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Morris Lecar equation (model for neural oscillator).
Integrate and fire (model for neural oscillator).
Hodgkin–Huxley equation (model for neural oscillator).
FitzHugh Nagumo equation (model for neural oscillator).
Leaky integrate and fire (model for neural oscillator).
Quadratic integrate and fire (model for neural oscillator).
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Continuum models for neural fields often take the form of nonlinear integro-differential equations where the integral term can be viewed as a nonlocal interaction term; see [37] for a derivation of neural field models.
TB singularity has appeared when investigating some of the models for neural bursting [3, 25] and its biological importance for bursting has been further underlined by Osinga et al. [20].
The need for ex vivo systems, lab-on-a-chip technologies and disease models for neural tissue engineering applications are emerging to overcome the shortages and drawbacks of traditional in vitro systems and animal models.
Differences between models for neural noise and response generation will affect particular expressions for these two terms.
Several studies have investigated the particle filter for BMI decoding with a variety of non-linear models for neural tuning: Gao et al. [26], [27], Brockwell et al. [25], Shoham et al. [28].
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