communication. 36
37
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Madan Mohan et al., 2024 2
Introduction
38
Communication between neural elements — neurons, neural populations and grey matter 39
regions, plays a central role in the functioning of the brain. Understanding the principles by 40
which signals are dynamically and flexibly transmitted in networked nervous systems remains 41
an open challenge and active area of research 1–3. Efforts in this direction have produced a 42
vast number of models of brain communication 1,4,5, ranging from information transfer via 43
neural oscillations6–10 to network measures of connectome communication 11–13. Despite the 44
abundance in models, efforts in model validation have been lacking, and it remains unclear 45
which methods faithfully describe empirical patterns of neural dynamics and signalling. A key 46
barrier to progress in model validation is our current inability to infer events of signal 47
transmission from recordings of neural activity. 48
49
Functional connectivity (FC) is commonly used as a proxy for neural communication. Broadly 50
defined, FC quantifies statistical dependencies in time series of neural activity using measures 51
such as the Pearson correlation or Mutual Information , capturing the extent to which the 52
dynamics of two brain regions are synchronised over a period of time. FC estimation has been 53
extensively used in model formulation and validation as well as in experimental and clinical 54
studies3,14–24. While useful, these FC measures are limited to capturing stable, sustained 55
statistical associations over time, which can dilute or mask discrete events of directional signal 56
transmission from one neural element to another. Information -theoretical measures such as 57
Transfer Entropy stand to address this issue, but are typically data - and computation-heavy 58
for whole-brain network inference25. 59
60
Explicitly tracking how activity (endogenous/exogenous perturbations) or signals propagate 61
across the underlying anatomical substrate can provide important insights into the principles 62
of inter-areal communication and help validate existing computational models . Current 63
Limitations
in neuroimaging technology have seen activity propagation tracing often applied 64
to smaller controlled stimulation experiments in microscale neuronal networks 26–28. Its 65
application at the w hole-brain scale is still limited 29–32, although approaches combining 66
existing data to yield robust insights seem to show promise33. In this work, our aim was to 67
develop an efficient method of inferring activity propagation patterns by combining the 68
practicality and efficiency of undirected FC estimation with the dynamical resolution afforded 69
by activity propagation tracing. We term this modified FC estimation protocol Event-marked 70
Windowed Communication (EWC ). Specifically, EWC involves identif ying salient events in 71
neural recordings (“stimuli”) and the subsequent estimation of FC within short temporally 72
ordered windows/subsamples of the signal. In this manner, EWC captures an indirect 73
statistical analogue of activity propagation as opposed to spatiotemporally localised 74
stimulation-response measurements. We first validate and demonstrate the utility of the EWC 75
implementation using a simple in-silico network motif with ground truth signalling embedded 76
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Madan Mohan et al., 2024 3
in its dynamics. We also show that the EWC approach allows us to use undirected FC 77
measures to capture directional interactions. We then study the computational tractability of 78
the approach by comparing network inference runtimes as a function of number of nodes. 79
Finally, we demonstrate a real-world application of the method on source -localised resting-80
state magnetoencephalography (MEG) recordings. 81
82
Results
83
84
Figure 1 – A pipeline to es1mate communica1on pa5erns from regional 1me series. (A) Regional ac1vi1es are divided into 10 85
second epochs, and each epoch is processed independently. (B) For each epoch, the regional ac1vi1es are z-scored to iden1fy 86
instances of devia1on from mean behaviour, which are termed “supra-threshold events”. (C) Each region is successively chosen 87
as a “source”. For each event of a source, a communica1on window that encompasses the ac1vity over a dura1on of 1 second, 88
is defined star1ng at the 1me point of the event. Similar communica1on windows are defined over the ac1vi1es of all other 89
regions (termed “targets”), star1ng at 1mepoints delayed with respect to the source event, in propor1on to the Euclidean 90
distance between the source and target. (D) For each event for a chosen source, the Event-marked Windowed Communica1on 91
(EWC) is es1mated between the source and all possible targets by compu1ng the condi1onal mutual informa1on between 92
the ac1vi1es contained in the communica1on windows of the source and target. The ac1vity of the target over 1 second in 93
the past is used as the condi1oning variable . The pairwise EWC values over all events of a source (within an epoch) are 94
averaged, to populate a row of the EWC matrix corresponding to the source index. Steps B-D are repeated over all epochs to 95
give epoch-level EWC matrices that capture the dynamic communica1on pa5erns over the en1re scan dura1on. 96
In this study, we develop a new method to quantify functional interactions between neural 97
