1987
DOI: 10.1137/0147031
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Bifurcations and Transitions to Chaos in the Three-Dimensional Lotka–Volterra Map

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Cited by 28 publications
(26 citation statements)
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“…The dynamic behaviors observed in this model are not yet well understood from a theoretical point of view; present knowledge cannot completely define the nature of the bifurcations involved (besides the well-known ((local)) bifurcations cited in the above example). Dynamics qualitatively similar to those observed here have been found in other maps on the plane from several authors (among others: Gumowski and Mira, 1980;Argoul and Arneodo, 1984;Grebogi, Ott and Yorke, 1983;Mira, 1987; and in particular, on Lotka-Volterra maps: Gardini, Lupini, Mammana and Messia, 1987;Gumowski and Mira, 1980).…”
Section: Remarksupporting
confidence: 91%
“…The dynamic behaviors observed in this model are not yet well understood from a theoretical point of view; present knowledge cannot completely define the nature of the bifurcations involved (besides the well-known ((local)) bifurcations cited in the above example). Dynamics qualitatively similar to those observed here have been found in other maps on the plane from several authors (among others: Gumowski and Mira, 1980;Argoul and Arneodo, 1984;Grebogi, Ott and Yorke, 1983;Mira, 1987; and in particular, on Lotka-Volterra maps: Gardini, Lupini, Mammana and Messia, 1987;Gumowski and Mira, 1980).…”
Section: Remarksupporting
confidence: 91%
“…In several applied models (see, e.g., [1,[3][4][5]) it has been observed that closed invariant curves in three dimensional (3D for short) maps can undergo a kind of doubling bifurcation sequence. The bifurcation mechanism leading to such a dynamic behavior was announced as an open problem at the European Conference on Iteration Theory in 2006 (ECIT-06) [6].…”
Section: Introductionmentioning
confidence: 99%
“…As an example, in Fig.1 we show the closed invariant attracting curve and a sequence of the bifurcations mentioned above in the Lotka-Volterra model represented by the 3D map x = x + Rx(1 − x − ay − bz) y = y + Ry(1 − bx − y − az) z = z + Rz(1 − ax − by − z) (1) where the parameters R and a are fixed as R = 1, a = 0.5, and b is varied (taken from [5] and [3]). Our aim is to give a qualitative description of the possible mechanism of such bifurcations.…”
Section: Introductionmentioning
confidence: 99%
“…Our aim is to investigate how well Runge-Kutta methods do at modelling ordinary differential equations by looking at the resulting maps as dynamical systems. Chaos in numerical analysis has been investigated before: the midpoint method in the papers by Yamaguti & Ushiki [1981] and Ushiki [1982], the Euler method by Gardini et al [1987], the Euler method and the Heun method by Peitgen & Richter [1986], and the Adams-Bashforth-Moulton methods in a paper by Prüfer [1985]. These studies dealt with the chaotic dynamics of the maps produced in their own right, without relating them to the original differential equations.…”
Section: Introductionmentioning
confidence: 99%