OAI/Computability/UniqueGames/Inverse/KMSAnalyticHybridEnergyTransport.lean
8 declarations, 0 contain sorry, 0 declared as axioms
Exact coordinate transport of hybrid derivative energy
Both ambient spaces, both selector subspaces, and the affine translate are transported together. The actual Fourier selector and the actual affine restriction then have the same normalized squared norm.
- theorem
OAI.UniqueGamesTheorem.Inverse.KMSAnalyticHybridEnergy.mem_map_equiv_iffline 32 - theorem
OAI.UniqueGamesTheorem.Inverse.KMSAnalyticHybridEnergy.hybrid_arrowCongrline 43Source documentation
The two clauses of the actual Hybrid selector are coordinate invariant.
theorem hybrid_arrowCongr (a : E ≃ₗ[F2] E') (b : F ≃ₗ[F2] F') (S : F →ₗ[F2] E) (A : Submodule F2 E) (B : Submodule F2 F) : LinearIdentities.Hybrid (LinearEquiv.arrowCongr b a S) (A.map a.toLinearMap) (B.map b.toLinearMap) ↔ LinearIdentities.Hybrid S A B := by … - theorem
OAI.UniqueGamesTheorem.Inverse.KMSAnalyticHybridEnergy.restriction_admissible_arrowCongrline 76Source documentation
The actual vanishing and range constraints of an affine perturbation transport to the mapped subspaces.
theorem restriction_admissible_arrowCongr (a : E ≃ₗ[F2] E') (b : F ≃ₗ[F2] F') (M : E →ₗ[F2] F) (A : Submodule F2 E) (B : Submodule F2 F) : (A.map a.toLinearMap ≤ (LinearEquiv.arrowCongr a b M).ker ∧ (LinearEquiv.arrowCongr a b M).range ≤ B.map b.toLinearMap) ↔ (A ≤ M.ker ∧ M.range ≤ B) := by … - theorem
OAI.UniqueGamesTheorem.Inverse.KMSAnalyticHybridEnergy.hybrid_embedding_rangeline 108Source documentation
Transported quotient parameters give exactly the directly transported affine perturbations; no multiplicity or normalization factor occurs.
theorem hybrid_embedding_range (a : E ≃ₗ[F2] E') (b : F ≃ₗ[F2] F') (A : Submodule F2 E) (B : Submodule F2 F) : ((LinearEquiv.arrowCongr a b).toLinearMap.comp (embedding A B)).range = (embedding (A.map a.toLinearMap) (B.map b.toLinearMap)).range := by … - theorem
OAI.UniqueGamesTheorem.Inverse.KMSAnalyticHybridEnergy.hybridProjector_pullbackline 140Source documentation
The actual Fourier Hybrid projector commutes with coordinate pullback.
theorem hybridProjector_pullback (a : E ≃ₗ[F2] E') (b : F ≃ₗ[F2] F') (f : (E' →ₗ[F2] F') → ℝ) (A : Submodule F2 E) (B : Submodule F2 F) : hybridProjector A B (fun M => f (LinearEquiv.arrowCongr a b M)) = fun M => hybridProjector (A.map a.toLinearMap) (B.map b.toLinearMap) f (LinearEquiv.arrowCongr a b M) := by … - theorem
OAI.UniqueGamesTheorem.Inverse.KMSAnalyticHybridEnergy.rankComponent_pullbackline 151Source documentation
The actual pure-rank Fourier component commutes with coordinate pullback.
theorem rankComponent_pullback (a : E ≃ₗ[F2] E') (b : F ≃ₗ[F2] F') (f : (E' →ₗ[F2] F') → ℝ) (i : ℕ) : rankComponent i (fun M => f (LinearEquiv.arrowCongr a b M)) = fun M => rankComponent i f (LinearEquiv.arrowCongr a b M) := by … - theorem
OAI.UniqueGamesTheorem.Inverse.KMSAnalyticHybridEnergy.hybridDerivative_energy_pullbackline 164Source documentation
Exact normalized energy transport, with the actual Hybrid selector, quotient restriction, and affine translate transported together.
theorem hybridDerivative_energy_pullback (a : E ≃ₗ[F2] E') (b : F ≃ₗ[F2] F') (f : (E' →ₗ[F2] F') → ℝ) (A : Submodule F2 E) (B : Submodule F2 F) (T : E →ₗ[F2] F) : (𝔼 N, hybridDerivative A B T (fun M => f (LinearEquiv.arrowCongr a b M)) N ^ 2) = 𝔼 N, hybridDerivative (A.map a.toLinearMap) (B.map b.toLinearMap) (LinearEquiv.arrowCongr a b T) f N ^ 2 := by … - theorem
OAI.UniqueGamesTheorem.Inverse.KMSAnalyticHybridEnergy.hybridDerivative_rankComponent_energy_pullbackline 183Source documentation
Pure-rank derivative energy is invariant under both coordinate changes.
theorem hybridDerivative_rankComponent_energy_pullback (a : E ≃ₗ[F2] E') (b : F ≃ₗ[F2] F') (f : (E' →ₗ[F2] F') → ℝ) (i : ℕ) (A : Submodule F2 E) (B : Submodule F2 F) (T : E →ₗ[F2] F) : (𝔼 N, hybridDerivative A B T (rankComponent i (fun M => f (LinearEquiv.arrowCongr a b M))) N ^ 2) = 𝔼 N, hybridDerivative (A.map a.toLinearMap) (B.map b.toLinearMap) (LinearEquiv.arrowCongr a b T) (rankComponent i f) N ^ 2 := by …