elements based on the detection of directional signalling events in their activity time series 98
(Fig.1). The Event-marked Windowed Communication (EWC) protocol is composed of 3 main 99
elements: 1) Event -identification 2) Temporal ordering based on conduction delays, and 3) 100
Windowing or subsampling. Specifically, our approach involves first identifying significant 101
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Madan Mohan et al., 2024 4
deviations from the mean of activity time series, which we term “supra-threshold events” (For 102
brevity, we will refer to them as “events” for the remainder of this paper). We then trace the 103
downstream effects of these events on the activities of other neural elements , while 104
considering the possible delays in signal conduction due to inter -element distances. 105
Importantly, we restrict the estimation of communication to a short “communication window”, 106
that starts at the timepoint of an event, for the source, and at a future timepoint for the target 107
(proportional to the source-target distance). Once a communication window is specified, the 108
magnitude of the signalling event is quantified by the statistical association between the 109
within-window activity time series of the source and target . EWC is flexible and this 110
association can be computed using various measures of FC, such as the partial correlation or 111
Mutual Information. Lastly, we derive an aggregate communication measure by averaging the 112
FC across communication windows. 113
114
The analyses of this paper can be divided into three main sections. First, we tested our 115
Method
in simulated time series produced by a simple connectivity motif in which node 116
activity was governed by Linear Stochastic Model (LSM) dynamics (Fig 2A). The simple 117
dynamical landscape of the LSM allowed us to impose ground truth signalling between 118
nodes. We assessed our method’s ability to identify these communication patterns in relation 119
to previously proposed measures of FC. Second, we characterise gains in computational time 120
afforded by estimating FC using EWC. Third, we apply our method on source localised MEG 121
recordings, and gauge the agreement between the FC inferred v ia EWC and bivariate 122
Transfer Entropy. 123
In the remainder of the paper, we will use the suffix “-Full” after the FC measure to indicate 124
a conventional estimation technique using the entire signal, and “ -EWC” to indicate our 125
implementation. 126
127
Asymmetric signalling over a network mo tif 128
We tested the EWC protocol in a four-node motif with Linear Stochastic Model (LSM) 129
dynamics (Fig.3). Three of the nodes in this network were connected in a linear topology 130
(nodes 1, 2, and 3), whereas node 4 was isolated (i.e. not influenced by the dynamics of other 131
nodes). In addition to the LSM dynamics, the nodes 1, 3, and 4 also pulsated at random times 132
according to a Poisson process. These pulses emulated punctual events of directional 133
signalling, with known sources at nodes 1, 3, and 4. 134
135
EWC was implemented using two measures of within -window FC, partial correlation (PC -136
EWC) and conditional mutual information (cMI -EWC). Note that, traditionally, these are 137
symmetric measures that cannot resolve directionality of functional interactions. We 138
benchmarked EWC against Transfer Entropy (TE -Full), which was conventionally estimated 139
based on the entire time series. We compared the ability of these measures to retrieve the 140
ground truth signalling motif in simulations with increasing noise levels. To enable comparison 141
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Madan Mohan et al., 2024 5
of the different measures, we estimated the standardised contrast between the FC in true 142
(existing) and false (absent) connections. 143
144
Figure 2 - Communica1on over a network mo1f. (A) (inset) We test our method of es1ma1ng communica1on pa5erns on a 145
simple 3-node network mo1f with a linear topology and an isolated node (4 -cyan). The ac1vi1es of the individual nodes in 146
this network are described by a Linear Stochas1c Model. The dynamics of the red, blue and cyan nodes have an addi1onal 147
Poisson process, causing it to spike at an average rate of 0.2 Hz, emula1ng communica1on events. 𝛿xy is the delay between 148
nodes x and y, in ms. The noise amplitude of the LSM, s , is varied rela1ve to the fixed Poisson pulse amplitude of the sources. 149
(A) Transfer entropy (in nats) between nodes, es1mated over the full signal. (B) Condi1onal Mutual Informa1on (in nats) 150
between nodes, es1mated as per the EWC protocol (C) Par1al Correla1on (Pearson-R) between nodes, es1mated as per EWC. 151
We show only the absolute Pearson correla1on. (D -F) Standardised contrast (difference between EWC of True and False 152
connec1ons, normalised by their pooled standard devia1on) plots associated with the FC es1mates. A non-zero contrast value 153
indicates discriminability. Shading in the plots represent ±SEM (20 trials). All plots maximally smoothed (i.e. using all available 154
points) to clearly reveal trends. 155
156
We considered the performance of our method as a function of the ratio between the noise 157
level in the system and the amplitude at which the source regions pulsate. The delay between 158
the sources (nodes 1, 3, and 4 ) and the target ( node 2) was set at 15ms, and the sources 159
pulsated according to a Poisson process with a mean frequency of 0.2Hz (Fig.2A - inset). The 160
