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LeanPool.MetricCodes.Conclusion

Binary and spherical code bounds #

The unconditional characteristic-minor argument and the final headline theorems.

The characteristic-minor identity for a box fibre: the compressed minor equals the inner- product constant times the channel numerator polynomial.

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    Agreement of the Cartan characteristic projector and the selected Clebsch range projector on the canonical box-axis tensor image.

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      theorem MetricCodes.Spherical.HigherHarmonicYoung.AllRankGTPhysicalInvalidRowProjectorVanishing.pieri_crossGram_intertwines_of_skew {r n : ℕ} (lam : Fin (r + 2) → ℕ) (mu : Fin (r + 1) → ℕ) (i : HigherYoungAllRankOrthogonalTensorPieriSourceSignatureInjectivity.PaddedPieriChannel (ThreeRowYoungBranching.appendZeroWeight lam)) (A : ↥(HarmonicYoungSpace (HigherYoungAllRankOrthogonalTensorPieriSourceSignatureInjectivity.paddedPieriSource (ThreeRowYoungBranching.appendZeroWeight lam) i)) →ₗ[ℝ] TensorProduct ℝ (SpherePacking.Euclidean (n + 1)) ↥(HarmonicYoungSpace (ThreeRowYoungBranching.appendZeroWeight lam))) (B : ↥(HarmonicYoungSpace (ThreeRowYoungBranching.appendZeroWeight (ThreeRowYoungBranching.appendZeroWeight mu))) →ₗ[ℝ] TensorProduct ℝ (SpherePacking.Euclidean (n + 1)) ↥(HarmonicYoungSpace (ThreeRowYoungBranching.appendZeroWeight lam))) (R : ↥(HarmonicYoungSpace (HigherYoungAllRankOrthogonalTensorPieriSourceSignatureInjectivity.paddedPieriSource (ThreeRowYoungBranching.appendZeroWeight lam) i)) →ₗ[ℝ] ↥(HarmonicYoungSpace (HigherYoungAllRankOrthogonalTensorPieriSourceSignatureInjectivity.paddedPieriSource (ThreeRowYoungBranching.appendZeroWeight lam) i))) (T : ↥(HarmonicYoungSpace (ThreeRowYoungBranching.appendZeroWeight (ThreeRowYoungBranching.appendZeroWeight mu))) →ₗ[ℝ] ↥(HarmonicYoungSpace (ThreeRowYoungBranching.appendZeroWeight (ThreeRowYoungBranching.appendZeroWeight mu)))) (S : TensorProduct ℝ (SpherePacking.Euclidean (n + 1)) ↥(HarmonicYoungSpace (ThreeRowYoungBranching.appendZeroWeight lam)) →ₗ[ℝ] TensorProduct ℝ (SpherePacking.Euclidean (n + 1)) ↥(HarmonicYoungSpace (ThreeRowYoungBranching.appendZeroWeight lam))) (hR : LinearMap.adjoint R = -R) (hS : LinearMap.adjoint S = -S) (hA : A ∘ₗ R = S ∘ₗ A) (hB : B ∘ₗ T = S ∘ₗ B) :
      theorem MetricCodes.Spherical.HigherHarmonicYoung.AllRankGTCharacteristicMinorOfValidRoots.gtAxisCompressedCharacteristicMinor_eq_channelNumerator_of_validRoots {r n : ℕ} (lam : Fin (r + 2) → ℕ) (mu : Fin (r + 1) → ℕ) (h : HigherRepresentationGraph.Interlaces lam mu) (hgram : AllRankGelfandTsetlinCanonicalFibre.PositiveGelfandTsetlinFischerGram lam mu h) (hfinite : HigherChannel.FiniteInterlacing (n + 1) lam mu) (hn : 2 * (r + 2) + 5 ≤ n + 1) (p q : ↥(HarmonicYoungSpace mu)) (hwall : Polynomial.eval (-HigherChannel.wallShift (n + 1) (r + 1)) (AllRankGTAxisCompressedCharacteristicMinor.gtAxisCompressedCharacteristicMinor lam mu h hgram p q) = 0) (hnegative : ∀ (row : Fin (r + 1)), HigherRepresentationGraph.Interlaces lam (HigherChannel.raiseWeight mu row) → Polynomial.eval (HigherYoungAllRankGTArrowheadSchurComplement.gtStabilizerArrowheadNode (HigherChannel.wallShift (n + 1) (r + 1)) (HigherChannel.stabilizerShift (n + 1) mu) (Sum.inr (row, false))) (AllRankGTAxisCompressedCharacteristicMinor.gtAxisCompressedCharacteristicMinor lam mu h hgram p q) = 0) (hpositive : ∀ (row : Fin (r + 1)), 0 < mu row → HigherRepresentationGraph.Interlaces lam (HigherYoungPenultimateRowProjectedLower.loweredInternalYoungWeight mu row) → Polynomial.eval (HigherYoungAllRankGTArrowheadSchurComplement.gtStabilizerArrowheadNode (HigherChannel.wallShift (n + 1) (r + 1)) (HigherChannel.stabilizerShift (n + 1) mu) (Sum.inr (row, true))) (AllRankGTAxisCompressedCharacteristicMinor.gtAxisCompressedCharacteristicMinor lam mu h hgram p q) = 0) :

