OAI/Computability/MaxCut/Games/KMSInjectionCountBounds.lean
47 declarations, 0 contain sorry, 0 declared as axioms
Elementary dimension bounds for the actual injection count. The lower bound is intentionally loose; its exponent suffices for the KMS norm ratio.
- theorem
OAI.MaxCutGames.Inverse.KMSInjectionCount.binary_factor_lowerline 13 - theorem
OAI.MaxCutGames.Inverse.KMSInjectionCount.beta_le_powline 29 - theorem
OAI.MaxCutGames.Inverse.KMSInjectionCount.beta_ge_powline 39 - theorem
OAI.MaxCutGames.Inverse.KMSInjectionCount.beta_positiveline 52 - theorem
OAI.MaxCutGames.Inverse.KMSInjectionCount.beta_self_leline 56 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.smallComponent_energy_cross_mulline 97Source documentation
The exact ratio is cross-multiplied, so the identity also covers zero components without any nonzero-energy premise.
theorem smallComponent_energy_cross_mul (ι : I →ₗ[F2] E) (hι : Function.Injective ι) (f : (E →ₗ[F2] F) → ℝ) (hf : IsBasisInvariant f) : (beta I E : ℝ) * (𝔼 X, smallComponent ι f X ^ 2) = (beta I I : ℝ) * (𝔼 X, rankComponent (Module.finrank F2 I) f X ^ 2) := by …Mentions: OAI.MaxCutGames.Inverse.KMSAnalytic.smallComponent, OAI.MaxCutGames.Inverse.KMSAnalytic.rankComponent
- theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.smallComponent_energy_ratioline 129Source documentation
Dividing by the positive, explicitly counted injection multiplicity gives the normalized small-space energy exactly.
theorem smallComponent_energy_ratio (ι : I →ₗ[F2] E) (hι : Function.Injective ι) (f : (E →ₗ[F2] F) → ℝ) (hf : IsBasisInvariant f) : (𝔼 X, smallComponent ι f X ^ 2) = (beta I I : ℝ) / (beta I E : ℝ) * (𝔼 X, rankComponent (Module.finrank F2 I) f X ^ 2) := by …Mentions: OAI.MaxCutGames.Inverse.KMSAnalytic.smallComponent, OAI.MaxCutGames.Inverse.KMSAnalytic.rankComponent
- theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.smallComponent_energy_pow_boundline 147Source documentation
An explicit dimension-only norm comparison obtained from the actual injection counts. The loose constant is sufficient for the analytic argument.
theorem smallComponent_energy_pow_bound (ι : I →ₗ[F2] E) (hι : Function.Injective ι) (f : (E →ₗ[F2] F) → ℝ) (hf : IsBasisInvariant f) : (2 : ℝ) ^ (Module.finrank F2 I * (Module.finrank F2 E - Module.finrank F2 I)) * (𝔼 X, smallComponent ι f X ^ 2) ≤ (2 : ℝ) ^ (Module.finrank F2 I * Module.finrank F2 I) * (𝔼 X, rankComponent (Module.finrank F2 I) f X ^ 2) := by …Mentions: OAI.MaxCutGames.Inverse.KMSAnalytic.smallComponent, OAI.MaxCutGames.Inverse.KMSAnalytic.rankComponent
- theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.smallComponent_energy_le_of_energy_leline 175Source documentation
The zero-fixed-character case uses only the original function's squared norm bound. In particular it applies to a pseudorandom indicator of density at most
ε, without assuming any restricted Fourier inequality.theorem smallComponent_energy_le_of_energy_le (ι : I →ₗ[F2] E) (hι : Function.Injective ι) (f : (E →ₗ[F2] F) → ℝ) (hf : IsBasisInvariant f) (ε : ℝ) (hε : (𝔼 X, f X ^ 2) ≤ ε) : (2 : ℝ) ^ (Module.finrank F2 I * (Module.finrank F2 E - Module.finrank F2 I)) * (𝔼 X, smallComponent ι f X ^ 2) ≤ (2 : ℝ) ^ (Module.finrank F2 I * Module.finrank F2 I) * ε := by …Mentions: OAI.MaxCutGames.Inverse.KMSAnalytic.smallComponent
- theorem
OAI.MaxCutGames.Inverse.KMSInjectionCount.pow_dim_mul_le_pow_sq_mul_betaline 202Source documentation
A subtraction-free form of the lower injection count.