ground truth comprises connections from node 1 to node 2 and 3 to 2. We observed that 161
estimating the TE-Full resulted in a good representation of the ground truth, with strong 162
interactions from nodes 1 and 3 to 2 (Fig.2A). Importantly, the corresponding contrast 163
distribution indicated that the interaction between node 4 (isolated) and 2 could be clearly 164
discriminated from the true interactions , providing evidence of good specificity (Fig.2D). 165
When the FC was instead measured using cMI-EWC, we observe d an interaction between 166
regions 4 and 2 , although this false positive interaction was considerably weaker than the 167
ground truth interactions from node 1 to 2, and 3 to 2, particularly at low noise levels (Fig.2B). 168
Interestingly, PC-EWC performed well when compared to cMI -EWC. Like TE-Full, PC-EWC 169
also resulted in a good representation of the ground truth (Fig.2C). The contrast between 170
estimated interactions show ed that true connections could be distinguished from absent 171
Partial Correlation (EWC)
1
3
24 42
𝜎
𝜈 = 0.2Hz
= 15ms42==
A B C
D E F
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Madan Mohan et al., 2024 6
connections even at large levels of noise (Fig.2F), although not as well as TE-Full. Importantly, 172
in the case of cMI -EWC and PC-EWC, asymmetric interactions were estimated, despite the 173
FC measures being undirected/symmetric. This asymmetry is a result of the temporal ordering 174
within the EWC implementation. 175
176
Additionally, we also tested whether a common source equidistant from two targets would 177
Result
in a spurious functional link between them (a closed triangle problem). For this we set 178
region 2 as the pulsating source and estimated the PC-EWC. We observed that our method 179
correctly identifie d communication from node 2 to both 1 and 3, with negligible 180
communication in the opposite direction, or between the targets (Fig.S1). We also tested the 181
EWC implementation over a range of conduction delays, and mean firing rates of the sources 182
(Fig.S2). 183
184
To summarise, our comparative analyses demonstrate that EWC can accurately capture 185
directional interactions over a range of noise levels, delays, and firing rates. We emphasize 186
that PC and cMI, being undirected/symmetric measures, were only able to capture directional 187
signalling due to the temporal ordering implemented by the EWC protocol. Despite these 188
positive results, based on our observations of the standardised contrast, we find that TE-Full 189
still provides the strongest discriminability between the absence and presence of signall ing 190
patterns. For this reason, we continue using TE-Full as a representative benchmark of directed 191
FC in the subsequent analyses. 192
193
Computational tractability of the EWC protocol 194
In this section, we compared the computational tractability of the EWC protocol by 195
comparing full versions of TE and MI, and EWC versions of TE, cMI and the PC. We used 196
these methods to estimate functional networks comprising increasing number of nodes. 197
Nodal time series were sampled from source -localised MEG recordings (see Methods) . 198
199
As expected, the computation time increased with network size in all cases. The conventional 200
implementation of the TE was the most computationally intensive approach (Fig.3A), whereas 201
PC-EWC estimation required ≈75% less time relative to TE -Full. However, the EWC 202
implementation of TE was considerably quicker than the conventional approach and required 203
just as long as the cMI-EWC. Interestingly, MI estimated from the full signal requires less time 204
to compute than the closely related cMI -EWC. This is however due to an increase in the 205
number of computations in the EWC approach, as we will discuss later. 206
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Madan Mohan et al., 2024 7
207
Figure 3 –Time taken for network inference as a func1on of network size. Signals spanning 200s (Twenty 10s epochs) sampled 208
from source-localised MEG recordings of 3 subjects. Sampling repeated 10 1mes per subject for each network size (Each box 209
plot spanning 30 data points). Circles represent outliers. (Inset) Percentage of 1me taken to compute PC-EWC, rela1ve to the 210
1me taken to compute TE-Full. For a range of network sizes, PC -EWC takes ≈75% less 1me to compute for a 200s scan, or 211
equivalently, is ≈4 1mes faster. 212
213
In short, we find that both methods of estimation (Full or EWC) and the within-window EWC 214
FC measure affect computation time. Importantly, using the EWC protocol generally leads to 215
a decrease in computation time. In addition, the gain in computational time grows as a 216
function of network size, indicating that EWC may confer pronounced benefits for the 217
estimation fine-grained functional networks (e.g. >1000 nodes). Combined with our results 218
from the previous section, we find that PC -EWC can be computed ≈4 times faster than TE-219
Full, while also resolving asymmetries in signalling. 220
221
Inferring whole -brain interaction patterns from MEG recordings 222
Having compared both the accuracy and computational efficiency of the EWC to the 223
conventional approach in-silico, in our final set of analyses, we extended the comparison onto 224
empirical neuroimaging data . Specifically, we compute and compare PC -EWC and TE-Full 225
from resting-state source-localised MEG recordings of 30 subjects , for the left hemisphere 226
