1993
DOI: 10.1152/jn.1993.69.6.2252
|View full text |Cite
|
Sign up to set email alerts
|

Nonlinear dynamics in a model neuron provide a novel mechanism for transient synaptic inputs to produce long-term alterations of postsynaptic activity

Abstract: 1. A mathematical model of a bursting molluscan neuron has been found to possess multiple modes of electrical activity, such as periodic beating (tonic firing), periodic bursting (bursts of action potentials separated by quiescent periods), and potentially chaotic bursting, all at a single set of parameters. The multiple modes correspond to multiple stable attractors, whose existence is an emergent property of the nonlinear dynamics of the system. 2. Transient synaptic inputs can switch the activity of the neu… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

2
62
0
2

Year Published

1995
1995
2022
2022

Publication Types

Select...
4
3

Relationship

0
7

Authors

Journals

citations
Cited by 106 publications
(66 citation statements)
references
References 14 publications
2
62
0
2
Order By: Relevance
“…Examples exist of models generating type II bursting in which instantaneous perturbations can reset the oscillation. These include the model of bursting in R 15 by Bertram (1993Bertram ( , 1994, where one of the slow variables is sufficiently fast at some voltages to respond quickly to the perturbation (although this model does not fit precisely into the present framework since it has a quintic, rather than cubic, slow manifold), and the R15 model by Canavier et al (1991) in which several bursting, beating, and chaotic attractors coexist (Canavier et al, 1993). Phase resetting, then, provides only a limited experimental tool in the classification of a bursting oscillation.…”
Section: Undershooting Spikes With Non-planar Fast Subsystems Althoumentioning
confidence: 99%
“…Examples exist of models generating type II bursting in which instantaneous perturbations can reset the oscillation. These include the model of bursting in R 15 by Bertram (1993Bertram ( , 1994, where one of the slow variables is sufficiently fast at some voltages to respond quickly to the perturbation (although this model does not fit precisely into the present framework since it has a quintic, rather than cubic, slow manifold), and the R15 model by Canavier et al (1991) in which several bursting, beating, and chaotic attractors coexist (Canavier et al, 1993). Phase resetting, then, provides only a limited experimental tool in the classification of a bursting oscillation.…”
Section: Undershooting Spikes With Non-planar Fast Subsystems Althoumentioning
confidence: 99%
“…͑1͒ and ͑2͒, respectively. The slow subsystem can act independently, 21 be affected synaptically, 17 or interact locally with the spiking fast subsystem 5,[15][16][17] to produce alternating periods of spiking and silence in time. To examine the dynamical mechanism implicit to a bursting behavior, y is treated as a bifurcation parameter of the fast subsystem.…”
Section: A Simple Parabolic Bursting Modelmentioning
confidence: 99%
“…͑2͒ degenerates into an algebraic equation, but the assumption is reasonable when there is a large time separation between fast and slow dynamics. Using this technique, all autonomously bursting single neuron models displaying multirhythmic bursting in literature 15,16 are topologically classified as the circle/circle type; 22,23 that is, their fast subsystem is driven back and forth across a saddle node on invariant circle ͑SNIC͒ bifurcation to produce alternating spiking and silent states. These models can be reduced to a form that supports a topological normal SNIC to and from the active phase.…”
Section: A Simple Parabolic Bursting Modelmentioning
confidence: 99%
See 2 more Smart Citations