By Yuri A. Kuznetsov

It is a ebook on nonlinear dynamical structures and their bifurcations less than parameter edition. It offers a reader with a reliable foundation in dynamical platforms concept, in addition to specific tactics for software of common mathematical effects to specific difficulties. distinctive cognizance is given to effective numerical implementations of the constructed concepts. numerous examples from contemporary learn papers are used as illustrations. The e-book is designed for complicated undergraduate or graduate scholars in utilized arithmetic, in addition to for Ph.D. scholars and researchers in physics, biology, engineering, and economics who use dynamical structures as version instruments of their stories. A reasonable mathematical historical past is thought, and, every time attainable, in basic terms hassle-free mathematical instruments are used. This re-creation preserves the constitution of the first version whereas updating the context to include fresh theoretical advancements, specifically new and greater numerical equipment for bifurcation research. overview of 1st version: "I be aware of of no different publication that so essentially explains the fundamental phenomena of bifurcation theory." Math studies "The e-book is a very good addition to the dynamical platforms literature. it truly is reliable to determine, in our sleek rush to speedy booklet, that we, as a mathematical group, nonetheless have time to collect, and in the sort of readable and thought of shape, the vital effects on our subject." Bulletin of the AMS

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There are no generalized eigenvectors associated to q. Thus, the monodromy matrix M (T0 ) has a one-dimensional invariant subspace spanned by q and a complementary (n − 1)-dimensional subspace Σ : M (T0 )Σ = Σ. Take the subspace Σ as a cross-section to the cycle at x0 = 0. 14) on Σ. Therefore, their eigenvalues µ1 , µ2 , . . , µn−1 coincide. 17) where, by deﬁnition, the divergence of a vector ﬁeld f (x) is given by n (div f )(x) = i=1 ∂fi (x) . ∂xi Thus, the product of all multipliers of any cycle is positive.

The map is smooth, and its Jacobian matrix at x0 coincides with the monodromy matrix: ∂ϕT0 x ∂x x=x0 = M (T0 ). We claim that the matrix M (T0 ) has an eigenvalue µ0 = 1. 15). Therefore, q = v(0) = f (x0 ) is transformed by M (T0 ) into itself: M (T0 )q = q. There are no generalized eigenvectors associated to q. Thus, the monodromy matrix M (T0 ) has a one-dimensional invariant subspace spanned by q and a complementary (n − 1)-dimensional subspace Σ : M (T0 )Σ = Σ. Take the subspace Σ as a cross-section to the cycle at x0 = 0.

N−1 of the Jacobian matrix A of the Poincar´e map P associated with a cycle L0 are independent of the point x0 on L0 , the cross-section Σ, and local coordinates on it. 16, where the planar case is presented for simplicity). We allow the points x1,2 to coincide, and we let the cross-sections Σ1,2 represent identical surfaces in Rn that diﬀer only in parametrization. Denote by P1 : Σ1 → Σ1 and P2 : Σ2 → Σ2 corresponding Poincar´e maps. Let ξ = (ξ1 , ξ2 , . . , ξn−1 ) be coordinates on Σ1 , and let η = (η1 , η2 , .