The localizations of a relative Brauer class and the cohomology of the ideles #
Let L/K be a finite Galois extension of number fields with Galois group G, embedded in Kˢ
by σ. A class x ∈ H²(G, Lˣ) gives the Brauer class relBrInfl K L σ x ∈ Br K, whose
localization at a place v of K is its base change to the completion K_v. It also gives,
through the principal ideles Lˣ → I_L (unitsToIdeles), a class of H²(G, I_L), which has a
semi-local component in H²(G, (K_v ⊗[K] L)ˣ) at every place v, finite
(idelesToSemilocalUnits) or infinite (idelesToInfiniteSemilocalUnits). This file shows that
the two families carry the same information: the semi-local component of x at v vanishes
exactly when the localization of its Brauer class at v does. Hence the image of x in
H²(G, I_L) vanishes exactly when every localization of its Brauer class vanishes
(map_unitsToIdeles_eq_zero_iff_brLocalization_eq_zero).
This is the idelic half of the injectivity of Br K → ⨁_v Br K_v (Albert–Brauer–Hasse–Noether):
a split class with trivial localizations dies in H²(G, I_L), so by the exact sequence
1 → Lˣ → I_L → C_L → 1 it comes from H¹(G, C_L).
The comparison at a place v goes through Shapiro's lemma. For a place w of L above v, the
semi-local units are coinduced from the units of the completion L_w as a representation of the
decomposition group D_w (semilocalUnitsCoindIso, infiniteSemilocalUnitsCoindIso), so the
semi-local component of x is determined by its restriction to D_w, read in L_wˣ
(groupCohomology.map_id_eq_zero_iff_of_comp_eq_resCoindToHom). The decomposition group is
the Galois group of L_w/K_v (decompositionHom), and there the restriction is the map
H²(Gal(L/K), Lˣ) → H²(Gal(L_w/K_v), L_wˣ) along restriction of automorphisms and the inclusion
Lˣ → L_wˣ (map_unitsToIdeles_idelesToSemilocalUnits_eq_zero_iff). That map is how base change
to K_v acts on inflated Brauer classes (brBaseChange_relBrInfl), and inflation into Br K_v is
injective (relBrInfl_injective).
Main results #
TauCeti.ClassFieldTheory.map_unitsToIdeles_idelesToSemilocalUnits_eq_zero_iff,TauCeti.ClassFieldTheory.map_unitsToIdeles_idelesToInfiniteSemilocalUnits_eq_zero_iff: in every degree, the semi-local component of a class ofHⁿ(G, Lˣ)at a finite or infinite placevvanishes exactly when its image inHⁿ(Gal(L_w/K_v), L_wˣ)does.map_unitsToIdeles_idelesToSemilocalUnits_eq_zero_iff_brBaseChange_eq_zero,map_unitsToIdeles_idelesToInfiniteSemilocalUnits_eq_zero_iff_brBaseChange_eq_zero: in degree two, it vanishes exactly when the localization atvof the Brauer class does.TauCeti.ClassFieldTheory.map_unitsToIdeles_eq_zero_iff_brLocalization_eq_zero: the image ofx ∈ H²(G, Lˣ)inH²(G, I_L)vanishes exactly when every localization ofrelBrInfl K L σ xvanishes.
References #
- J. S. Milne, Class Field Theory, Chapter VII, Lemma 2.4 and Proposition 2.5, and Chapter VIII, §4.
- J. Tate, Global class field theory, in J. W. S. Cassels and A. Fröhlich (eds.), Algebraic Number Theory, Chapter VII, §§6–7.
The semi-local component of a class of Hⁿ(Gal(L/K), Lˣ) at a finite place v vanishes
exactly when the class vanishes in Hⁿ(Gal(L_w/K_v), L_wˣ), for any place w of L above v,
along restriction of automorphisms and the inclusion Lˣ → L_wˣ.
The semi-local component of a class of H²(Gal(L/K), Lˣ) at a finite place v vanishes
exactly when the localization at v of its Brauer class vanishes.
The semi-local component of a class of Hⁿ(Gal(L/K), Lˣ) at an infinite place v
vanishes exactly when the class vanishes in Hⁿ(Gal(L_w/K_v), L_wˣ), for any place w of L
above v, along restriction of automorphisms and the inclusion Lˣ → L_wˣ.
The semi-local component of a class of H²(Gal(L/K), Lˣ) at an infinite place v
vanishes exactly when the localization at v of its Brauer class vanishes.
All places together #
A split Brauer class has trivial localizations exactly when it dies in the cohomology of the
ideles. For L/K finite Galois, embedded in Kˢ by σ, a class x ∈ H²(Gal(L/K), Lˣ) maps to
zero in H²(Gal(L/K), I_L) under the principal ideles exactly when every localization of the
Brauer class relBrInfl K L σ x, at the finite and at the infinite places, vanishes.