theorem pow_dim_mul_le_pow_sq_mul_beta (hdim : Module.finrank F2 I ≤ Module.finrank F2 E) : (2 : ℝ) ^ (Module.finrank F2 I * Module.finrank F2 E) ≤ (2 : ℝ) ^ (Module.finrank F2 I * Module.finrank F2 I) * (beta I E : ℝ) := by …Mentions: OAI.MaxCutGames.Inverse.KMSInjectionCount.F2, OAI.MaxCutGames.Inverse.KMSInjectionCount.beta
- theorem
OAI.MaxCutGames.Inverse.KMSInjectionCount.beta_ratio_le_powline 220Source documentation
The small-to-ambient injection ratio, with the full ambient exponent.
theorem beta_ratio_le_pow [Finite I] (hdim : Module.finrank F2 I ≤ Module.finrank F2 E) : (beta I I : ℝ) / (beta I E : ℝ) ≤ (2 : ℝ) ^ (2 * (Module.finrank F2 I * Module.finrank F2 I)) / (2 : ℝ) ^ (Module.finrank F2 I * Module.finrank F2 E) := by …Mentions: OAI.MaxCutGames.Inverse.KMSInjectionCount.F2, OAI.MaxCutGames.Inverse.KMSInjectionCount.beta
- theorem
OAI.MaxCutGames.Inverse.KMSInjectionCount.pow_mul_le_of_beta_cross_mulline 247Source documentation
Convert a count-weighted energy identity into a clean dimension bound.
theorem pow_mul_le_of_beta_cross_mul [Finite I] (hdim : Module.finrank F2 I ≤ Module.finrank F2 E) {x y : ℝ} (hx : 0 ≤ x) (hy : 0 ≤ y) (hcross : (beta I E : ℝ) * x = (beta I I : ℝ) * y) : (2 : ℝ) ^ (Module.finrank F2 I * Module.finrank F2 E) * x ≤ (2 : ℝ) ^ (2 * (Module.finrank F2 I * Module.finrank F2 I)) * y := by …Mentions: OAI.MaxCutGames.Inverse.KMSInjectionCount.F2, OAI.MaxCutGames.Inverse.KMSInjectionCount.beta
- theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.smallComponent_energy_base_boundline 298 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.fixedFrequencyEnergy_zero_dim_boundline 325Source documentation
In a zero-dimensional partial codomain every prescribed frequency is the unique one, so the base sum is exactly the small-component squared norm.
theorem fixedFrequencyEnergy_zero_dim_bound (ι : I →ₗ[F2] E) (hι : Function.Injective ι) (f : (E →ₗ[F2] F) → ℝ) (hf : IsBasisInvariant f) (ε : ℝ) (hg : HomogeneousRestrictionBound (Module.finrank F2 I) ε f) (π : I →ₗ[F2] J) (A : F →ₗ[F2] J) (hJ : Module.finrank F2 J = 0) : (2 : ℝ) ^ ((Module.finrank F2 I + Module.finrank F2 J) * Module.finrank F2 E) * fixedFrequencyEnergy ι f π A ≤ (2 : ℝ) ^ (4 * Module.finrank F2 I * Module.finrank F2 I) * ε := by …Mentions: OAI.MaxCutGames.Inverse.KMSAnalytic.HomogeneousRestrictionBound, OAI.MaxCutGames.Inverse.KMSAnalytic.fixedFrequencyEnergy
- theorem
OAI.MaxCutGames.Inverse.KMSFourthMoment.character_codomain_compositionline 362Source documentation
Restricting the codomain of a primal map restricts the domain of its dual frequency. This identity is independent of the choice of bases.
theorem character_codomain_composition (J : B →ₗ[F2] F) (S : F →ₗ[F2] E) (X : E →ₗ[F2] B) : linearTraceCharacter S (J.comp X) = linearTraceCharacter (S.comp J) X := by … - theorem
OAI.MaxCutGames.Inverse.KMSFourthMoment.coefficient_codomain_pullbackline 377Source documentation
Coefficients of the actual restricted function are the unnormalized sum over exactly those original frequencies whose restriction is the new one. The statement allows arbitrary linear
J; injections are the KMS use case.theorem coefficient_codomain_pullback (J : B →ₗ[F2] F) (f : (E →ₗ[F2] F) → ℝ) (T : B →ₗ[F2] E) : linearCoeff (fun X => f (J.comp X)) T = ∑ S : F →ₗ[F2] E, if S.comp J = T then linearCoeff f S else 0 := by … - theorem
OAI.MaxCutGames.Inverse.KMSFourthMoment.coefficient_codomain_pullback_fiberline 398Source documentation
The same merging identity on the actual fiber type. This form is ready for the hyperplane extension bijection, without changing normalization.
theorem coefficient_codomain_pullback_fiber (J : B →ₗ[F2] F) (f : (E →ₗ[F2] F) → ℝ) (T : B →ₗ[F2] E) : linearCoeff (fun X => f (J.comp X)) T = ∑ S : {S : F →ₗ[F2] E // S.comp J = T}, linearCoeff f S.val := by … - def
OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtendline 439Source documentation
Extend a frequency by specifying its value on the new coordinate.