      The stabilizer relative Casimir shifted by one half of the identity.

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        The linear embedding of Euclidean space obtained by appending a zero coordinate.

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          The isometric embedding of Euclidean space obtained by appending a zero coordinate.

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            The tensor isometry combining the transverse Euclidean inclusion with a canonical Gelfand–Tsetlin fibre.

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              The transverse negative-sector map obtained by composing Clebsch raising with the transverse tensor embedding.

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                The transverse positive-sector map obtained by composing Clebsch lowering with the transverse tensor embedding.

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                  The transverse negative-sector map normalized by its positive Gram scalar to a linear isometry.

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                    The transverse positive-sector map normalized by its positive Gram scalar to a linear isometry.

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                      A physical stabilizer tensor map transported through two appended zero rows in its source and one in its target.

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                        A chosen full branch whose signature is the appended stabilizer weight raised in its last coordinate.

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                          The canonical full-branch fibre corresponding to the wall signature.

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                            The tensor isometry combining the transverse Euclidean inclusion with the canonical wall fibre.

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                              The transverse wall-sector map obtained by composing Clebsch raising with the wall tensor embedding.

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                                The gt wall sector gram used in the spherical-code argument.

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                                  theorem MetricCodes.Spherical.HigherHarmonicYoung.AllRankGTWallSectorGram.gtWallSectorGram_pos {r n : ℕ} (lam : Fin (r + 2) → ℕ) (mu : Fin (r + 1) → ℕ) (h : HigherRepresentationGraph.Interlaces lam mu) (hn : 2 * (r + 1) + 5 ≤ n + 1) (hlast : 0 < lam (Fin.last (r + 1))) :

                                  The tensor isometry combining the transverse Euclidean inclusion with a supplied stabilizer isometry.

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                                    The transverse wall-sector map normalized by its positive Gram scalar to a linear isometry.

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                                      The tensor isometry induced by a canonical full-branch fibre while retaining the Euclidean tensor factor.

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                                        The tensor isometry induced by the transverse Euclidean inclusion while retaining the harmonic Young factor.

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                                          The tensor isometry combining the transverse Euclidean inclusion with a canonical full- branch fibre.

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                                            The isometry sending a harmonic Young vector to its tensor with the last coordinate axis.

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                                              The isometry obtained by embedding a full-branch fibre and tensoring with the last coordinate axis.

