Arbitrary-rank interlacing #
Mickelsson operators, interlacing schedules, and canonical projected-axis witnesses.
The upper polarization path commutator used in the spherical-code argument.
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- MetricCodes.Spherical.HigherHarmonicYoung.ArbitraryRowMickelssonPathCommutator.upperPolarizationPathCommutator a b [] = 0
- MetricCodes.Spherical.HigherHarmonicYoung.ArbitraryRowMickelssonPathCommutator.upperPolarizationPathCommutator a b [head] = 0
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The intermediate polarization expression linking the front and tail paths in simple-root toggle identities.
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Multiply the simple-root toggle bridge by the coordinate at the path's starting row.
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The coordinate toggle bridge with no front path, using the coordinate in row a.
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The coordinate-weighted lowering path through the sorted rows of S and then the terminal
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The coordinate-weighted lowering-path summand in the arbitrary-row axial raising operator.
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Every prefix of the axial raising schedule leaves the current weight antitone.
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The ideal generated by the axis coordinates in rows strictly before row.
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The ideal generated jointly by the Gram radial relations and the earlier-row axis coordinates.
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Each successive axial raising step has a positive leading scalar at its current weight.
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- MetricCodes.Spherical.HigherHarmonicYoung.ArbitraryRankGelfandTsetlinTriangularNormalForm.positiveLeadingAxialSchedule lam [] = True
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The list of axis-coordinate polynomials in rows strictly before row.
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The list of Gram quadratics followed by the earlier-row axis-coordinate generators.
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Retain the old row coordinates as polynomial variables and send the additional row and coordinate to zero.
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The polynomial retraction obtained by setting the additional row and transverse coordinate to zero.
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The reverse interlacing polynomial seed bundled as a map to homogeneous highest-weight space.
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The reverse interlacing harmonic branch used in the spherical-code argument.
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The reverse interlacing harmonic branch normalized to an isometry using its positive Gram scalar.
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The ambient coordinate derivation used in the spherical-code argument.
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The ambient rotation used in the spherical-code argument.
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The row polarization operator expressed as a sum of coordinate-weighted partial derivations.
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The commutator of two polynomial derivations, bundled again as a derivation.
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- MetricCodes.Spherical.HigherHarmonicYoung.MixedSignature.derivationCommutator D₁ D₂ = Derivation.mk' (↑D₁ ∘ₗ ↑D₂ - ↑D₂ ∘ₗ ↑D₁) ⋯
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The euclidean ambient rotation used in the spherical-code argument.
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Negate the output of a channel isometry by precomposing it with negation.
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The young ambient casimir used in the spherical-code argument.
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The polynomial Casimir operator, one half of the negative sum of squared ambient rotations.
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A linear map between harmonic Young spaces that intertwines every ambient rotation operator.
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The box axis used in the spherical-code argument.
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Choose the channel or its negation according to the sign of the axis coefficient c.
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Data encoding the coherent box sector construction.
- channel : HigherYoungMovingFibres.YoungVertex (HigherYoungActualGraphAssembly.boxSignature a n) source →ₗᵢ[ℝ] TensorProduct ℝ (SpherePacking.Euclidean n) (HigherYoungMovingFibres.YoungVertex (HigherYoungActualGraphAssembly.boxSignature a n) target)
The channel component.
- rotation (c d : Fin n) : self.channel.toLinearMap ∘ₗ HigherHarmonicYoung.MixedSignature.youngAmbientRotation (HigherYoungActualGraphAssembly.boxSignature a n source) c d = HigherHarmonicYoung.ClebschRotation.tensorAmbientRotation (HigherYoungActualGraphAssembly.boxSignature a n target) c d ∘ₗ self.channel.toLinearMap
- coefficient : ℝ
The coefficient component.
- coefficient_sq : self.coefficient ^ 2 = HigherHierarchyActualBoxSufficiency.boxProbability a b n target source
- axis (x : HigherProjectionInstantiation.SpherePoint n) (v : ↥(HigherHierarchyActualBoxSufficiency.BoxStabilizer n b)) : (LinearMap.adjoint self.channel.toLinearMap) (↑x ⊗ₜ[ℝ] (HigherYoungMovingFibres.movingYoungFibre (HigherYoungActualGraphAssembly.boxSignature a n target) o (fibre target) x) v) = self.coefficient • (HigherYoungMovingFibres.movingYoungFibre (HigherYoungActualGraphAssembly.boxSignature a n source) o (fibre source) x) v
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Data encoding the box lowering projected axis witness construction.
- gram : ℝ
The gram component.
- gram_inner (p q : HigherYoungMovingFibres.YoungVertex (HigherYoungActualGraphAssembly.boxSignature a n) source) : inner ℝ ((HigherHarmonicYoung.youngClebschLower (HigherYoungActualGraphAssembly.boxSignature a n target) (HigherYoungActualGraphAssembly.boxSignature a n source) hdeg row) p) ((HigherHarmonicYoung.youngClebschLower (HigherYoungActualGraphAssembly.boxSignature a n target) (HigherYoungActualGraphAssembly.boxSignature a n source) hdeg row) q) = self.gram * inner ℝ p q
- coefficient : ℝ
The coefficient component.
