
The Rulkov map is a two-dimensional
iterated map used to model a biological
neuron
A neuron, neurone, or nerve cell is an membrane potential#Cell excitability, electrically excitable cell (biology), cell that communicates with other cells via specialized connections called synapses. The neuron is the main component of nervous ...
. It was proposed by Nikolai F. Rulkov in 2001.
["Modelling of spiking-bursting neural behavior using two dimensional map]
/ref> The use of this map to study neural networks
A neural network is a network or circuit of biological neurons, or, in a modern sense, an artificial neural network, composed of artificial neurons or nodes. Thus, a neural network is either a biological neural network, made up of biological ...
has computational advantages because the map is easier to iterate than a continuous dynamical system
In mathematics, a dynamical system is a system in which a function describes the time dependence of a point in an ambient space. Examples include the mathematical models that describe the swinging of a clock pendulum, the flow of water in a ...
. This saves memory and simplifies the computation of large neural networks.
The model
The Rulkov map, with as discrete time, can be represented by the following dynamical equations:
:
:
where represents the membrane potential
Membrane potential (also transmembrane potential or membrane voltage) is the difference in electric potential between the interior and the exterior of a biological cell. That is, there is a difference in the energy required for electric charge ...
of the neuron. The variable in the model is a slow variable due to a very small value of . Unlike variable , variable does not have explicit biological meaning, though some analogy to gating variables can be drawn. The parameter can be thought of as an external dc current given to the neuron and is a nonlinearity parameter of the map. Different combinations of parameters and give rise to different dynamical states of the neuron like resting, tonic spiking and chaotic bursts. The chaotic bursting is enabled above
Analysis
The dynamics of the Rulkov map can be analyzed by analyzing the dynamics of its one dimensional fast submap. Since the variable evolves very slowly, for moderate amount of time it can be treated as a parameter with constant value in the variable's evolution equation (which we now call as one dimensional fast submap because as compared to , is a fast variable). Depending on the value of , this submap can have either one or three fixed points. One of these fixed points is stable, another is unstable and third may change the stability. As increases, two of these fixed points (stable one and unstable one) merge and disappear by saddle-node bifurcation In the mathematical area of bifurcation theory a saddle-node bifurcation, tangential bifurcation or fold bifurcation is a local bifurcation in which two fixed points (or equilibria) of a dynamical system collide and annihilate each other. The term ...
.
See also
*Biological neuron model
Biological neuron models, also known as a spiking neuron models, are mathematical descriptions of the properties of certain cells in the nervous system that generate sharp electrical potentials across their cell membrane, roughly one millisecon ...
*Hodgkin–Huxley model
The Hodgkin–Huxley model, or conductance-based model, is a mathematical model that describes how action potentials in neurons are initiated and propagated. It is a set of nonlinear differential equations that approximates the electrical charac ...
*FitzHugh–Nagumo model
The FitzHugh–Nagumo model (FHN), named after Richard FitzHugh (1922–2007) who suggested the system in 1961 and J. Nagumo ''et al''. who created the equivalent circuit the following year, describes a prototype of an excitable system (e.g., a n ...
*Chialvo map
The Chialvo map is a two-dimensional map proposed by Dante R. Chialvo in 1995 to describe the generic dynamics of excitable systems. The model is inspired by Kunihiko Kaneko's Coupled map lattice (CML) numerical approach which considers time ...
References
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Dynamical systems