(right-hemisphere results Fig.S3). The temporal ordering was based on delays proportional 227
to the inter-regional Euclidean distance (see Methods). 228
229
For each subject, we computed the correlation between the PC -EWC and TE-Full matrices 230
and found that the two measures led to highly correlated estimates of functional connectivity 231
0
200
400
600
800
1000
1200
1400
1600Network inference time for a 200s recording (s)
3 10 20 50 100
N
TE-Full
cMI-EWC
TE-EWC
MI-Full
PC-EWC
-100
-80
-60
-40
-20
Relative time taken to compute PC-EWC
(% of time to compute TE-Full)
10 20
N
503 100
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Madan Mohan et al., 2024 8
(Fig 4B). The median correlation coefficient across subjects was r≈0.82 (p<0.0001) (Fig 4C 232
top). Critically, although PC-EWC and TE-Full were very similar, the EWC protocol offered a 233
speedup per epoch by a factor of ≈6.5 (Fig.4D bottom). In addition to the high subject-level 234
agreement, the EWC implementation also allows us to study how signalling directions and 235
strengths change across the scan, by estimating the degree of asymmetry and variance of 236
estimates at different scales (event-, epoch-, and subject-levels) (Fig.S4). 237
238
To summarise, in this section we demonstrate a real-world application of the EWC, using PC-239
EWC and TE-Full. We show that the FC estimated as per the EWC shows good agreement 240
with our conventional reference using the TE, and does so at a fraction of the computational 241
cost. This lends support to the EWC as a viable technique for practical applications , 242
particularly involving multiple functional components. 243
244
Figure 4 – Applica1on of EWC on source-localised MEG recordings. (A) Res1ng-state MEG scans of 30 subjects from the
Human Connectome Project (HCP) were pre-processed, source localised, orthogonalized, and epoched into 10 second
segments. (B) (Top) The subject-level FC for the leb hemisphere was es1mated as PC-EWC and TE-Full. (Bo5om) Edgewise
correla1on distribu1on between the subject-level FC matrices. The red line marks the median correla1on. (C) (Top)
Sca5erplot of edge weights for a representa1ve subject (closest to the median correla1on). Correla1on aber excluding
outliers (> 4 standard devia1on) - r≈0.82, p<0.0001. (Bo5om) inference 1me per epoch across subjects, for each of the
methods.
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Madan Mohan et al., 2024 9
Discussion
245
Understanding how the brain routes information is an open problem in neuroscience with 246
crucial implications to our knowledge of perception and cognition. In this work, we focus on 247
the first step to wards addressing this problem – reliably inferring communication from 248
neuroimaging data. We introduce a time series analytical technique, termed Event -marked 249
Windowed Communication (EWC), to capture dynamic statistical relationships driven by inter-250
regional communication. This method quantifies inter-regional relationships using functional 251
connectivity (FC) measures estimated on select subsamples of the signal. We demonstrated 252
the merits and limitations of this method in silico, using different FC measures, and compared 253
it to established methods of inferring directional relationships (Fig.2). We then applied it to 254
source-localised MEG data, where high correlation was evident between subject-level FC 255
patterns derived using EWC and conventional approaches (Fig.4). Importantly, we also 256
showed that the EWC protocol is computationally efficient (≈6.5 times faster per 10s-epoch 257
when using the PC ) (Fig.3,4C-bottom), and additionally capable of capturing changes in 258
asymmetric relationships over the scan (Fig.S4). 259
260
Studying how activity or information flows between neural elements is crucial to our 261
understanding of the mechanisms of communication. In addition to EWC, multiple previous 262
works have explored this important topic from diverse standpoints, such as neuronal 263
avalanches26,27,31, direct stimulation -response measurements 33, functional hierarchies 21, FC 264
dynamics32,34, and information -theoretic methods 25,35,36, to name a few. EWC differs from 265
previous work primarily in its handling of time series . As opposed to measures/features 266
computed using the entirety of recordings or parts of them (as in sliding window approaches), 267
EWC restricts FC estimation to select subsamples of the signal, to infer activity propagation 268
between neural elements. By targeting the FC estimation to select subsamples of the scan , 269
EWC effectively computes a resting-state “event-related potential ”. Importantly, being a 270
general and flexible framework, the EWC implementation can be easily incorporated into 271
previously developed methodologies involving neural time series e.g. using feature vectors 272
instead of raw time series35. 273
274
Estimating EWC comprises three steps: 1) event identification 2) temporal ordering 3) 275
windowing/subsampling. Each of these elements have associated advantages and 276
limitations. We discuss these points below. 277
278
Typically, FC is estimated for the entire scan, or in the case of dynamical-FC, for consecutive 279
windows of the scan24,37,38. A limitation of such an approach to capture activity propagation 280
is that inter -regional communication may occur only at select time epochs and this 281
information may be obscured by internal dynamics. The purpose of the event-identification 282
step in the EWC is to identify salient features in regional dynamics, that then serve as a 283
