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TauCeti.Algebra.Lie.HighestWeight.CentralCharacter.Isomorphism

The Harish-Chandra isomorphism #

Let L be a finite-dimensional Lie algebra with non-degenerate Killing form over an algebraically closed field K of characteristic zero, H a Cartan subalgebra and b a base of its root system, with Weyl vector ρ. The Harish-Chandra projection TauCeti.hcProjection b : Z(U(L)) →ₐ[K] S(H) records the central characters, χ_λ(z) = (hcProjection b z)(λ), and lands in the dot-invariants S(H)^{W·}; its linear normalization TauCeti.hcProjectionLinear b, the translate by -ρ, lands in the Weyl invariants S(H)^W. Both are injective (TauCeti.hcProjection_injective) and onto (TauCeti.range_hcProjection and TauCeti.range_hcProjectionLinear). This file packages them as isomorphisms

Z(U(L)) ≃ₐ[K] S(H)^{W·} and Z(U(L)) ≃ₐ[K] S(H)^W

(TauCeti.harishChandraIso and TauCeti.harishChandraLinearIso), and derives the central-character orbit theorem: χ_λ = χ_μ exactly when μ lies in the dot orbit W · λ (TauCeti.vermaCentralCharacter_eq_iff). Given equal central characters, every dot-invariant p is hcProjection b z for a central z, so p takes the same value at λ and μ; since the dot-invariants separate dot orbits (TauCeti.forall_mem_dotInvariants_lift_eq_iff), μ ∈ W · λ.

Main definitions #

Main results #

References #

The isomorphisms #

The linear Harish-Chandra isomorphism Z(U(L)) ≃ₐ[K] S(H)^W: the linear Harish-Chandra projection TauCeti.hcProjectionLinear b, with its values in the Weyl invariants.

Instances For
    @[simp]

    The linear Harish-Chandra isomorphism is the linear Harish-Chandra projection.

    @[simp]

    The inverse of the linear Harish-Chandra isomorphism sends a Weyl invariant to the central element projecting to it.

    The Harish-Chandra isomorphism Z(U(L)) ≃ₐ[K] S(H)^{W·}: the Harish-Chandra projection TauCeti.hcProjection b, with its values in the dot-invariants.

    Instances For
      @[simp]

      The Harish-Chandra isomorphism is the Harish-Chandra projection.

      @[simp]

      The inverse of the Harish-Chandra isomorphism sends a dot-invariant to the central element projecting to it.

      The two Harish-Chandra isomorphisms differ by the translation by -ρ from the dot-invariants to the Weyl invariants: the linear one is the Harish-Chandra isomorphism followed by TauCeti.dotInvariantsEquivLinearInvariants b.

      Inverse filtration #

      @[simp]

      The inverse linear Harish-Chandra isomorphism preserves degrees: a Weyl invariant has degree at most n exactly when the corresponding central element has PBW degree at most n.

      @[simp]

      The inverse Harish-Chandra isomorphism preserves degrees: a dot-invariant has degree at most n exactly when the corresponding central element has PBW degree at most n.

      Central characters and dot orbits #

      Harish-Chandra's theorem on central characters: two weights lam and mu have the same central character, χ_lam = χ_mu, exactly when mu lies in the dot orbit of lam, that is mu = w · lam = w (lam + ρ) - ρ for an element w of the Weyl group.