OAI/Analysis/MassAction/UniformOffsetDecay.lean
5 declarations, 0 contain sorry, 0 declared as axioms
- lemma
OAI.Problem326.power_isLittleO_at_zeroline 12 - theorem
OAI.Problem326.exists_common_offset_decayline 28Source documentation
Finitely many offsets with power decay strictly stronger than
h^tshare one stronger decay exponent. The individual powers may vary with the label.theorem exists_common_offset_decay {ι : Type uIota} [Fintype ι] [Nonempty ι] (c : ι → ℝ → ℝ) (t : ℝ) (hc : ∀ i, ∃ β : ℝ, t < β ∧ c i =O[𝓝[>] 0] (fun h => h ^ β)) : ∃ η : ℝ, t < η ∧ ∀ i, c i =o[𝓝[>] 0] (fun h => h ^ η) := by … - theorem
OAI.Problem326.exists_radius_with_offset_decayline 45Source documentation
A pre-existing localization radius can be shrunk so that all local offsets are little-o of
h^(t+ρ), as required by the affine-family gluing argument.theorem exists_radius_with_offset_decay {ι : Type uIota} [Fintype ι] [Nonempty ι] (c : ι → ℝ → ℝ) (t ρ₀ : ℝ) (hρ₀ : 0 < ρ₀) (hc : ∀ i, ∃ β : ℝ, t < β ∧ c i =O[𝓝[>] 0] (fun h => h ^ β)) : ∃ ρ : ℝ, 0 < ρ ∧ ρ < ρ₀ ∧ ∀ i, c i =o[𝓝[>] 0] (fun h => h ^ (t + ρ)) := by … - theorem
OAI.Problem326.shifted_offset_isBigOline 63Source documentation
The offsets produced by the type construction have the required big-O bound even though the leading negative power prevents a little-o bound at that same exponent.
theorem shifted_offset_isBigO {d : ℝ → ℝ} {β : ℝ} (hd : d =o[𝓝[>] 0] (fun h => h ^ β)) : (fun h => -(h ^ β) + d h) =O[𝓝[>] 0] (fun h => h ^ β) := by … - theorem
OAI.Problem326.shifted_offset_normalized_limitline 70Source documentation
Normalizing a constructed negative-shift offset by its leading power gives limit
-1; this is the exact sequential input used by fixed-minimum activity estimates.theorem shifted_offset_normalized_limit {d : ℝ → ℝ} {β : ℝ} (hd : d =o[𝓝[>] 0] (fun h => h ^ β)) : Tendsto (fun h : ℝ => (-(h ^ β) + d h) / h ^ β) (𝓝[>] 0) (𝓝 (-1)) := by …