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Madan Mohan et al., 2024 10
Reference
point from which downstream effects are gauged. In task-based paradigms, these 284
segments are generally marked by controlled stimulus triggers. On the other hand, in task -285
free recordings, change-point detection or point-process analysis-based tools can be used to 286
capture salient changes in regional dynamics39–42. EWC reuses a simple method employed in 287
previous works that traces activity propagation to parts of the signal that deviate from mean 288
behaviour, through z-scoring31. Limiting the signal that is analysed to the proximity of the 289
events additionally makes the EWC computationally tractable when compared to 290
conventional approaches (Fig.3). 291
292
The temporal ordering aspect, which is designed to account for delays in signal conduction 293
over the network, incorporates directionality into the protocol, irrespective of the FC measure 294
used. This allows us to use undirected/symmetric measures like PC or cMI, to resolve transient 295
asymmetric FC relationships (Fig.2B,C,E,F). Any symmetric FC measure (coherence, phase 296
locking value, phase lag index etc.43–45) can similarly be rendered directional if implemented 297
in this manner. Care must however be taken to ensure that the considered delays are within 298
a reasonable range, to avoid capturing effects that might not likely be caused by the observed 299
event. 300
301
Limiting the FC estimation to a window/subsample of the signal proximal to the events offers 302
multiple advantages. It is well suited for scenarios where there is limited information regarding 303
the spatiotemporal span of the effects, allowing us to capture extended effects as opposed 304
to a local one (at a single time point) . Furthermore, averaging the results over multiple 305
windows (events) increases the robustness of the estimate. It also reduces the size of the 306
signal for which the FC must be estimated, decreasing the computational time. 307
308
In contrast to conventional FC implementations however, EWC typically involves a higher 309
number of number of computations – instead of a single computation per epoch, there are 310
now computations associated with each event within the epoch (albeit involving shorter 311
segments of data). This effect is apparent in Fig.3, where MI-Full is computed considerably 312
faster than its EWC counterpart – cMI-EWC. 313
314
Although we find that there is a strong agreement between the subject-level PC-EWC and 315
TE-Full, we noted that agree ment in terms of their asymmetry or directionality was not 316
statistically significant. This could be due to the PC and TE captur ing different statistical 317
dependencies in the data. This difference may have been subtle in the simple network-motif 318
(resulting in both the PC and TE capturing the true signalling asymmetries), but more 319
pronounced at larger scales. 320
321
Methodological considerations 322
323
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Madan Mohan et al., 2024 11
We designed EWC to capture communication-driven statistical relationships or as a statistical 324
analogue of activity propagation . Its development involved the use of several simplifying 325
assumptions to ensure computational and analytical tractability. These points need to be 326
considered to fully appreciate the scope of this work and limitations. For example, a z-value-327
based event identification as we used in this study, will be sensitive to changes in the mean 328
activity – this is evident in Fig.S2F, where an increase in the source firing rate results in firing 329
events not being identified, resulting in diminished estimates. Similarly, errors in delay 330
estimation, which affect the temporal ordering, can result in the effect of the event being 331
missed entirely. The window length is also a crucial component and must be chosen so that 332
it captures the immediate effects of the event, while also being long enough to ensure that 333
there are enough datapoints for an accurate FC estimate. The window and epoch lengths 334
also determine the resolution at which the dynamics of asymmetric relationships can be 335
observed (event-/epoch-scale vs. subject-scale). 336
337
It is also important to remember that EWC is not a direct measure of communication but is 338
instead a measure of the statistical consequence of communication. It can only be used to 339
infer communication. Care must be taken while choosing the FC measure, since different 340
measures capture different features of signal similarity (correlation, phase synchrony etc.), 341
while also being valid only on certain derivatives of the original signal e.g. Mutual information 342
can be computed between any signal (with different interpretations), whereas the phase lag 343
index is computed between the instantaneous phase time series. The effect of FC measure 344
choice is evident in Fig.2B,C,E,F, where the cMI indicates strong interaction from node 4 to 345
2, despite the lack of any interaction by construction. The PC on the other hand , does not 346
capture this functional link. In the case of non-negative FC measures like the cMI, estimates 347
can sometimes be inflated due a positive bias (despite filtering based on significance testing). 348
This can be corrected by subtracting a null-derived estimate from the observed (significant) 349
estimate. 350
351
Additionally, it must be noted that although our protocol restricts the estimation of the EWC 352
to supra-threshold events, we do not claim that communication does not take place during 353
the sub-threshold segments. The significant deviations are used to systematically reduce the 354
analysis space, since it is more difficult to establish whether EWC estimates are due to 355
communication as opposed to some other regional process or noise , in the sub -threshold 356
segments. 357
358
Conclusion
359
In conclusion, our work presents a new method to infer neural communication patterns 360
through a restricted FC estimation approach based on activity propagation events. Our 361
Method
yields FC estimates comparable to that of well -established techniques at a fraction 362
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Madan Mohan et al., 2024 12
of the computational time, opening up new avenues for the investigation of signalling in large 363
networks of neural elements. 364
365
Code availability 366
All the code used to generate activity propagation maps using the EWC is available at 367
https://github.com/vmadanmohan/EWC . 368
369
Methods
370
Dataset 371
Resting state MEG scans of 30 subjects (22 -35 years, 17F), along with associated MEG 372
anatomical data, 3T structural MRI data, and empty-room recordings, were obtained from the 373
Human Connectome Project (Van Essen et al., 2013), through the ConnectomeDB platform. 374
The MEG scans varied in duration from 5-6 minutes, at a sampling rate ( 𝑆𝑅) of 2035Hz, and 375
anti-aliasing low pass filtered at 400Hz. 376
377
Processing 378
The MEG scans were processed entirely using the MATLAB 46 -based Brainstorm software47, 379
and in accordance with pipeline described in Brainstorm's HCP -MEG tutorial 48. MEG 380
recordings were first coregistered to the subject's structural MRI using the MEG anatomical 381
data. A notch filter (60, 120, 180, 240 and 300Hz), followed by high pass filter (0.3Hz) were 382
applied to resting state and empty -room recordings, to filter out power -supply and slow -383
wave/DC-offset artifacts respectively. Each subject's recording was then visually inspected, 384
along with the channel power spectral density, to weed out bad channels and bad time 385
segments. The ECG and EOG recordings were then used to identify heartbeats and eye -386
blinks, after which associated artifacts were removed using their signal space projections 387
(SSPs)49. 388
389
The source-level activities at 8000 points, defined by the fsLR4k mesh, were then estimated 390
from the sensor -level recordings. This involved first computing the head model using 391
overlapping spheres and constrained dipoles normal to the cortical surface, and estimating 392
the noise covariance from the empty -room recordings. Source -level activities were then 393
estimated using the dSPM method 50 available in Brainstorm. The sources were then 394
parcellated using the Schaefer-Yeo 7-network 100 atlas51, with the parcel activity computed 395
as the mean of the constituent source activities. 396
397
The centroid coordinates of the Regions of Interest (ROIs) were used to define a Euclidean 398
distance (ED) matrix between all possible pairs of regions. Assuming a conduction velocity of 399
10m/s, inter -regional distances were proportionally converted to time delays ( 𝛿 ) as 400
𝛿!" = 𝐸𝐷!" 𝑣⁄ 401
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Madan Mohan et al., 2024 13
Where 𝑣 is the conduction velocity (CV) of neural signals, set to 10 𝑚 𝑠⁄ . 402
Parcellated source-localised resting-state MEG recordings were corrected for source leakage 403
effects by removing zero-lag correlations as per 52, using the OHBA Software Library (OSL) 404
package in Python53. 405
406
Estimating inter-areal communication 407
“-EWC” implementation 408
The three main elements of EWC are – 1) event-identification, and 2) Temporal ordering 409
based on conduction delays, and 3) estimation of the FC between event -marked 410
windows/subsamples. 411
Source-level parcellated time series were first epoched into 10𝑠 segments. Epochs that 412
contained bad segments were removed, and each epoch was then processed independently. 413
The data within an epoch was first z-scored: This helped identify the spread of regional 414
activities around their respective mean behaviours. For all regions, the timepoints at which 415
the |𝑧| > 3 were labelled as “events” and marked strong significant deviations from mean 416
behaviour. We argued that these significant events should cause measurable effects on the 417
activity of the rest of the brain. Additionally, finite signal conduction times would imply that 418
these downstream effects be delayed. We also focused the estimation of inter -areal 419
communication to a segment of the time series starting at the event timepoint – termed a 420
“communication window”, spanning a duration of 1𝑠. 421
422
The following steps were executed iteratively, over all ROIs, for each event: 423
424
1. A region was chosen as a source, and a window of 1𝑠 was defined starting at the 425
event. Any additional events that fell within this window were removed and not 426
considered in the subsequent iterations, to avoid excessive computation. The window 427
length was chosen to be short enough to capture the immediate effects of the 428
communication events and minimise contributions from internal dynamics. 429
2. A window of similar length was placed at the time series of all other ROIs (targets) 430
within the same hemisphere , at timepoints delayed in proportion to the Euclidean 431