def hyperplaneExtend (z : B →ₗ[F2] E) (v : E) : (B × F2) →ₗ[F2] E := …
- theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtend_applyline 442 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtend_comp_inlline 445 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtend_new_coordinateline 449 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtend_recoverline 453Source documentation
Recover a linear map from its old coordinates and its new-coordinate value.
theorem hyperplaneExtend_recover (S : (B × F2) →ₗ[F2] E) : hyperplaneExtend (S.comp (LinearMap.inl F2 B F2)) (S (0, 1)) = S := by …Mentions: OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtend
- def
OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtensionEquivline 462Source documentation
Exact parametrization of a restriction fiber, including dependent extensions.
def hyperplaneExtensionEquiv (z : B →ₗ[F2] E) : E ≃ {S : (B × F2) →ₗ[F2] E // S.comp (LinearMap.inl F2 B F2) = z} where … - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtend_injectiveline 472 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.range_hyperplaneExtendline 478Source documentation
The range is the old range plus the span of the new vector.
theorem range_hyperplaneExtend (z : B →ₗ[F2] E) (v : E) : (hyperplaneExtend z v).range = z.range ⊔ Submodule.span F2 {v} := by …Mentions: OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtend
- theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.range_hyperplaneExtend_of_memline 482 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.ker_hyperplaneExtend_of_notMemline 488Source documentation
All outside-range extensions have the same actual kernel.
theorem ker_hyperplaneExtend_of_notMem (z : B →ₗ[F2] E) {v : E} (hv : v ∉ z.range) : (hyperplaneExtend z v).ker = z.ker.prod (⊥ : Submodule F2 F2) := by …Mentions: OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtend
- theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.coefficient_hyperplaneExtend_eqline 500 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.card_hyperplaneExtension_outsideline 512Source documentation
The number of outside choices is exactly the ambient cardinality minus the old range cardinality.
theorem card_hyperplaneExtension_outside (z : B →ₗ[F2] E) : (Finset.univ.filter (fun v : E => v ∉ z.range)).card = Fintype.card E - Fintype.card z.range := by … - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.card_hyperplaneExtension_outside_powline 519 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.sum_hyperplaneExtend_outsideline 527Source documentation
Exact sum of the common coefficient over all outside-range extensions.
theorem sum_hyperplaneExtend_outside (f : (E →ₗ[F2] (B × F2)) → ℝ) (hf : KMSBasisInvariant.IsBasisInvariant f) (z : B →ₗ[F2] E) {v : E} (hv : v ∉ z.range) : (∑ u with u ∉ z.range, linearCoeff f (hyperplaneExtend z u)) = ((Fintype.card E - Fintype.card z.range : ℕ) : ℝ) * linearCoeff f (hyperplaneExtend z v) := by …Mentions: OAI.MaxCutGames.Inverse.KMSBasisInvariant.IsBasisInvariant, OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtend
- theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.sum_hyperplaneExtendline 542Source documentation
Split the full extension fiber into dependent and independent choices.
theorem sum_hyperplaneExtend (f : (E →ₗ[F2] (B × F2)) → ℝ) (hf : KMSBasisInvariant.IsBasisInvariant f) (z : B →ₗ[F2] E) {v : E} (hv : v ∉ z.range) : (∑ u : E, linearCoeff f (hyperplaneExtend z u)) = (∑ u with u ∈ z.range, linearCoeff f (hyperplaneExtend z u)) + ((Fintype.card E - Fintype.card z.range : ℕ) : ℝ) * linearCoeff f (hyperplaneExtend z v) := by …Mentions: OAI.MaxCutGames.Inverse.KMSBasisInvariant.IsBasisInvariant, OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtend
- theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.coefficient_hyperplaneExtend_recursionline 554Source documentation
Solve the extension sum for the coefficient of an independent extension.
theorem coefficient_hyperplaneExtend_recursion (f : (E →ₗ[F2] (B × F2)) → ℝ) (hf : KMSBasisInvariant.IsBasisInvariant f) (z : B →ₗ[F2] E) {v : E} (hv : v ∉ z.range) : linearCoeff f (hyperplaneExtend z v) = ((∑ u : E, linearCoeff f (hyperplaneExtend z u)) - ∑ u with u ∈ z.range, linearCoeff f (hyperplaneExtend z u)) / ((Fintype.card E - Fintype.card z.range : ℕ) : ℝ) := by …Mentions: OAI.MaxCutGames.Inverse.KMSBasisInvariant.IsBasisInvariant, OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtend
- theorem
OAI.MaxCutGames.Inverse.KMSFourthMoment.coefficient_hyperplane_restrictionline 598Source documentation
Exact codomain-restriction coefficient, reindexed by the extension vector. The sum has no cardinality normalization.
