OAI/RepresentationTheory/RowColumn/Sectors.lean

GitHub source file

45 declarations, 0 contain sorry, 0 declared as axioms

  1. def OAI.RowColumn.MatrixState.evenAlgebra line 14
  2. lemma OAI.RowColumn.MatrixState.evenAlgebra_mem line 39
  3. lemma OAI.RowColumn.MatrixState.tensorMatrix_even_support line 43
  4. lemma OAI.RowColumn.MatrixState.oddCount_eq line 50
  5. def OAI.RowColumn.MatrixState.sectorTensor line 55
  6. lemma OAI.RowColumn.MatrixState.sectorTensor_mul line 59
  7. lemma OAI.RowColumn.MatrixState.sectorTensor_star line 81
  8. lemma OAI.RowColumn.MatrixState.sectorTensor_one line 89
  9. def OAI.RowColumn.MatrixState.sectorPowerHom line 94
  10. lemma OAI.RowColumn.Signed.frame_pred_congr line 110
  11. lemma OAI.RowColumn.Signed.oddFrame_parity_congr line 122
  12. lemma OAI.RowColumn.Signed.oddPerm_parity_congr line 129
  13. def OAI.RowColumn.FiniteStarAlgebra.unitarySpan line 155
  14. lemma OAI.RowColumn.FiniteStarAlgebra.unitarySpan_eq_span line 171
  15. lemma OAI.RowColumn.FiniteStarAlgebra.unitarySpan_mem line 185
  16. def OAI.RowColumn.FiniteStarAlgebra.unitarySpanHom line 188
  17. lemma OAI.RowColumn.FiniteStarAlgebra.unitarySpanHom_spans line 196
  18. def OAI.RowColumn.MatrixState.discreteContinuousHom line 212
  19. def OAI.RowColumn.MatrixState.precompFunctionHom line 222
  20. lemma OAI.RowColumn.MatrixState.sum_single_function line 231
  21. lemma OAI.RowColumn.MatrixState.function_unitary line 236
  22. theorem OAI.RowColumn.MatrixState.exists_spectral_phase_family line 247

    Source documentation

    A genuine finite spectral phase family inside the prescribed closed star algebra. In the application this is the even one-slot matrix algebra.

    theorem exists_spectral_phase_family {C : Type*} [Fintype C] [DecidableEq C]
        (M : Matrix C C ℂ) (hM : M.IsHermitian)
        (K : StarSubalgebra ℂ (Matrix C C ℂ)) (hK : IsClosed (K : Set (Matrix C C ℂ)))
        (hMK : M ∈ K) :
        ∃ (d : ℕ) (P : Fin d → Matrix C C ℂ) (z : Fin d → ℂ),
          (∑ i, z i • P i) = M ∧ (∀ i, P i ∈ K) ∧
          ∀ θ : Fin d → ℂ, (∀ i, ‖θ i‖=1) → (∑ i, θ i • P i) ∈ unitary (Matrix C C ℂ) := by
    …
  23. lemma OAI.RowColumn.MatrixState.tensorMatrix_linear_combination line 293
  24. def OAI.RowColumn.MatrixState.typeTensor line 303
  25. lemma OAI.RowColumn.MatrixState.tensorMatrix_by_type line 308
  26. def OAI.RowColumn.MatrixState.phaseMatrix line 321
  27. lemma OAI.RowColumn.MatrixState.tensorMatrix_phase line 325
  28. lemma OAI.RowColumn.MatrixState.typeTensor_fourier line 335
  29. theorem OAI.RowColumn.MatrixState.tensorMatrix_mem_phase_span line 353

    Source documentation

    Every identical tensor of a linear combination of a finite family lies in the span of its finite phase tensors. Applied to an even spectral family, all the spanning tensors are genuine global even unitaries.

    theorem tensorMatrix_mem_phase_span (P : J → Matrix C C ℂ) (z : J → ℂ) :
        tensorMatrix (fun _ : S => ∑ j, z j • P j) ∈
          Submodule.span ℂ (Set.range fun θ : Phases J (Fintype.card S) =>
            tensorMatrix (fun _ : S => phaseMatrix P θ)) := by
    …

    Mentions: OAI.RowColumn.MatrixState.tensorMatrix, OAI.RowColumn.MatrixState.phaseMatrix

  30. abbrev OAI.RowColumn.MatrixState.Sector line 379
  31. def OAI.RowColumn.MatrixState.sectorUnitary line 381
  32. def OAI.RowColumn.MatrixState.sectorAlgebra line 385
  33. lemma OAI.RowColumn.MatrixState.sectorUnitary_apply line 388
  34. def OAI.RowColumn.MatrixState.tensorRestriction line 392
  35. lemma OAI.RowColumn.MatrixState.tensorRestriction_apply line 400
  36. theorem OAI.RowColumn.MatrixState.sectorTensor_mem_algebra line 406

    Source documentation

    Identical even positive tensors really belong to the finite algebra of actual global even unitary tensors. This is a proved phase-Fourier identity, not a commutant-duality assumption.

    theorem sectorTensor_mem_algebra (M : Matrix C C ℂ) (hM : M.IsHermitian) (heven : M ∈ evenAlgebra odd) :
        (Matrix.toEuclideanCLM (n := Words (S := S) odd k) (𝕜 := ℂ)) (sectorTensor odd k (fun _ : S => M)) ∈ sectorAlgebra (S := S) odd k := by
    …

    Mentions: OAI.RowColumn.MatrixState.evenAlgebra, OAI.RowColumn.MatrixState.sectorTensor, OAI.RowColumn.MatrixState.sectorAlgebra

  37. abbrev OAI.RowColumn.MatrixState.GlobalTypes line 440
  38. def OAI.RowColumn.MatrixState.sectorTypeMatrix line 442
  39. lemma OAI.RowColumn.MatrixState.sectorTensor_type_expansion line 447
  40. lemma OAI.RowColumn.MatrixState.sectorAlgebra_le_type_span line 456
  41. theorem OAI.RowColumn.MatrixState.sectorAlgebra_finrank line 471

    Source documentation

    Polynomial Fourier algebra dimension, counted by joint word types. No representation-theoretic carrier-dimension estimate is assumed.

    theorem sectorAlgebra_finrank : Module.finrank ℂ (sectorAlgebra (S := S) odd k) ≤
    …

    Mentions: OAI.RowColumn.MatrixState.sectorAlgebra

  42. lemma OAI.RowColumn.MatrixState.sectorTensor_transport line 497
  43. lemma OAI.RowColumn.MatrixState.matrix_wordVector line 503
  44. lemma OAI.RowColumn.MatrixState.tensor_commutes_signed line 509
  45. theorem OAI.RowColumn.MatrixState.sectorAlgebra_commutes line 537

    Source documentation

    The polynomial-dimensional tensor algebra commutes with the genuine signed permutation representation, with no commutant-duality assumption.

    theorem sectorAlgebra_commutes (a : sectorAlgebra (S := S) odd k)
    …

    Mentions: OAI.RowColumn.MatrixState.sectorAlgebra