Supporting results for the analytic Hamiltonian KAM construction.
Finite-cutoff lower bounds on all retained nonzero integer frequency pairings.
Equations
- KamProject.Arnold1963.FiniteNonresonant ω K N = ∀ k ∈ KamProject.Arnold1963.lowModes n N, K / KamProject.Arnold1963.indexLength k ^ (n + 1) ≤ ‖KamProject.Arnold1963.indexPairing k ω‖
Instances For
def
KamProject.Arnold1963.nonresonantDomain
{n : ℕ}
(G : Set (ComplexSpace n))
(ω : ComplexSpace n → ComplexSpace n)
(K N : ℝ)
:
Set (ComplexSpace n)
The action subdomain satisfying the finite-cutoff nonresonance condition.
Equations
- KamProject.Arnold1963.nonresonantDomain G ω K N = {p : KamProject.Arnold1963.ComplexSpace n | p ∈ G ∧ KamProject.Arnold1963.FiniteNonresonant (ω p) K N}
Instances For
theorem
KamProject.Arnold1963.FiniteNonresonant.ne_zero
{n : ℕ}
{ω : ComplexSpace n}
{K N : ℝ}
(h : FiniteNonresonant ω K N)
(hK : 0 < K)
{k : FourierIndex n}
(hk : k ∈ lowModes n N)
:
@[simp]
@[simp]
theorem
KamProject.Arnold1963.FiniteNonresonant.conj
{n : ℕ}
{ω : ComplexSpace n}
{K N : ℝ}
(h : FiniteNonresonant ω K N)
:
FiniteNonresonant (conjVec ω) K N
theorem
KamProject.Arnold1963.nonresonantDomain_conj
{n : ℕ}
{G : Set (ComplexSpace n)}
{ω : ComplexSpace n → ComplexSpace n}
{K N : ℝ}
(hG : ConjInvariant G)
(hω : ∀ p ∈ G, ω (conjVec p) = conjVec (ω p))
:
ConjInvariant (nonresonantDomain G ω K N)
theorem
KamProject.Arnold1963.analyticAt_indexPairing
{n : ℕ}
(k : FourierIndex n)
(z : ComplexSpace n)
:
AnalyticAt ℂ (indexPairing k) z