Escaping points, dense orbits, and Devaney chaos #
The remaining dynamical consequences use covering, periodic points, and Baire category.
Part of Lasse Rempe's formalisation of Shen and Rempe-Gillen's exponential-map paper,
with generative AI assistance including Copilot, Claude, and particularly ChatGPT.
The initial proof architecture uses John Harrison's HOL Light formalisation.
See LeanPool.ExpChaotic for attribution and the upstream source.
Escaping points, transitivity, and dense orbits #
The compact-covering theorem makes the remaining conclusions of Shen and Rempe-Gillen's Theorem 1.1 particularly short. Escaping is expressed directly by eventual escape from every Euclidean ball. Dense orbits are constructed by applying the Baire theorem to the sets of points whose orbit visits each member of a fixed countable basis of the plane.
A point escapes to infinity if its orbit eventually leaves every centred Euclidean ball.
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- ExponentialJuliaSetMisiurewicz.EscapesToInfinity z = ∀ (R : ℝ), ∃ (N : ℕ), ∀ n ≥ N, R ≤ ‖ExponentialJuliaSetMisiurewicz.expIterate n z‖
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The escaping set of the complex exponential map.
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Every real point escapes to infinity under iteration of the exponential map.
Any point whose orbit reaches the real axis subsequently escapes to infinity.
Theorem 4.1. The escaping set of the complex exponential map is dense in the plane.
Theorem 5.1. The complex exponential map is topologically transitive.
The set of starting points whose orbit visits a specified set.
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The orbit-visit set of a nonempty open set is itself open and dense.
The set of points whose forward orbit under the exponential is dense in the plane.
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Visiting every member of mathlib's countable basis is equivalent to having dense orbit.
Corollary 5.6. Points with dense forward orbit are dense in the plane.
Removing a countable set still leaves a dense set of points with dense orbit.
Corollary 5.6. The set of points with dense orbit is uncountable.
Devaney chaos on the plane: continuity, dense periodic points, and transitivity.
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Theorem 1.2. The complex exponential map is chaotic in Devaney's sense.