Abstract

Recent experimental results on spike avalanches measured in the urethane-anesthetized rat cortex have revealed scaling relations that indicate a phase transition at a specific level of cortical firing rate variability. The scaling relations point to critical exponents whose values differ from those of a branching process, which has been the canonical model employed to understand brain criticality. This suggested that a different model, with a different phase transition, might be required to explain the data. Here we show that this is not necessarily the case. By employing two different models belonging to the same universality class as the branching process (mean-field directed percolation) and treating the simulation data exactly like experimental data, we reproduce most of the experimental results. We find that subsampling the model and adjusting the time bin used to define avalanches (as done with experimental data) are sufficient ingredients to change the apparent exponents of the critical point. Moreover, experimental data is only reproduced within a very narrow range in parameter space around the phase transition.

Highlights

  • In the first results that fueled the critical brain hypothesis, Beggs and Plenz (2003) observed intermittent bursts of local field potentials (LFPs) in in vitro multielectrode recordings of cultured and acute slices of the rat brain

  • These exponents and dynamic behavior of the model are typical of a system undergoing a meanfield directed percolation (MF-DP) phase transition

  • For the new experimental data, we verified that the scaling relation combining the three exponents (Equation 4) was satisfied at an intermediate value coefficient of variation (CV)∗, away from the synchronous and asynchronous extremes

Read more

Summary

Introduction

In the first results that fueled the critical brain hypothesis, Beggs and Plenz (2003) observed intermittent bursts of local field potentials (LFPs) in in vitro multielectrode recordings of cultured and acute slices of the rat brain. These scale-invariant distributions were interpreted as a signature that the brain could be operating at criticality— a second-order phase transition (Beggs and Plenz, 2003; Beggs, 2007; Chialvo, 2010; Shew and Plenz, 2013; Plenz and Niebur, 2014; Tomen et al, 2019) These two critical exponents together are compatible with a branching process at its critical point (Harris, 1963), a conclusion that was further strengthened by the experimentally established critical branching parameter of 1 for neuronal avalanches (Beggs and Plenz, 2003). This points to a phase transition between a so-called absorbing phase (zero population firing rate) and an active phase (non-zero stationary population firing rate)

Methods
Results
Conclusion

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.