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multiple time scale dynamics with two fast variables and one slow ...

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Note that we do not give a detailed description of <strong>dynamics</strong> associated to a<br />

singular Hopf bifurcation <strong>and</strong> refer the reader to the previous extensive litera-<br />

ture e.g. [4, 5, 13, 86, 52].<br />

6.3 Canard Explosion<br />

We describe the main results about canard explosion in <strong>fast</strong>-<strong>slow</strong> systems <strong>with</strong><br />

<strong>one</strong> <strong>fast</strong> <strong>and</strong> <strong>one</strong> <strong>slow</strong> variable from [86]. Consider a planar <strong>fast</strong>-<strong>slow</strong> system of<br />

the form<br />

x ′ = f (x, y,λ,ǫ)<br />

y ′ = ǫg(x, y,λ,ǫ) (6.3)<br />

where f, g∈C k (R 4 , R) for k≥3,λ∈R is a parameter <strong>and</strong> 0 0 so that C0 is locally a parabola <strong>with</strong> a minimum at the<br />

origin. Using (6.4) <strong>and</strong> the implicit function theorem we have that C0 is the<br />

graph of a function y = φ(x) forφ : U → R where U is a sufficiently small<br />

neighborhood of x=0. Assume that C0 splits into an attracting <strong>and</strong> a repelling<br />

149

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