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                                                theorem MetricCodes.Spherical.HigherHarmonicYoung.AllRankGTPhysicalCompleteBlockReconstruction.inner_eq_zero_of_mem_iSup_range_of_adjoint_eq_zero {ι : Type u_1} {V : Type u_2} [NormedAddCommGroup V] [InnerProductSpace ℝ V] [FiniteDimensional ℝ V] (E : ι → Type u_3) [(i : ι) → NormedAddCommGroup (E i)] [(i : ι) → InnerProductSpace ℝ (E i)] [∀ (i : ι), FiniteDimensional ℝ (E i)] (A : (i : ι) → E i →ₗ[ℝ] V) (y : V) (hzero : ∀ (i : ι), (LinearMap.adjoint (A i)) y = 0) (x : V) (hx : x ∈ ⨆ (i : ι), (A i).range) :
                                                inner ℝ x y = 0
                                                theorem MetricCodes.Spherical.HigherHarmonicYoung.AllRankGTPhysicalCompleteBlockReconstruction.eq_zero_of_iSup_range_sup_eq_top_of_adjoint_eq_zero {ι : Type u_1} {κ : Type u_2} {V : Type u_3} [NormedAddCommGroup V] [InnerProductSpace ℝ V] [FiniteDimensional ℝ V] (E : ι → Type u_4) (F : κ → Type u_5) [(i : ι) → NormedAddCommGroup (E i)] [(i : ι) → InnerProductSpace ℝ (E i)] [∀ (i : ι), FiniteDimensional ℝ (E i)] [(j : κ) → NormedAddCommGroup (F j)] [(j : κ) → InnerProductSpace ℝ (F j)] [∀ (j : κ), FiniteDimensional ℝ (F j)] (A : (i : ι) → E i →ₗ[ℝ] V) (B : (j : κ) → F j →ₗ[ℝ] V) (hcomplete : (⨆ (i : ι), (A i).range) ⊔ ⨆ (j : κ), (B j).range = ⊤) (y : V) (haxis : ∀ (i : ι), (LinearMap.adjoint (A i)) y = 0) (htransverse : ∀ (j : κ), (LinearMap.adjoint (B j)) y = 0) :
                                                y = 0
                                                theorem MetricCodes.Spherical.HigherHarmonicYoung.AllRankGTPhysicalCompleteBlockReconstruction.eq_of_iSup_range_sup_eq_top_of_adjoint_eq {ι : Type u_1} {κ : Type u_2} {V : Type u_3} [NormedAddCommGroup V] [InnerProductSpace ℝ V] [FiniteDimensional ℝ V] (E : ι → Type u_4) (F : κ → Type u_5) [(i : ι) → NormedAddCommGroup (E i)] [(i : ι) → InnerProductSpace ℝ (E i)] [∀ (i : ι), FiniteDimensional ℝ (E i)] [(j : κ) → NormedAddCommGroup (F j)] [(j : κ) → InnerProductSpace ℝ (F j)] [∀ (j : κ), FiniteDimensional ℝ (F j)] (A : (i : ι) → E i →ₗ[ℝ] V) (B : (j : κ) → F j →ₗ[ℝ] V) (hcomplete : (⨆ (i : ι), (A i).range) ⊔ ⨆ (j : κ), (B j).range = ⊤) (x y : V) (haxis : ∀ (i : ι), (LinearMap.adjoint (A i)) x = (LinearMap.adjoint (A i)) y) (htransverse : ∀ (j : κ), (LinearMap.adjoint (B j)) x = (LinearMap.adjoint (B j)) y) :
                                                x = y

                                                The canonical Gelfand–Tsetlin axis tensor map bundled as a linear isometry.

