Physical blowups via buffered time change in a mean-field neural network
Nikolaos Papadopoulos, Thibaud Taillefumier

TL;DR
This paper characterizes and unambiguously defines physical blowup solutions in mean-field neural networks, demonstrating their uniqueness and regularization via buffering mechanisms, which helps understand synchronized spiking events.
Contribution
It introduces a fixed-point formulation for physical blowup solutions and a buffering regularization to select meaningful solutions in mean-field neural models.
Findings
Physical blowup solutions are uniquely characterized.
Buffering regularization converges to physical solutions.
Nonzero refractory periods prevent eternal blowups.
Abstract
Idealized networks of integrate-and-fire neurons with impulse-like interactions obey McKean-Vlasov diffusion equations in the mean-field limit. These equations are prone to blowups: for a strong enough interaction coupling, the mean-field rate of interaction diverges in finite time with a finite fraction of neurons spiking simultaneously, thereby marking a macroscopic synchronous event. Characterizing these blowup singularities analytically is the key to understanding the emergence and persistence of spiking synchrony in mean-field neural models. Such a treatment is possible via time change techniques for a Poissonian variation of the classically considered integrate-and-fire dynamics. However, just as for shock solutions for nonlinear conservation laws, there are several admissible blowup solutions to the corresponding McKean-Vlasov equations. Because of this ambiguity, it is unclear…
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