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Titlebook: Dynamical Systems V; Bifurcation Theory a V. I. Arnol’d Book 1994 Springer-Verlag Berlin Heidelberg 1994 Bifurcation Theory.Bifurkationsthe

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Herz, Kreislauf und Hämodynamik them”, said Poincaré (., Part 2, Chapter V (Analysis and physics), p. 222 (1905b)). In 1931, following this prescription, A.A. Andronov (1933) came out with a vast program (also set forth in the preface to Andronov and Khajkin, 1937) which differs from the contemporary program of catastrophe theori
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Verständlichkeit ist nur der Anfangnt the entire space of objects studied as a finite union of submanifolds of codimensions not greater than . (called .) and a remainder of codimension ⩾. + 1 so that within each class an object’s properties that are of interest to us do not change. Then all objects in typical, no more than .-paramete
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ius" and a "maniac". Catastrophe theory is accurately described as singularity theory and its (genuine) applications. The authors of this book, previously published as Volume 5 of the Encyclopaedia, have given a masterly exposition of these two theories, with penetrating insight.978-3-540-65379-0978-3-642-57884-7
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Bifurcations of Equilibriaparameters are changed continuously and smoothly. Thus, upon loss of stability, a limit cycle may arise from a singular point, and the loss of stability by a limit cycle may give rise to chaos. Such changes are termed bifurcations.
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Bifurcations of Limit Cycles. Therefore the basic objects of study in this chapter are the bifurcations of germs of diffeomorphisms at a fixed point. Local families of germs of diffeomorphisms, their equivalence and weak equivalence, and induced and versal deformations of such germs are defined just as for germs of vector fiel
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