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                                                  theorem MetricCodes.Spherical.HigherHarmonicYoung.AllRankGTPhysicalRetainedAdditiveColumn.linearMap_comp_eq_smul_add_of_complete_adjoint_block_rows {ι : Type u_1} {κ : Type u_2} {E : Type u_3} {F : Type u_4} {V : Type u_5} [AddCommGroup E] [Module ℝ E] [AddCommGroup F] [Module ℝ F] [NormedAddCommGroup V] [InnerProductSpace ℝ V] [FiniteDimensional ℝ V] (X : ι → Type u_6) (Y : κ → Type u_7) [(i : ι) → NormedAddCommGroup (X i)] [(i : ι) → InnerProductSpace ℝ (X i)] [∀ (i : ι), FiniteDimensional ℝ (X i)] [(j : κ) → NormedAddCommGroup (Y j)] [(j : κ) → InnerProductSpace ℝ (Y j)] [∀ (j : κ), FiniteDimensional ℝ (Y j)] (C : (i : ι) → X i →ₗ[ℝ] V) (D : (j : κ) → Y j →ₗ[ℝ] V) (hcomplete : (⨆ (i : ι), (C i).range) ⊔ ⨆ (j : κ), (D j).range = ⊤) (T : Module.End ℝ V) (B : E →ₗ[ℝ] V) (A : F →ₗ[ℝ] V) (K : E →ₗ[ℝ] F) (d : ℝ) (haxis : ∀ (i : ι), LinearMap.adjoint (C i) ∘ₗ T ∘ₗ B = d • LinearMap.adjoint (C i) ∘ₗ B + (LinearMap.adjoint (C i) ∘ₗ A) ∘ₗ K) (htransverse : ∀ (j : κ), LinearMap.adjoint (D j) ∘ₗ T ∘ₗ B = d • LinearMap.adjoint (D j) ∘ₗ B + (LinearMap.adjoint (D j) ∘ₗ A) ∘ₗ K) :
                                                  T ∘ₗ B = d • B + A ∘ₗ K
                                                  theorem MetricCodes.Spherical.HigherHarmonicYoung.AllRankGTPhysicalRetainedAdditiveColumn.gtRelativeCasimir_comp_eq_smul_add_of_full_axis_transverse_rows {r n : ℕ} (lam : Fin (r + 1) → ℕ) (hn : 2 * r + 5 ≤ n + 1) (hdom : Antitone lam) {E : Type u_1} {F : Type u_2} [AddCommGroup E] [Module ℝ E] [AddCommGroup F] [Module ℝ F] (B : E →ₗ[ℝ] TensorProduct ℝ (SpherePacking.Euclidean (n + 1)) ↥(HarmonicYoungSpace lam)) (A : F →ₗ[ℝ] TensorProduct ℝ (SpherePacking.Euclidean (n + 1)) ↥(HarmonicYoungSpace lam)) (K : E →ₗ[ℝ] F) (d : ℝ) (haxis : ∀ (mu : BranchingDimension.FullBranchWeight lam), LinearMap.adjoint (AllRankGTActualAxisTransverseDecomposition.gtFullAxisEmbedding lam hn mu).toLinearMap ∘ₗ AllRankGTRelativeCasimirProjector.gtRelativeCasimir lam ∘ₗ B = d • LinearMap.adjoint (AllRankGTActualAxisTransverseDecomposition.gtFullAxisEmbedding lam hn mu).toLinearMap ∘ₗ B + (LinearMap.adjoint (AllRankGTActualAxisTransverseDecomposition.gtFullAxisEmbedding lam hn mu).toLinearMap ∘ₗ A) ∘ₗ K) (htransverse : ∀ (mu : BranchingDimension.FullBranchWeight lam), LinearMap.adjoint (AllRankGTTransverseFullBranchDecomposition.gtFullTransverseEmbedding lam hn mu).toLinearMap ∘ₗ AllRankGTRelativeCasimirProjector.gtRelativeCasimir lam ∘ₗ B = d • LinearMap.adjoint (AllRankGTTransverseFullBranchDecomposition.gtFullTransverseEmbedding lam hn mu).toLinearMap ∘ₗ B + (LinearMap.adjoint (AllRankGTTransverseFullBranchDecomposition.gtFullTransverseEmbedding lam hn mu).toLinearMap ∘ₗ A) ∘ₗ K) :
                                                  theorem MetricCodes.Spherical.HigherHarmonicYoung.AllRankGTPhysicalRetainedAdditiveColumn.gtRelativeCasimir_comp_eq_smul_add_of_orthogonal_full_block_rows {r n : ℕ} (lam : Fin (r + 1) → ℕ) (hn : 2 * r + 5 ≤ n + 1) (hdom : Antitone lam) {E : Type u_1} {F : Type u_2} [AddCommGroup E] [Module ℝ E] [AddCommGroup F] [Module ℝ F] (B : E →ₗ[ℝ] TensorProduct ℝ (SpherePacking.Euclidean (n + 1)) ↥(HarmonicYoungSpace lam)) (A : F →ₗ[ℝ] TensorProduct ℝ (SpherePacking.Euclidean (n + 1)) ↥(HarmonicYoungSpace lam)) (K : E →ₗ[ℝ] F) (d : ℝ) (haxisOrth : ∀ (mu : BranchingDimension.FullBranchWeight lam), LinearMap.adjoint (AllRankGTActualAxisTransverseDecomposition.gtFullAxisEmbedding lam hn mu).toLinearMap ∘ₗ B = 0) (htransverseOrth : ∀ (mu : BranchingDimension.FullBranchWeight lam), LinearMap.adjoint (AllRankGTTransverseFullBranchDecomposition.gtFullTransverseEmbedding lam hn mu).toLinearMap ∘ₗ A = 0) (haxis : ∀ (mu : BranchingDimension.FullBranchWeight lam), LinearMap.adjoint (AllRankGTActualAxisTransverseDecomposition.gtFullAxisEmbedding lam hn mu).toLinearMap ∘ₗ AllRankGTRelativeCasimirProjector.gtRelativeCasimir lam ∘ₗ B = (LinearMap.adjoint (AllRankGTActualAxisTransverseDecomposition.gtFullAxisEmbedding lam hn mu).toLinearMap ∘ₗ A) ∘ₗ K) (htransverse : ∀ (mu : BranchingDimension.FullBranchWeight lam), LinearMap.adjoint (AllRankGTTransverseFullBranchDecomposition.gtFullTransverseEmbedding lam hn mu).toLinearMap ∘ₗ AllRankGTRelativeCasimirProjector.gtRelativeCasimir lam ∘ₗ B = d • LinearMap.adjoint (AllRankGTTransverseFullBranchDecomposition.gtFullTransverseEmbedding lam hn mu).toLinearMap ∘ₗ B) :