- coefficient_sq : self.coefficient ^ 2 = self.gram * HigherHierarchyActualBoxSufficiency.boxProbability a b n target source
- projected_axis (v : ↥(HigherHierarchyActualBoxSufficiency.BoxStabilizer n b)) : (HigherHarmonicYoung.projectedCoordinateRaise (HigherYoungActualGraphAssembly.boxSignature a n source) (HigherYoungActualGraphAssembly.boxSignature a n target) hdeg row ↑o) ((fibre target) v) = self.coefficient • (fibre source) v
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Data encoding the box raising projected axis witness construction.
- gram : ℝ
The gram component.
- gram_inner (p q : HigherYoungMovingFibres.YoungVertex (HigherYoungActualGraphAssembly.boxSignature a n) source) : inner ℝ ((HigherHarmonicYoung.youngClebschRaise (HigherYoungActualGraphAssembly.boxSignature a n target) (HigherYoungActualGraphAssembly.boxSignature a n source) hdeg row) p) ((HigherHarmonicYoung.youngClebschRaise (HigherYoungActualGraphAssembly.boxSignature a n target) (HigherYoungActualGraphAssembly.boxSignature a n source) hdeg row) q) = self.gram * inner ℝ p q
- coefficient : ℝ
The coefficient component.
- coefficient_sq : self.coefficient ^ 2 = self.gram * HigherHierarchyActualBoxSufficiency.boxProbability a b n target source
- projected_axis (v : ↥(HigherHierarchyActualBoxSufficiency.BoxStabilizer n b)) : (HigherHarmonicYoung.projectedCoordinateLower (HigherYoungActualGraphAssembly.boxSignature a n source) (HigherYoungActualGraphAssembly.boxSignature a n target) hdeg row ↑o) ((fibre target) v) = self.coefficient • (fibre source) v
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The coherent sector obtained by normalizing a lowering channel from its projected-axis witness.
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The coherent sector obtained by normalizing a raising channel from its projected-axis witness.
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Data encoding the box projected axis witness construction.
- lower {r m n : ℕ} {a : Fin (r + 2) → ℝ} {b : Fin (r + 1) → ℝ} {o : HigherProjectionInstantiation.SpherePoint n} {fibre : (i : HigherYoungActualGraphAssembly.BoxIndex (r + 1) m) → ↥(HigherHierarchyActualBoxSufficiency.BoxStabilizer n b) →ₗᵢ[ℝ] HigherYoungMovingFibres.YoungVertex (HigherYoungActualGraphAssembly.boxSignature a n) i} {target source : HigherYoungActualGraphAssembly.BoxIndex (r + 1) m} {h : 0 < HigherHierarchyActualBoxSufficiency.boxProbability a b n target source} (row : Fin (r + 2)) (hdeg : ∑ i : Fin (r + 1 + 1), HigherYoungActualGraphAssembly.boxSignature a n source i = ∑ i : Fin (r + 1 + 1), HigherYoungActualGraphAssembly.boxSignature a n target i + 1) (data : BoxLoweringProjectedAxisWitness a b o fibre target source h row hdeg) : BoxProjectedAxisWitness a b o fibre target source h
- raise {r m n : ℕ} {a : Fin (r + 2) → ℝ} {b : Fin (r + 1) → ℝ} {o : HigherProjectionInstantiation.SpherePoint n} {fibre : (i : HigherYoungActualGraphAssembly.BoxIndex (r + 1) m) → ↥(HigherHierarchyActualBoxSufficiency.BoxStabilizer n b) →ₗᵢ[ℝ] HigherYoungMovingFibres.YoungVertex (HigherYoungActualGraphAssembly.boxSignature a n) i} {target source : HigherYoungActualGraphAssembly.BoxIndex (r + 1) m} {h : 0 < HigherHierarchyActualBoxSufficiency.boxProbability a b n target source} (row : Fin (r + 2)) (hdeg : ∑ i : Fin (r + 1 + 1), HigherYoungActualGraphAssembly.boxSignature a n target i = ∑ i : Fin (r + 1 + 1), HigherYoungActualGraphAssembly.boxSignature a n source i + 1) (data : BoxRaisingProjectedAxisWitness a b o fibre target source h row hdeg) : BoxProjectedAxisWitness a b o fibre target source h
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Construct a coherent box sector from either a lowering or a raising projected-axis witness.
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Assemble box representation data from coherent sectors, compatible axis identities, and Weyl dimension certificates.
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The box representation data of projected axis witnesses used in the spherical-code argument.
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The adjacent normalized axis coefficient used in the spherical-code argument.
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The predicate asserting rotation invariant.
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- MetricCodes.Spherical.HigherYoungMixedGapLieGram.IsRotationInvariant R W = ∀ (i : I), ∀ v ∈ W, (R i) v ∈ W
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The young rotation family used in the spherical-code argument.
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The Gram operator of the reverse interlacing harmonic branch, its adjoint composed with the branch.
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The positive gelfand tsetlin fischer gram used in the spherical-code argument.
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The canonical gelfand tsetlin fischer gram used in the spherical-code argument.
