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TauCeti.Geometry.Hodge.Semisimple

Polarizable pure Hodge structures are semisimple #

A polarization splits off every rational Hodge substructure, so the lattice of rational Hodge substructures of a polarizable pure Hodge structure is complemented. Over a finite-dimensional rational space that lattice is also modular and satisfies the descending chain condition, and the two properties together give the classical decomposition: a polarizable pure Hodge structure is the direct sum of finitely many simple rational Hodge substructures — the atoms of the lattice — independent and spanning.

The complement itself is the orthogonal complement TauCeti.Hodge.RationalHodgeSubstructure.orthogonal for a polarizing form; the decomposition is then the lattice-theoretic TauCeti.exists_finset_isAtom_sup_eq, which splits off one atom at a time in any complemented modular lattice with the descending chain condition. Only some polarizing form is used, never a chosen one, so the statements are about TauCeti.Hodge.IsPolarizable structures: this is the semisimplicity of the polarizable Hodge structures, for which the choice of a form is not part of the object. Categorically, every monomorphism of polarizable rational Hodge structures corestricts to an isomorphism onto its rational image. The orthogonal retraction of that image therefore splits the original monomorphism, making TauCeti.Hodge.PolarizableHodgeStructureCat a SplitMonoCategory. The finite independent family of atoms also assembles through categorical biproducts, so every object is isomorphic to a finite biproduct of simple objects.

Following Voisin, Hodge Theory and Complex Algebraic Geometry I, §7.1.2, and Peters–Steenbrink, Mixed Hodge Structures, §2.

Main declarations #

theorem TauCeti.Hodge.RationalHodgeSubstructure.complementedLattice {Vℤ : Type u} {Vℚ : Type v} {Vℂ : Type w} [AddCommGroup Vℤ] [AddCommGroup Vℚ] [Module ℚ Vℚ] [AddCommGroup Vℂ] [Module ℂ Vℂ] {ιℚ : Vℤ →ₗ[ℤ] Vℚ} {ιℂ : Vℤ →ₗ[ℤ] Vℂ} {hℚ : IsBaseChange ℚ ιℚ} {hℂ : IsBaseChange ℂ ιℂ} {n : ℤ} {hs : HodgeStructure hℂ n} [Module.Finite ℚ Vℚ] (P : Polarization hℂ hs) :

A polarization makes the lattice of rational Hodge substructures complemented: the orthogonal complement for its form is a lattice complement.

theorem TauCeti.Hodge.RationalHodgeSubstructure.complementedLattice_of_isPolarizable {Vℤ : Type u} {Vℚ : Type v} {Vℂ : Type w} [AddCommGroup Vℤ] [AddCommGroup Vℚ] [Module ℚ Vℚ] [AddCommGroup Vℂ] [Module ℂ Vℂ] {ιℚ : Vℤ →ₗ[ℤ] Vℚ} {ιℂ : Vℤ →ₗ[ℤ] Vℂ} {hℚ : IsBaseChange ℚ ιℚ} {hℂ : IsBaseChange ℂ ιℂ} {n : ℤ} {hs : HodgeStructure hℂ n} [Module.Finite ℚ Vℚ] (h : IsPolarizable hℂ hs) :

Every rational Hodge substructure of a polarizable pure Hodge structure is a direct summand: the lattice of rational Hodge substructures is complemented.

theorem TauCeti.Hodge.RationalHodgeSubstructure.exists_finset_isAtom_sup_eq {Vℤ : Type u} {Vℚ : Type v} {Vℂ : Type w} [AddCommGroup Vℤ] [AddCommGroup Vℚ] [Module ℚ Vℚ] [AddCommGroup Vℂ] [Module ℂ Vℂ] {ιℚ : Vℤ →ₗ[ℤ] Vℚ} {ιℂ : Vℤ →ₗ[ℤ] Vℂ} {hℚ : IsBaseChange ℚ ιℚ} {hℂ : IsBaseChange ℂ ιℂ} {n : ℤ} {hs : HodgeStructure hℂ n} [Module.Finite ℚ Vℚ] (P : Polarization hℂ hs) (W : RationalHodgeSubstructure hℚ hs) :
∃ (s : Finset (RationalHodgeSubstructure hℚ hs)), (∀ U ∈ s, IsAtom U) ∧ s.SupIndep id ∧ s.sup id = W