                                                  The cross block of the relative Casimir from a supplied tensor map to the canonical Gelfand–Tsetlin axis image.

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                                                    theorem MetricCodes.Spherical.HigherHarmonicYoung.AllRankGTPhysicalSelectedTwoBlockClosure.mem_submodule_of_complete_orthogonal_two_family_projections {ι : Type u_1} {κ : Type u_2} {H : Type u_3} [Finite ι] [Finite κ] [NormedAddCommGroup H] [InnerProductSpace ℝ H] [FiniteDimensional ℝ H] (U : ι → Submodule ℝ H) (V : κ → Submodule ℝ H) (hU : ∀ (i j : ι), i ≠ j → U i ⟂ U j) (hV : ∀ (i j : κ), i ≠ j → V i ⟂ V j) (hUV : ∀ (i : ι) (j : κ), U i ⟂ V j) (hcomplete : (⨆ (i : ι), U i) ⊔ ⨆ (j : κ), V j = ⊤) (S : Submodule ℝ H) (x : H) (haxis : ∀ (i : ι), (U i).starProjection x ∈ S) (htransverse : ∀ (j : κ), (V j).starProjection x ∈ S) :
                                                    x ∈ S

                                                    The signed characteristic adjugate expressed as a sum of characteristic projectors weighted by the nodal polynomials with one node removed.

