1975
DOI: 10.1090/qam/445095
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Perturbation analysis of an approximation to the Hodgkin-Huxley theory

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Cited by 149 publications
(58 citation statements)
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References 12 publications
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“…(1) and (2) admit solutions only in the form of traveling waves (autowaves) [2,3,5,8,10,12,28,29], and when ǫ ≪ 1 and α > ∼ 1 (KN systems) they admit only solutions in the form of static patterns, the simplest of which are AS in the form of solitary spots and stripes of high or low values of the activator surrounded by the "sea" of low or high values of the activator, respectively ("hot" and "cold" AS) [11,12]. Notice that because of the monostability of the considered system the radius of a spot or the width of a stripe cannot be greater than certain value of order one [11,12].…”
Section: Scenarios Of Pattern Formation: Results Of the Simulationsmentioning
confidence: 99%
“…(1) and (2) admit solutions only in the form of traveling waves (autowaves) [2,3,5,8,10,12,28,29], and when ǫ ≪ 1 and α > ∼ 1 (KN systems) they admit only solutions in the form of static patterns, the simplest of which are AS in the form of solitary spots and stripes of high or low values of the activator surrounded by the "sea" of low or high values of the activator, respectively ("hot" and "cold" AS) [11,12]. Notice that because of the monostability of the considered system the radius of a spot or the width of a stripe cannot be greater than certain value of order one [11,12].…”
Section: Scenarios Of Pattern Formation: Results Of the Simulationsmentioning
confidence: 99%
“…To do so, it is convenient to approximate the traveling pulse solution by a periodic orbit of large period so that we can use certain theoretical results obtained for adjoint solutions to such periodic solutions. Previous work has established that the singular perturbation construction of traveling pulses to a reaction-diffusion analogue of (3.1) on the real line, in the absence of stimulation, generalizes directly to give the existence of a periodic solution on a finite spatial domain with periodic boundary conditions [4]. Indeed, the argument for the existence of traveling pulses in [20] shows how to generalize the construction in [4] to the unstimulated form of (3.1), and the extension to the periodic case follows immediately.…”
Section: Behavior Of the Solution To The Adjoint Equationmentioning
confidence: 99%
“…In [5], a similar symmetry argument is used to obtain an appropriate trailing back solution to the Fitzhugh-Nagumo equations. More generally, however, it may happen that, as V increases along the g + (V ) branch, the cusp of the sigmoid is encountered before a drop point is found for which the back speed matches that of the front.…”
Section: Singular Perturbation Constructionmentioning
confidence: 99%
“…Examined extensively in the form of the reaction-diffusion equations, traveling fronts (see [37], [22], [21]), pulses (see [5], [30], [29]), standing patterns (see [16], [53]), and other spatial structures [60], [36] (see [55] for review) have each been analytically demonstrated to exist as solutions.…”
Section: Singular Perturbation Constructionmentioning
confidence: 99%