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TauCeti.NumberTheory.ClassFieldTheory.Global.LiftIndependence

Lifts of idele-class cohomology to the ideles and their local invariants #

Let K be a number field and L/F a finite Galois layer inside Kˢ. The global invariant of a class of H²(Gal(L/F), C_L) is to be the sum of the local invariants ideleSumLocalInv of a lift of it to H²(Gal(L'/F), I_{L'}), for a refinement L'/F of the layer where such a lift exists. This file shows that two such lifts, to two refinements, have the same sum of local invariants up to the sum of the local invariants of a global Brauer class.

The comparison runs through the multiplicative group. The sum of the local invariants of the image of a class y ∈ H²(Gal(L/F), Lˣ) under the principal ideles is the sum of the local invariants of a global Brauer class, namely of the class of y in Br K obtained by inflation to the ground subgroup and corestriction to G_K (ideleSumLocalInv_multiplicativeToIdeleH2). This holds because inflation and corestriction are natural in the coefficient module (ideleLayerCorInfl_multiplicativeToIdeleH2), and because the localization of idele cohomology extends the localization of Brauer classes along the principal ideles (ideleLocalization_principalIdele).

Two lifts y₁, y₂ to refinements L₁/F and L₂/F of one class are inflated to a common refinement M/F (LayerRefinement.exists_commonRefinement). There they have the same image in H²(Gal(M/F), C_M), since the comparison with idele classes commutes with inflation (ideleToClassH2_cohomologyInfl), so they differ by the image of a class of H²(Gal(M/F), Mˣ) (ker_ideleToClassH2). Since inflation preserves the sum of the local invariants (ideleSumLocalInv_infl), the sums for y₁ and y₂ differ by the sum of the local invariants of a global Brauer class (exists_ideleSumLocalInv_eq_add_sumLocalInv_of_ideleToClassH2_eq). Together with the reciprocity law of the global Brauer sequence, that the local invariants of a global Brauer class sum to zero, this makes the sum of the local invariants of a lift independent of the lift and of the refinement.

Main definitions #

Main results #

References #

The class over the absolute Galois group of a multiplicative class #

The class over G_K of a units-layer class: for a layer V ◁ U of the units formation, inflation H²(U ⧸ V, ((Kˢ)ˣ)^V) → H²(U, (Kˢ)ˣ) followed by corestriction from the open subgroup U to G_K. In field notation it carries H²(Gal(L/F), Lˣ) to Br K.

Instances For

    The class over G_K of a units-layer class is the corestriction of its inflation.

    Inflation and corestriction commute with the principal ideles: the class over G_K of the image of y ∈ H²(Gal(L/F), Lˣ) in H²(Gal(L/F), I_L) is the image along the principal ideles (Kˢ)ˣ → I_{Kˢ} of the class of y over G_K.

    The local invariants of a principal class are those of a global Brauer class: the sum of the local invariants of the image of y ∈ H²(Gal(L/F), Lˣ) in H²(Gal(L/F), I_L) is the sum of the local invariants of the class of y in Br K.

    Two lifts of one idele-class class #

    theorem TauCeti.ClassFieldTheory.exists_ideleSumLocalInv_eq_add_sumLocalInv_of_ideleToClassH2_eq (K : Type) [Field K] [NumberField K] {Lay Lay₁ Lay₂ : NormalLayer (AbsoluteGaloisGroup K)} (T₁ : LayerRefinement Lay Lay₁) (T₂ : LayerRefinement Lay Lay₂) (x : ↑(Lay.H (globalFormation K) 2)) (y₁ : ↑(Lay₁.H (ideleFormation K) 2)) (y₂ : ↑(Lay₂.H (ideleFormation K) 2)) (h₁ : (ideleToClassH2 K Lay₁) y₁ = (CategoryTheory.ConcreteCategory.hom (T₁.cohomologyInfl (globalFormation K) 2)) x) (h₂ : (ideleToClassH2 K Lay₂) y₂ = (CategoryTheory.ConcreteCategory.hom (T₂.cohomologyInfl (globalFormation K) 2)) x) :
    ∃ (b : Br K), (ideleSumLocalInv K Lay₁) y₁ = (ideleSumLocalInv K Lay₂) y₂ + (sumLocalInv K) ((brLocalization K) b)

    Two lifts of one idele-class class have the same local invariants up to a global class. Let y₁ and y₂ lift the inflations of one class x ∈ H²(Gal(L/F), C_L) to refinements L₁/F and L₂/F of its layer. Then the sums of the local invariants of y₁ and y₂ differ by the sum of the local invariants of a global Brauer class b ∈ Br K.