An overview is given on two representative methods of dynamical reduction known as centermanifold reduction and phase reduction. These theories are presented in a somewhat more unified fashion than the theories in the past. The target systems of reduction are coupled limit-cycle oscillators. Particular emphasis is placed on the remarkable structural similarity existing between these theories. While the two basic principles, i.e. (i) reduction of dynamical degrees of freedom and (ii) transformation of reduced evolution equation to a canonical form, are shared commonly by reduction methods in general, it is shown how these principles are incorporated into the above two reduction theories in a coherent manner. Regarding the phase reduction, a new formulation of perturbative expansion is presented for discrete populations of oscillators. The style of description is intended to be so informal that one may digest, without being bothered with technicalities, what has been done after all under the word reduction. arXiv:1910.13775v1 [nlin.AO] 30 Oct 2019
II. CENTER-MANIFOLD REDUCTIONWe begin with the center-manifold reduction for a single oscillator, and then proceed to multi-oscillator systems. It will be seen how the two elements of reduction, namely, the reduction of dynamical degrees of freedom and transformation of the evolution equation to a canonical form, are incorporated into a systematic perturbation theory.
A. Reduction of a single free oscillatorThe situation of our concern is the neighborhood of the Hopf bifurcation of an n-dimensional dynamical systeṁ X = F(X) with fixed point X = 0. We separate F into an unperturbed part and perturbation, where the former