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TauCeti.Geometry.Manifold.Morse.GradientFlow

Convergence of negative gradient trajectories trapped in a compact set #

Let f be a C² function on a boundaryless finite-dimensional manifold M carrying a C¹ Riemannian metric, and let γ be the maximal integral curve of the negative gradient -grad f through a point x. Neither M nor the sublevels of f need be compact, and the metric need not be complete. Along γ the function f decreases with derivative -‖grad f‖² (TauCeti.hasDerivAt_comp_maximalIntegralCurve_neg_mgradient); this is the energy dissipation identity, whose integrated form identifies the total energy ∫ ‖grad f (γ t)‖² dt with the drop of f (TauCeti.integral_Ioi_norm_mgradient_sq_maximalIntegralCurve).

Suppose that the forward trajectory of x stays in a compact set K. Then it exists for all positive time, every cluster point of γ t as t → ∞ is a critical point of f, and if K contains only finitely many critical points the trajectory converges to one of them (TauCeti.exists_tendsto_maximalIntegralCurve_neg_mgradient). This is the manifold counterpart, for an arbitrary Riemannian metric, of the vector-space theorem IsIntegralCurveOn.exists_tendsto_atTop. The ω-limit set of the trajectory is nonempty, connected and invariant under the local flow, and f is constant on it, so the gradient vanishes there.

A proper Morse function bounded below traps each forward trajectory in its initial compact sublevel, so every forward negative gradient trajectory of such a function converges to a critical point (TauCeti.IsMorse.exists_tendsto_maximalIntegralCurve_neg_mgradient). The metric is arbitrary: it need not be adapted to the Morse charts of f.

Main declarations #

References #

The maximal integral curve of -grad f is C¹ on its interval of definition.

Energy dissipation #

Energy dissipation along a negative gradient trajectory. Along the maximal integral curve γ of -grad f, the function f has derivative -‖grad f (γ t)‖².

Energy monotonicity. The function f is antitone along the maximal integral curve of its negative gradient.

A forward trajectory stays in the sublevel of its initial point. The forward part of the maximal integral curve of -grad f through x lies in the sublevel {y | f y ≤ f x}.

The energy identity on a bounded time interval. Between two times a and b of its interval of definition, the energy ½ ∫ ‖γ'‖² of the maximal integral curve γ of -grad f is half the drop f (γ a) - f (γ b).

The energy of a forward trajectory is finite. If the maximal integral curve of -grad f through x exists for all positive time and f has a limit along it, then ‖grad f‖² is integrable along it on (0, ∞).

The energy identity. If the maximal integral curve of -grad f through x exists for all positive time and f tends to c along it, then ∫₀^∞ ‖grad f (γ t)‖² dt = f x - c.

Trapped trajectories #

A trapped forward trajectory exists for all positive time. If the forward part of the maximal integral curve of -grad f through x stays in a compact set, it is defined on [0, ∞).

The ω-limit points of a trapped trajectory are critical. If the forward part of the maximal integral curve of -grad f through x stays in a compact set, every cluster point of this curve as t → ∞ is a critical point of f.

Convergence of a trapped negative gradient trajectory. If the forward part of the maximal integral curve of -grad f through x stays in a compact set K containing only finitely many critical points of f, the trajectory converges to one of these critical points. That it exists for all positive time is TauCeti.Ici_subset_maximalIntegralCurveInterval_neg_mgradient.

Negative gradient trajectories of a proper Morse function converge. If f is a proper Morse function bounded below, the maximal integral curve of -grad f through any point converges to a critical point of f, for any C¹ Riemannian metric.