distance between the source and the target (see Processing). The 1𝑠 length of the 432
window can also accommodate the effects of source signals travelling at velocities 433
much slower than 10𝑚/𝑠 (used in the calculation of inter-regional delays). 434
3. The FC measure (PC, cMI) was computed between all pairs of the source and target 435
signals within the respective windows, conditional upon the target's immediate past 436
activity over the duration of one window, up to the event. This conditioning was done 437
to remove biases due to internal dynamics (not associated with communication). The 438
FC estimates were checked for significance, with a Bonferroni-corrected threshold of 439
𝛼 =
!.!#
$!"!#$%
, and set to zero for p -values above this threshold. The final measure is 440
termed the Event-marked Windowed Communication (EWC). 441
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Madan Mohan et al., 2024 14
4. The event -level EWC values from the source to all possible targets were then 442
averaged to yield the source’s epoch-level EWC. 443
444
Once the above steps were completed for all possible sources, we were left with an epoch -445
level 𝑁 × 𝑁 EWC matrix, that captures the communication between all source -target pairs, 446
averaged over all the events in the epoch. For a given subject whose scans were divided into 447
𝑀 epochs, the communication protocol yields an 𝑁 × 𝑁 × 𝑀 EWC matrix over the entire scan 448
duration. This matrix is then averaged across epochs to give the subject-level EWC matrix. 449
450
“-Full” implementation 451
Source-level parcellated time series were first epoched into 10𝑠 segments. Epochs that 452
contained bad segments were removed, and each epoch was then processed independently. 453
The FC was computed in a pairwise manner, between all regions, between the entire epoch 454
time series. Each FC estimate was significance tested with a threshold of 𝛼 = 0.01. Like the 455
EWC implementation, the pairwise FC was computed for all epochs, yielding an 𝑁 × 𝑁 × 𝑀 456
matrix (for 𝑀 epochs) over the entire scan duration. 457
458
Partial correlation 459
The partial correlation (PC) quantifies the linear association between two random variables, 460
while discounting the effects of a third variable. In the EWC implementation, we set the third 461
variable as the target’s past over a single window duration, up to the timepoint of the event. 462
We compute the PC using MATLAB’s “partialcorr” function. The significance level was set to 463
𝛼 =
!.!#
$!"!#$%
. The partial correlation is a continuous function varying from -1 to 1 , indicating 464
perfectly negative to perfectly positive linear correlation respectively. 465
466
Conditional Mutual Information 467
The conditional Mutual Information (cMI) is an information theoretic measure that quantifies 468
the shared information between random variables (representing regional activities) in the 469
context of the activity of some exogenous additional regions (represented as a conditioning 470
variable). It is a variant of the widely used Mutual Information (MI)25,54–56. 471
Given random variables X and Y, containing the activities of two regions, and a third random 472
variable Z, containing the activity of a third region (or a set of multiple regions), the cMI is 473
measured in terms of entropies as: 474
𝐼(𝑋; 𝑌|𝑍) = 𝐻(𝑋|𝑍) + 𝐻(𝑌|𝑍) − 𝐻(𝑋, 𝑌|𝑍) 475
476
Where 𝐻(𝑋|𝑍) and 𝐻(𝑌|𝑍) are the conditional entropies associated with variables X and Y, 477
and 𝐻(𝑋, 𝑌|𝑍) is the conditional joint entropy. 478
The cMI is a symmetric measure, that varies from 0 when the two random variables are 479
independent of each other, to ∞ when they are identical. 480
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Madan Mohan et al., 2024 15
The target’s past activity was used as the conditional variable, to remove any biases to the 481
measured communication from internal dynamics. 482
483
Transfer Entropy 484
The Transfer Entropy is a widely used information-theoretic measure of directional influences 485
2,3,25,36,57,58. Specifically, for two random variables X and Y, it quantifies how much uncertainty 486
in the future of Y (target) is reduced through the knowledge of the past of X (source), 487
conditional on the past of Y. It is technically a special case of the cMI, where the shared 488
information is estimated between relatively time-shifted random variables: 489
𝑇%→'(𝑘, 𝑙) = 𝐼 @𝑋(
(*); 𝑌(,#A𝑌(
(-)B , 490
Where 𝑋(
(*) = {X./0/#, … , X./#, X.} . There are multivariate variants of the TE, which also 491
condition it on other possibly mediating variables. In this work, we use its simplest form – the 492
bivariate TE. Multivariate forms of the TE are generally better than other techniques at 493
capturing ground truth asymmetries but are considerably more data - and computation -494
intensive25. 495
496
We used the Gaussian estimator in the Java Information Dynamics Toolkit (JIDT)59 to compute 497
all information theoretic quantities. Using the Gaussian estimator allowed each estimate to 498
be significance -tested analytically from the χ1 -distribution. The estimators were run with 499
default properties, except for the source -destination delay in the TE estimator, which was 500
changed from the default value of 1, to the Euclidean distance -based inter-regional delay 501
(see Processing). All information theoretic quantities (including the EWC) are measured in 502
nats. 503
504
Demonstration on a network model 505
In order to identify the merits and limitations of our approach prior to its application to 506