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                                                      theorem MetricCodes.Spherical.HigherHarmonicYoung.AllRankGTAxisCompressedValidNodeRoot.gtAxisCompressedCharacteristicMinor_eval_eq_zero_of_arrowhead_operator_row {r n : ℕ} (lam : Fin (r + 2) → ℕ) (mu : Fin (r + 1) → ℕ) (h : HigherRepresentationGraph.Interlaces lam mu) (hgram : AllRankGelfandTsetlinCanonicalFibre.PositiveGelfandTsetlinFischerGram lam mu h) (hfinite : HigherChannel.FiniteInterlacing (n + 1) lam mu) (p q : ↥(HarmonicYoungSpace mu)) (B : ↥(HarmonicYoungSpace mu) →ₗ[ℝ] TensorProduct ℝ (SpherePacking.Euclidean (n + 1)) ↥(HarmonicYoungSpace lam)) (node : ℝ) (coupling : Module.End ℝ ↥(HarmonicYoungSpace mu)) (hcoupling : Function.Injective ⇑coupling) (horth : (LinearMap.adjoint B) ((AllRankGTCompressedResolvent.canonicalGelfandTsetlinAxisTensor lam mu h hgram) q) = 0) (hchar : ((Polynomial.aeval (AllRankGTRelativeCasimirProjector.gtRelativeCasimir lam)) (HigherYoungAllRankGTCharacteristicResidue.gtChannelCharacteristicPolynomial (n + 1) lam)) ((AllRankGTCompressedResolvent.canonicalGelfandTsetlinAxisTensor lam mu h hgram) q) = 0) (hrow : ∀ (x : TensorProduct ℝ (SpherePacking.Euclidean (n + 1)) ↥(HarmonicYoungSpace lam)), (LinearMap.adjoint B) ((AllRankGTRelativeCasimirProjector.gtRelativeCasimir lam) x) = node • (LinearMap.adjoint B) x + coupling ((LinearMap.adjoint (AllRankGTCompressedResolvent.canonicalGelfandTsetlinAxisTensor lam mu h hgram)) x)) :
                                                      theorem MetricCodes.Spherical.HigherHarmonicYoung.AllRankGTCartanSpectralCouplingNonvanishing.arrowhead_eigen_of_coupling_kernel {E : Type u_1} {F : Type u_2} {V : Type u_3} [AddCommGroup E] [Module ℝ E] [AddCommGroup F] [Module ℝ F] [AddCommGroup V] [Module ℝ V] (T : Module.End ℝ V) (B : E →ₗ[ℝ] V) (A : F →ₗ[ℝ] V) (K : E →ₗ[ℝ] F) (d : ℝ) (hrow : T ∘ₗ B = d • B + A ∘ₗ K) (p : E) (hp : K p = 0) :
                                                      T (B p) = d • B p
                                                      theorem MetricCodes.Spherical.HigherHarmonicYoung.AllRankGTCartanSpectralCouplingNonvanishing.arrowhead_coupling_eq_zero_of_apply_eq_zero {E : Type u_1} {F : Type u_2} {V : Type u_3} [AddCommGroup E] [Module ℝ E] [AddCommGroup F] [Module ℝ F] [AddCommGroup V] [Module ℝ V] (T : Module.End ℝ V) (B : E →ₗ[ℝ] V) (hB : Function.Injective ⇑B) (A : F →ₗ[ℝ] V) (K : E →ₗ[ℝ] F) (P : Polynomial ℝ) (d : ℝ) (hrow : T ∘ₗ B = d • B + A ∘ₗ K) (hchar : ∀ (p : E), ((Polynomial.aeval T) P) (B p) = 0) (heval : Polynomial.eval d P ≠ 0) (p : E) (hp : K p = 0) :
                                                      p = 0
                                                      theorem MetricCodes.Spherical.HigherHarmonicYoung.AllRankGTValidTransverseMinorRoots.gtAxisCompressedCharacteristicMinor_eval_actualPhysicalNode_eq_zero {r n : ℕ} (lam : Fin (r + 2) → ℕ) (mu : Fin (r + 1) → ℕ) (h : HigherRepresentationGraph.Interlaces lam mu) (hgram : AllRankGelfandTsetlinCanonicalFibre.PositiveGelfandTsetlinFischerGram lam mu h) (hfinite : HigherChannel.FiniteInterlacing (n + 1) lam mu) (hn : 2 * (r + 2) + 5 ≤ n + 1) (B : ↥(HarmonicYoungSpace mu) →ₗᵢ[ℝ] TensorProduct ℝ (SpherePacking.Euclidean (n + 1)) ↥(HarmonicYoungSpace lam)) (node : ℝ) (K : Module.End ℝ ↥(HarmonicYoungSpace mu)) (horthogonal : ∀ (p q : ↥(HarmonicYoungSpace mu)), inner ℝ ((AllRankGTCompressedResolvent.canonicalGelfandTsetlinAxisTensor lam mu h hgram) p) (B q) = 0) (hcolumn : AllRankGTRelativeCasimirProjector.gtRelativeCasimir lam ∘ₗ B.toLinearMap = node • B.toLinearMap + AllRankGTCompressedResolvent.canonicalGelfandTsetlinAxisTensor lam mu h hgram ∘ₗ K) (hsector : ∀ (p : ↥(HarmonicYoungSpace mu)), ((Polynomial.aeval (AllRankGTRelativeCasimirProjector.gtRelativeCasimir lam)) (HigherYoungAllRankGTCharacteristicResidue.gtChannelCharacteristicPolynomial (n + 1) lam)) (B p) = 0) (hnode : ∀ (i : Fin (r + 2) × Bool), node ≠ HigherChannel.signedNode (HigherChannel.ambientShift (n + 1) lam) i) (p q : ↥(HarmonicYoungSpace mu)) :
                                                      theorem MetricCodes.Spherical.HigherHierarchy.main_general {s : ℝ} (hs : 0 < s) (hs' : s < 1) :
                                                      (∀ {r : ℕ} {R : ℝ} (a : Fin (r + 1) → ℝ) (b : Fin r → ℝ), Interlacing a b → s < 2 * Gamma a b → Phi a b < R → ∀ᶠ (n : ℕ) in Filter.atTop, ∀ (C : SpherePacking.SphericalCode n s), ↑C.points.card < 2 ^ (R * ↑n)) ∧ sphericalCodeRate s ≤ closedHierarchyVariationalRate s
                                                      noncomputable def SpherePacking.kissingNumber (n : ℕ) :

                                                      The kissing number used in the spherical-code argument.

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