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The canonical gelfand tsetlin fibre used in the spherical-code argument.
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The canonical box gelfand tsetlin fibre used in the spherical-code argument.
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The difference of row weights corrected by the difference of their indices.
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- MetricCodes.Spherical.HigherYoungArbitraryRowDownstreamCorrection.downstreamShift lam a i = ↑(lam a) - ↑(lam i) + ↑↑i - ↑↑a
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The row derivative recursively corrected by polarizations of derivatives in later rows.
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The finite set of rows strictly after the selected row.
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- MetricCodes.Spherical.HigherHarmonicYoung.ArbitraryRankInternalRowLowerGram.downstreamRows row = {q : Fin (r + 1) | row < q}
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The denominator in a downstream Gram factor, combining truncated weight and row-index differences.
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- MetricCodes.Spherical.HigherHarmonicYoung.ArbitraryRankInternalRowLowerGram.downstreamDenominator lam row q = ↑(lam row - lam q) + ↑(↑q - ↑row)
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The internal row lower gram scalar used in the spherical-code argument.
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Compose upper polarization operators along a row path, with the empty and singleton paths acting identically.
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- MetricCodes.Spherical.HigherHarmonicYoung.ArbitraryRowProjectedLowerOperator.upperPolarizationPath [] = LinearMap.id
- MetricCodes.Spherical.HigherHarmonicYoung.ArbitraryRowProjectedLowerOperator.upperPolarizationPath [head] = LinearMap.id
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The weighted sum of coordinate derivatives followed by upper polarization paths, adjoint to axial raising.
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The ratio of two successive shifted row differences used in the downstream scalar product.
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The finite set of rows strictly greater than i.
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The finite set of rows strictly between i and d.
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The sum of Fischer pairings between row derivatives and their downstream-corrected counterparts.
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Data encoding the genuine lowering fibre axis construction.
- coefficient : ℝ
The coefficient component.
- coefficient_sq : self.coefficient ^ 2 = HigherHarmonicYoung.ArbitraryRankInternalRowLowerGram.internalRowLowerGramScalar (HigherYoungActualGraphAssembly.boxSignature a n source) row * HigherChannel.plusProbability n (HigherYoungActualGraphAssembly.boxSignature a n target) (HigherHierarchy.Weyl.flooredWeight b n) row
- projected_axis (v : ↥(HigherHierarchyActualBoxSufficiency.BoxStabilizer n b)) : (HigherHarmonicYoung.projectedCoordinateRaise (HigherYoungActualGraphAssembly.boxSignature a n source) (HigherYoungActualGraphAssembly.boxSignature a n target) hdeg row ↑o) ((fibre target) v) = self.coefficient • (fibre source) v
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Construct the lowering projected-axis witness from genuine Gelfand–Tsetlin fibre-axis data.
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Construct the raising projected-axis witness from a positive Gram scalar, the minus- probability identity, and the projected-axis identity.
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Construct the raising projected-axis witness from the forward Gelfand–Tsetlin coefficient, the Weyl Gram ratio, and the reverse projected-axis identity.
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Data encoding the canonical box edge axis construction.
- forward : HigherYoungArbitraryRowLoweringProjectedAxisWitness.GenuineLoweringFibreAxisData a b o fibre low high row ⋯
The forward component.
- raisingGram : ℝ
The raising gram component.
- raisingGram_inner (p q : HigherYoungMovingFibres.YoungVertex (HigherYoungActualGraphAssembly.boxSignature a n) low) : inner ℝ ((youngClebschRaise (HigherYoungActualGraphAssembly.boxSignature a n high) (HigherYoungActualGraphAssembly.boxSignature a n low) ⋯ row) p) ((youngClebschRaise (HigherYoungActualGraphAssembly.boxSignature a n high) (HigherYoungActualGraphAssembly.boxSignature a n low) ⋯ row) q) = self.raisingGram * inner ℝ p q
- raisingGram_ratio : self.raisingGram = ArbitraryRankInternalRowLowerGram.internalRowLowerGramScalar (HigherYoungActualGraphAssembly.boxSignature a n high) row * HigherChannel.weylEdgeRatio n (HigherYoungActualGraphAssembly.boxSignature a n low) row
- reverse_range (v : ↥(HigherHierarchyActualBoxSufficiency.BoxStabilizer n b)) : (projectedCoordinateLower (HigherYoungActualGraphAssembly.boxSignature a n low) (HigherYoungActualGraphAssembly.boxSignature a n high) ⋯ row ↑o) ((fibre high) v) ∈ (fibre low).range
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The canonical box projected axis witness used in the spherical-code argument.
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The initial simple-root operators annihilate the fixed-axis raised highest-weight polynomials before the selected row.
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The axial raising map on homogeneous highest-weight space constructed from initial simple- root cancellation.
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The axial raising map on homogeneous highest-weight space for an antitone initial weight.
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The arbitrary row axial lower scalar used in the spherical-code argument.
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The arbitrary row same axis harmonic raise used in the spherical-code argument.
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The adjacent reverse prefix used in the spherical-code argument.
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The adjacent reverse suffix used in the spherical-code argument.
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