Summable total action-domain loss, including resonance shells and boundary layers.
noncomputable def
KamProject.Arnold1963.Iteration.actionLossFactor
(n : ℕ)
(θ₀ Θ₀ : NNReal)
(D : ℝ)
:
The coefficient transporting the frequency-space loss budget to real action volume.
Equations
- KamProject.Arnold1963.Iteration.actionLossFactor n θ₀ Θ₀ D = (2 * ↑Θ₀ / ↑θ₀) ^ n * KamProject.Arnold1963.resonanceLossConstant n * D
Instances For
noncomputable def
KamProject.Arnold1963.Iteration.lossBudget
(n : ℕ)
(δ₁ θ₀ Θ₀ : NNReal)
(κ D : ℝ)
(s : ℕ)
:
The extended nonnegative action-volume loss budget for one iteration stage.
Equations
- KamProject.Arnold1963.Iteration.lossBudget n δ₁ θ₀ Θ₀ κ D s = ENNReal.ofReal (KamProject.Arnold1963.Iteration.actionLossFactor n θ₀ Θ₀ D * KamProject.Arnold1963.Iteration.rawLoss n δ₁ Θ₀ κ s)
Instances For
theorem
KamProject.Arnold1963.Iteration.InitialParameters.rawLoss_nonneg
{n : ℕ}
{δ₁ θ₀ Θ₀ ρ₀ : NNReal}
{κ D : ℝ}
(b : InitialParameters n δ₁ θ₀ Θ₀ ρ₀ κ D)
(s : ℕ)
:
theorem
KamProject.Arnold1963.Iteration.InitialParameters.rawLoss_le
{n : ℕ}
{δ₁ θ₀ Θ₀ ρ₀ : NNReal}
{κ D : ℝ}
(b : InitialParameters n δ₁ θ₀ Θ₀ ρ₀ κ D)
(s : ℕ)
:
rawLoss n δ₁ Θ₀ κ s ≤ κ * ↑δ₁ * newShellBudget (previousCutoff n δ₁ s) (cutoff n δ₁ s) + ↑(delta δ₁ s)
theorem
KamProject.Arnold1963.Iteration.InitialParameters.rawLoss_summable
{n : ℕ}
{δ₁ θ₀ Θ₀ ρ₀ : NNReal}
{κ D : ℝ}
(b : InitialParameters n δ₁ θ₀ Θ₀ ρ₀ κ D)
:
theorem
KamProject.Arnold1963.Iteration.InitialParameters.actionLossFactor_pos
{n : ℕ}
{δ₁ θ₀ Θ₀ ρ₀ : NNReal}
{κ D : ℝ}
(b : InitialParameters n δ₁ θ₀ Θ₀ ρ₀ κ D)
:
theorem
KamProject.Arnold1963.Iteration.InitialParameters.initial_measure_budget
{n : ℕ}
{δ₁ θ₀ Θ₀ ρ₀ : NNReal}
{κ D : ℝ}
(b : InitialParameters n δ₁ θ₀ Θ₀ ρ₀ κ D)
:
theorem
KamProject.Arnold1963.Iteration.InitialParameters.total_budget
{n : ℕ}
{δ₁ θ₀ Θ₀ ρ₀ : NNReal}
{κ D : ℝ}
(b : InitialParameters n δ₁ θ₀ Θ₀ ρ₀ κ D)
:
theorem
KamProject.Arnold1963.Iteration.InitialParameters.lossBudget_tsum_lt
{n : ℕ}
{δ₁ θ₀ Θ₀ ρ₀ : NNReal}
{κ D : ℝ}
(b : InitialParameters n δ₁ θ₀ Θ₀ ρ₀ κ D)
: