Definitions/Def_AlgebraicGeometry_ThetaGroupAction.lean
Translations, theta points and Schrödinger frames on abelian schemes
Throughout, S is a commutative ring, f : A \to \operatorname{Spec} S is a morphism of schemes equipped with a relative group law L, and t : \operatorname{Spec} R \to \operatorname{Spec} S is an affine test object; write A_R = A \times_{\operatorname{Spec} S} \operatorname{Spec} R with projections \mathrm{pr} = pullback.fst f t and q = pullback.snd f t, and \mathcal L_R = \mathrm{pr}^*\mathcal L for \mathcal L an object of A.Modules. For a point x of SchemeHomOver t f (a morphism \operatorname{Spec} R \to A over t), translate f L t x is the endomorphism \tau_x of A_R whose first component is the L-product, over the base q \circ t, of the tautological point \mathrm{pr} with x pulled back along q, and whose second component is q; translate_snd records that \tau_x is a morphism over \operatorname{Spec} R.
A term of ThetaPt f L 𝓛 t is a pair consisting of such a point pt together with an isomorphism iso of modules \tau_{\mathrm{pt}}^*\mathcal L_R \cong \mathcal L_R; no further condition (invertibility of \mathcal L, membership of the kernel, normalisation) is imposed. For such a \theta, ThetaPt.act θ s sends a global section s of \mathcal L_R to the image under the forward component of iso of the pullback of s along \tau_{\mathrm{pt}}, the two relevant open sets \tau_{\mathrm{pt}}^{-1}(\top) and \top being the same. baseScalar f t r is the global function on A_R obtained from r \in R through \Gamma(\operatorname{Spec} R) \cong R and q.
Finally, for \delta : \mathrm{Fin}\,g \to \mathbb N with all \delta_i nonzero and H = \prod_i \mathbb Z/\delta_i, a SchrodingerFrame consists of sections \sigma_h of \mathcal L_R indexed by h \in H such that c \mapsto \sum_h \mathrm{baseScalar}(c_h)\,\sigma_h is a bijection R^H \to \Gamma(\mathcal L_R,\top), together with theta points \theta_h for h \in H and \eta_\chi for each additive character \chi : H \to R, subject to the two families of equations \theta_h \cdot \sigma_{h'} = \sigma_{h+h'} and \eta_\chi \cdot \sigma_h = \chi(h)\,\sigma_h. Only these identities are required: the assignments h \mapsto \theta_h and \chi \mapsto \eta_\chi are not asked to be homomorphisms, and no group structure on theta points is introduced.
Relation to Mathlib
Mathlib has no theta groups or theta structures for abelian schemes; these definitions are the project's own, formulated on top of Mathlib's sheaves of modules on a scheme and the project's relative group laws and pullbacks of local sections.
Where it is used
These are the vocabulary items for theta rigidifications of polarised abelian schemes of type \delta: a Schrödinger frame is exactly a basis of sections of the polarisation bundle on which chosen lifts of the two Lagrangian subgroups of the kernel act by the standard translation and character formulae, which is what the fine moduli statements for polarised abelian schemes of a given type are phrased against.
References
- D. Mumford, On the equations defining abelian varieties I, Inventiones Mathematicae 1 (1966), 287–354
- D. Mumford, Abelian Varieties, Tata Institute of Fundamental Research Studies in Mathematics 5, Oxford University Press, 1970
References are suggested automatically and have not been individually verified.
English text generated automatically from the Lean source; the Lean statement is authoritative.
- 72 lines
- 15 declarations
- used in the statements of 4 theorems and imported by 2 proofs
- imports 2 definition modules
Source file: Definitions/Def_AlgebraicGeometry_ThetaGroupAction.lean
Imports
Declarations
- def
AlgebraicGeometry.Polarisation.translate - theorem
AlgebraicGeometry.Polarisation.translate_snd - structure
AlgebraicGeometry.Polarisation.ThetaPt - field
AlgebraicGeometry.Polarisation.ThetaPt.t - field
AlgebraicGeometry.Polarisation.ThetaPt.pt - field
AlgebraicGeometry.Polarisation.ThetaPt.iso - def
AlgebraicGeometry.Polarisation.ThetaPt.act - def
AlgebraicGeometry.Polarisation.baseScalar - structure
AlgebraicGeometry.Polarisation.SchrodingerFrame - field
AlgebraicGeometry.Polarisation.SchrodingerFrame.t - field
AlgebraicGeometry.Polarisation.SchrodingerFrame.basis - field
AlgebraicGeometry.Polarisation.SchrodingerFrame.lift - field
AlgebraicGeometry.Polarisation.SchrodingerFrame.dualLift - field
AlgebraicGeometry.Polarisation.SchrodingerFrame.lift_act - field
AlgebraicGeometry.Polarisation.SchrodingerFrame.dualLift_act
Source
import Definitions.Def_AlgebraicGeometry_PolarisedAbelianSchemeOfType import Definitions.Def_AlgebraicGeometry_ModulesPullbackLocalSection set_option autoImplicit false noncomputable section universe u open CategoryTheory CategoryTheory.Limits MonoidalCategory AlgebraicGeometry NeronModelInfra GoodReductionJacobian namespace AlgebraicGeometry.Polarisation variable {S : Type u} [CommRing S] {A : Scheme.{u}} (f : A ⟶ Spec (CommRingCat.of S)) (L : RelativeGroupLaw S f) def translate {R : Type u} [CommRing R] (t : Spec (CommRingCat.of R) ⟶ Spec (CommRingCat.of S)) (x : SchemeHomOver t f) : pullback f t ⟶ pullback f t := pullback.lift (L.mul (pullback.snd f t ≫ t) ⟨pullback.fst f t, pullback.condition⟩ (schemeHomOverComp (pullback.snd f t) rfl x)).1 (pullback.snd f t) (L.mul (pullback.snd f t ≫ t) ⟨pullback.fst f t, pullback.condition⟩ (schemeHomOverComp (pullback.snd f t) rfl x)).2 theorem translate_snd {R : Type u} [CommRing R] (t : Spec (CommRingCat.of R) ⟶ Spec (CommRingCat.of S)) (x : SchemeHomOver t f) : translate f L t x ≫ pullback.snd f t = pullback.snd f t := pullback.lift_snd _ _ _ structure ThetaPt (𝓛 : A.Modules) {R : Type u} [CommRing R] (t : Spec (CommRingCat.of R) ⟶ Spec (CommRingCat.of S)) where pt : SchemeHomOver t f iso : (Scheme.Modules.pullback (translate f L t pt)).obj ((Scheme.Modules.pullback (pullback.fst f t)).obj 𝓛) ≅ (Scheme.Modules.pullback (pullback.fst f t)).obj 𝓛 namespace ThetaPt variable {f} {L} {𝓛 : A.Modules} {R : Type u} [CommRing R] {t : Spec (CommRingCat.of R) ⟶ Spec (CommRingCat.of S)} def act (θ : ThetaPt f L 𝓛 t) (s : Γ((Scheme.Modules.pullback (pullback.fst f t)).obj 𝓛, ⊤)) : Γ((Scheme.Modules.pullback (pullback.fst f t)).obj 𝓛, ⊤) := (θ.iso.hom.app ((translate f L t θ.pt) ⁻¹ᵁ ⊤) (Scheme.Modules.pullbackLocalSection (translate f L t θ.pt) s) : Γ((Scheme.Modules.pullback (pullback.fst f t)).obj 𝓛, (translate f L t θ.pt) ⁻¹ᵁ ⊤)) end ThetaPt def baseScalar {R : Type u} [CommRing R] (t : Spec (CommRingCat.of R) ⟶ Spec (CommRingCat.of S)) (r : R) : Γ(pullback f t, ⊤) := (pullback.snd f t).appTop.hom ((Scheme.ΓSpecIso (CommRingCat.of R)).inv.hom r) structure SchrodingerFrame (𝓛 : A.Modules) {R : Type u} [CommRing R] (t : Spec (CommRingCat.of R) ⟶ Spec (CommRingCat.of S)) {g : ℕ} (δ : Fin g → ℕ) [∀ i, NeZero (δ i)] where σ : ((i : Fin g) → ZMod (δ i)) → Γ((Scheme.Modules.pullback (pullback.fst f t)).obj 𝓛, ⊤) basis : Function.Bijective fun c : ((i : Fin g) → ZMod (δ i)) → R => ∑ h, baseScalar f t (c h) • σ h lift : ((i : Fin g) → ZMod (δ i)) → ThetaPt f L 𝓛 t dualLift : AddChar ((i : Fin g) → ZMod (δ i)) R → ThetaPt f L 𝓛 t lift_act : ∀ h h', (lift h).act (σ h') = σ (h + h') dualLift_act : ∀ χ h, (dualLift χ).act (σ h) = baseScalar f t (χ h) • σ h end AlgebraicGeometry.Polarisation end
Statements phrased using this module (4)
- Étale-local existence of Schrödinger frames of type δ
AlgebraicGeometry.PolarisedAbelianScheme.exists_schrodingerFrame_of_rootedSymmetricOfType1,326 below · depth 30 - Theta points realising arbitrary additive characters of H(δ)
AlgebraicGeometry.Polarisation.ThetaPt.exists_forall_act_eq_baseScalar_addChar_smul_of_forall_addMonoidHom13 below · depth 31 - Gluing theta points along a complete orthogonal family of idempotents
AlgebraicGeometry.Polarisation.ThetaPt.exists_pt_eq_comp_act_eq_of_isIdempotentElem_of_sum_eq_one8 below · depth 32 - Faithfulness of R on global sections of the pulled-back polarisation
AlgebraicGeometry.PolarisedAbelianScheme.eq_zero_of_forall_baseScalar_smul_eq_zero54 below · depth 35