OAI/Computability/UniqueGames/Inverse/KMSAnalyticHybridEnergyTransportSmallMixed.lean
6 declarations, 0 contain sorry, 0 declared as axioms
Exact transport of mixed small-component slices
A codomain equivalence transports the fixed primal coordinates and the prescribed partial frequency together. The frequency reindexing is bijective, so the actual slice energy has no multiplicity or normalization factor.
- theorem
OAI.UniqueGamesTheorem.Inverse.KMSAnalyticHybridEnergy.partialRestrict_codomain_pullbackline 34Source documentation
Transport of the fixed block and the free block commutes with the actual partial restriction.
theorem partialRestrict_codomain_pullback (b : F ≃ₗ[F2] F') (g : ((A × I) →ₗ[F2] F') → ℝ) (u : A →ₗ[F2] F) : partialRestrict (fun Y => g (b.toLinearMap.comp Y)) u = fun X => partialRestrict g (b.toLinearMap.comp u) (b.toLinearMap.comp X) := by … - theorem
OAI.UniqueGamesTheorem.Inverse.KMSAnalyticHybridEnergy.arrowCongr_refl_left_applyline 47 - theorem
OAI.UniqueGamesTheorem.Inverse.KMSAnalyticHybridEnergy.arrowCongr_refl_right_applyline 52 - theorem
OAI.UniqueGamesTheorem.Inverse.KMSAnalyticHybridEnergy.linearCoeff_postcomp_equivline 66Source documentation
Exact coefficient transport for a function pulled back only in its primal codomain.
theorem linearCoeff_postcomp_equiv (b : F ≃ₗ[F2] F') (g : (I →ₗ[F2] F') → ℝ) (T : F →ₗ[F2] I) : linearCoeff (fun X => g (b.toLinearMap.comp X)) T = linearCoeff g (T.comp b.symm.toLinearMap) := by … - theorem
OAI.UniqueGamesTheorem.Inverse.KMSAnalyticHybridEnergy.sliceEnergy_codomain_pullbackline 76Source documentation
Transport the prescribed frequency with the codomain. This identity requires no surjectivity of the prescribed-frequency projection.
theorem sliceEnergy_codomain_pullback (b : F ≃ₗ[F2] F') (g : (I →ₗ[F2] F') → ℝ) (π : I →ₗ[F2] J) (ν : F →ₗ[F2] J) : sliceEnergy (fun T : F →ₗ[F2] I => π.comp T = ν) (fun X => g (b.toLinearMap.comp X)) = sliceEnergy (fun T : F' →ₗ[F2] I => π.comp T = ν.comp b.symm.toLinearMap) g := by … - theorem
OAI.UniqueGamesTheorem.Inverse.KMSAnalyticHybridEnergy.sliceEnergy_partialRestrict_smallComponent_pullbackline 110Source documentation
The actual mixed small-component energy is invariant when its ambient coordinates, embedding, fixed primal map, and prescribed frequency are all transported together.
theorem sliceEnergy_partialRestrict_smallComponent_pullback (a : E ≃ₗ[F2] E') (b : F ≃ₗ[F2] F') (ι : (A × I) →ₗ[F2] E) (f : (E' →ₗ[F2] F') → ℝ) (π : I →ₗ[F2] J) (ν : F →ₗ[F2] J) (u : A →ₗ[F2] F) : sliceEnergy (fun T : F →ₗ[F2] I => π.comp T = ν) (partialRestrict (smallComponent ι (fun M => f (LinearEquiv.arrowCongr a b M))) u) = sliceEnergy (fun T : F' →ₗ[F2] I => π.comp T = ν.comp b.symm.toLinearMap) (partialRestrict (smallComponent (a.toLinearMap.comp ι) f) (b.toLinearMap.comp u)) := by …