Introduce the vector . Its autonomous ordinary differential equation iswhere the coordinate indices start at zero. Appending the clock removes the explicit time dependence.
For a vector field with local existence and uniqueness, its flow is the solution at elapsed time starting at . The uniqueness theorem for ordinary differential equations gives whenever both sides are defined. The orbit is . For a forward-complete solution its omega-limit set isequivalently the set of limits along sequences . A homoclinic orbit is a nonconstant complete orbit approaching the same equilibrium as and . This last definition concerns a general autonomous system; the appended clock itself cannot approach an equilibrium.
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