neuroimaging data, we tested it on the activities of a four-node system with Linear Stochastic 507
Model60 dynamics. The dynamics of a node 𝑖 is described as: 508
𝑥2̇ = −𝑥3 + 𝐾 L 𝐶34 𝑥4N𝑡 − 𝛿34Q
4∈$
+ 𝜎𝒩(0,1) 509
Where 𝐶34 is the connectivity strength between nodes 𝑖 and 𝑗 , 𝐾 is a global coupling 510
parameter ( 𝐾 = 1), δ34 is the time delay between 𝑖 and 𝑗 (proportional to the Euclidean 511
distance), 𝒩(0,1) denotes random standard normal noise , and σ is the noise amplitude. 512
Three of the nodes were connected in a linear chain-like topology, and the fourth node was 513
isolated from the rest of the system i.e. 𝐶#1 = 𝐶1# = 𝐶16 = 𝐶61 = 1; 𝐶#6 = 𝐶6# = 0; 𝐶73 = 𝐶37 =514
0 ∀ 𝑖 ∈ {1,2,3}. 515
In addition to the LSM dynamics, a Poisson process caused both the terminal nodes to 516
“pulse” randomly, with an average frequency ν, and with a pulse amplitude of 0.1. This 517
resulted in the dynamics of the central node to be a mix of its internal dynamics, and random 518
inputs from the two terminal nodes. While Poisson spiking is a convenient means of exercising 519
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Madan Mohan et al., 2024 16
control over ground-truth signalling, it can result in an inflation of nodes’ mean activities from 520
the “baseline” at high ν, due to rapid fluctuations. 521
The communication protocol was tested across systematic variations of σ, 𝛿16, and ν. 522
523
For each set of parameter values, we simulated the dynamics for 205𝑠, at a sampling rate of 524
2035𝐻𝑧, using an Euler integrator. Epoch duration and communication window durations 525
were set to 10𝑠 and 1𝑠 respectively. 20 trials of each simulation were carried out. 526
527
Communication was inferred using the TE (Full implementation), cMI and PC (EWC 528
implementation) (see Protocol), on the activity time series of all four nodes. 529
530
Computation time benchmarking 531
To compare the computation times for different protocols as a function of network size, 532
activity propagation was inferred as TE -Full, MI-Full, TE-EWC, cMI-EWC, and PC -EWC for 533
time-series data of 200s. To ensure that the estimated computation times were realistic, the 534
recordings were randomly sampled source localised MEG recordings (see Processing). The 535
following steps were repeated for a network size 𝑁 (for 10 trials): 536
1. 𝑁 regions are randomly chosen, and the associated regional time series were trimmed 537
to 200s (sampling frequency = 2035Hz). 538
2. Inter-regional delays were set to 0.015ms. 539
3. Activity propagation was estimated between all pairs of regions as TE -Full, MI-Full, 540
TE-EWC, cMI-EWC, and PC-EWC. 541
4. Repeat with a new random selection of regions. 542
543
Acknowledgment s 544
V.M.M. is supported by the Melbour ne Research Scholarship , University of Melbourne . 545
R.F.H.C. is funded by a NHMRC Emerging Leadership Investigator Grant ( Grant number: 546
2017527). C.S. acknowledges support from the Australian Research Council ( Grant number: 547
DP170101815). A.Z. is supported by an ARC Future Fellowship and the Rebecca L. Cooper 548
Foundation. Data were provided [in part] by the Human Connectome Project, WU -Minn 549
Consortium (Principal Investigators: David Van Essen and Kamil Ugurbil; 1U54MH091657) 550
funded by the 16 NIH Institutes and Centers that support the NIH Blueprint for Neuroscience 551
Research; and by the McDonnell Center for Systems Neuroscience at Washington University. 552
This research was supported by The University of Melbourne’s Research Computing Services 553
and the Petascale Campus Initiative. 554
555
556
557
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Madan Mohan et al., 2024 17
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Event 2 Event 3Event 1
Source
Target
Target
1
2
3
𝛿12
Communication
window
𝛿13
Average over
all events
Epoching Event localization
(Activity propagation
pattern between all pairs of
regions, in an epoch)
EWC
1
1
2
2
3
3
Targets
Sources Repeat over
epochs
Epoch 1
Epoch 2
Epoch M
...
A B
C D
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Partial Correlation (EWC)
1
3
24 42
𝜎
𝜈 = 0.2Hz
= 15ms42= =
A B C
D E F
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(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 July 31, 2024. ; https://doi.org/10.1101/2024.07.30.605466doi: bioRxiv preprint
0
200
400
600
800
1000
1200
1400
1600Network inference time for a 200s recording (s)
3 10 20 50 100
N
TE-Full
cMI-EWC
TE-EWC
MI-Full
PC-EWC
-100
-80
-60
-40
-20
Relative time taken to compute PC-EWC
(% of time to compute TE-Full)
10 20
N
503 100
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(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 July 31, 2024. ; https://doi.org/10.1101/2024.07.30.605466doi: bioRxiv preprint
Corr.
Biv. Transfer Entropy (Full)
Sub. 1
Sub. 2
Sub. N
Partial correlation (EWC)
Sub. 1
Sub. 2
Sub. N
0.6 0.65 0.7 0.75 0.8 0.85 0.9 0.95
|Pearson-R|
0
2
4
6
8
10
12Probability Density
Median correlation = 0.82095
Human Connectome
Project (HCP)
MEG subjects
(n=30)
.
.
.
MEG scans
(Sensor space)
Regional activities
(Source space)
Source localisation
Parcellation
Delay estimation
Orthogonalisation
Source
Target
Communication
window
Information flow
A
B C
Partial corr. (EWC) TE (Full)
0
10
20
30
40
50
60Inference time per epoch (s)
.CC-BY-NC 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 July 31, 2024. ; https://doi.org/10.1101/2024.07.30.605466doi: bioRxiv preprint
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