Every rational Hodge substructure of a polarized pure Hodge structure is a finite direct sum of simple substructures: it is the supremum of a finite independent family of atoms of the lattice of rational Hodge substructures.

theorem TauCeti.Hodge.exists_finset_isAtom_sup_eq_top {Vℤ : Type u} {Vℚ : Type v} {Vℂ : Type w} [AddCommGroup Vℤ] [AddCommGroup Vℚ] [Module ℚ Vℚ] [AddCommGroup Vℂ] [Module ℂ Vℂ] {ιℚ : Vℤ →ₗ[ℤ] Vℚ} {ιℂ : Vℤ →ₗ[ℤ] Vℂ} {hℂ : IsBaseChange ℂ ιℂ} {n : ℤ} {hs : HodgeStructure hℂ n} [Module.Finite ℚ Vℚ] (hℚ : IsBaseChange ℚ ιℚ) (h : IsPolarizable hℂ hs) :
∃ (s : Finset (RationalHodgeSubstructure hℚ hs)), (∀ U ∈ s, IsAtom U) ∧ s.SupIndep id ∧ s.sup id = ⊤

Semisimplicity of polarizable pure Hodge structures. A polarizable pure Hodge structure on a finite-dimensional rational space is the direct sum of finitely many simple rational Hodge substructures: there is a finite independent family of atoms of the lattice of rational Hodge substructures whose supremum is everything.

Categorical semisimplicity of polarizable rational Hodge structures. Every monomorphism splits. The splitting is obtained by identifying the source with the rational image and then using the orthogonal retraction of that image in the target.

Decomposition into simple objects #

The canonical map from the biproduct of a finite family of rational Hodge substructures to the ambient Hodge structure.

Instances For
    @[simp]

    The canonical map out of the biproduct restricts on each summand to the inclusion of the corresponding rational Hodge substructure.

    @[simp]

    The canonical map out of the biproduct restricts on each summand to the inclusion of the corresponding rational Hodge substructure.

    A nonzero morphism into the object induced by an atomic rational Hodge substructure is surjective on rational carriers.

    An atom of the lattice of rational Hodge substructures gives a simple object of the category of polarizable rational Hodge structures.

    The map from the ambient object to the biproduct given by projection onto each member of an independent spanning family along the supremum of the other members.

    Instances For
      @[simp]

      Each component of the lift from an independent spanning family is projection along the supremum of the other substructures.

      @[simp]

      Each component of the lift from an independent spanning family is projection along the supremum of the other substructures.

      @[simp]

      The canonical map out of an independent spanning biproduct followed by its projection map is the identity.

      @[simp]

      The canonical map out of an independent spanning biproduct followed by its projection map is the identity.

      The canonical map from an independent spanning biproduct is surjective on rational carriers.

      The canonical map from an independent spanning biproduct is an isomorphism.

      An independent finite family of rational Hodge substructures spanning the ambient structure gives an isomorphism from their biproduct to the ambient object.

      Instances For
        @[simp]

        The forward map of the biproduct isomorphism is the canonical map induced by the substructure inclusions.

        @[simp]

        The inverse of the biproduct isomorphism is the lift of the complementary retractions.

        The isomorphism from an independent spanning family restricts on each summand to its substructure inclusion.

        The isomorphism from an independent spanning family restricts on each summand to its substructure inclusion.

        Each component of the inverse of the biproduct isomorphism is projection along the supremum of the other substructures.

        Each component of the inverse of the biproduct isomorphism is projection along the supremum of the other substructures.

        Categorical semisimplicity of polarizable rational Hodge structures. Every object is isomorphic to a finite biproduct of simple objects induced by rational Hodge substructures.