theorem coefficient_hyperplane_restriction (f : (E →ₗ[F2] (B × F2)) → ℝ) (z : B →ₗ[F2] E) : linearCoeff (fun X => f ((LinearMap.inl F2 B F2).comp X)) z = ∑ u : E, linearCoeff f (hyperplaneExtend z u) := by … - theorem
OAI.MaxCutGames.Inverse.KMSFourthMoment.coefficient_zoomOut_recursionline 609Source documentation
KMS's genuine zoom-out recurrence, in product coordinates. The denominator is the exact number of independent extension vectors. Basis invariance is used to prove their Fourier coefficients coincide.
theorem coefficient_zoomOut_recursion (f : (E →ₗ[F2] (B × F2)) → ℝ) (hf : KMSBasisInvariant.IsBasisInvariant f) (z : B →ₗ[F2] E) {v : E} (hv : v ∉ z.range) : linearCoeff f (hyperplaneExtend z v) = (linearCoeff (fun X => f ((LinearMap.inl F2 B F2).comp X)) z - ∑ u with u ∈ z.range, linearCoeff f (hyperplaneExtend z u)) / ((Fintype.card E - Fintype.card z.range : ℕ) : ℝ) := by …Mentions: OAI.MaxCutGames.Inverse.KMSBasisInvariant.IsBasisInvariant
- theorem
OAI.MaxCutGames.Inverse.KMSFourthMoment.coefficient_zoomOut_mulline 621Source documentation
A denominator-free form convenient for squared-norm estimates.
theorem coefficient_zoomOut_mul (f : (E →ₗ[F2] (B × F2)) → ℝ) (hf : KMSBasisInvariant.IsBasisInvariant f) (z : B →ₗ[F2] E) {v : E} (hv : v ∉ z.range) : ((Fintype.card E - Fintype.card z.range : ℕ) : ℝ) * linearCoeff f (hyperplaneExtend z v) = linearCoeff (fun X => f ((LinearMap.inl F2 B F2).comp X)) z - ∑ u with u ∈ z.range, linearCoeff f (hyperplaneExtend z u) := by …Mentions: OAI.MaxCutGames.Inverse.KMSBasisInvariant.IsBasisInvariant
- theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.sub_sum_sq_le_card_mulline 650Source documentation
Cauchy--Schwarz with the distinguished scalar included as one extra summand. This form also handles an empty dependent branch.
theorem sub_sum_sq_le_card_mul {C : Type*} [Fintype C] (x : ℝ) (a : C → ℝ) : (x - ∑ c, a c) ^ 2 ≤ ((Fintype.card C : ℝ) + 1) * (x ^ 2 + ∑ c, a c ^ 2) := by … - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.coefficient_zoomOut_sq_boundline 669Source documentation
An actual independent extension coefficient is controlled by its homogeneous restriction coefficient and every dependent extension.
theorem coefficient_zoomOut_sq_bound (f : (E →ₗ[F2] (B × F2)) → ℝ) (hf : IsBasisInvariant f) (z : B →ₗ[F2] E) {v : E} (hv : v ∉ z.range) : (((Fintype.card E - Fintype.card z.range : ℕ) : ℝ) ^ 2) * linearCoeff f (hyperplaneExtend z v) ^ 2 ≤ ((Fintype.card z.range : ℝ) + 1) * (linearCoeff (fun X => f ((LinearMap.inl F2 B F2).comp X)) z ^ 2 + ∑ u : z.range, linearCoeff f (hyperplaneExtend z u.val) ^ 2) := by …Mentions: OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtend
- def
OAI.MaxCutGames.Inverse.KMSAnalytic.leftEmbeddingline 701 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.leftEmbedding_injectiveline 704 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.lastVector_not_mem_left_rangeline 710 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.range_left_comp_of_surjectiveline 716 - def
OAI.MaxCutGames.Inverse.KMSAnalytic.liftedRangeEquivline 728Source documentation
The dependent extensions are enumerated exactly once by the small space.
def liftedRangeEquiv (ι : (J × F2) →ₗ[F2] E) (hι : Function.Injective ι) (z : B →ₗ[F2] J) (hz : Function.Surjective z) : J ≃ ((leftEmbedding ι).comp z).range := … - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.liftedRangeEquiv_valline 742 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.card_lifted_rangeline 746 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.sum_lifted_rangeline 752 - theorem
OAI.MaxCutGames.Inverse.KMSAnalytic.hyperplaneExtend_left_compline 759