Geometric connectedness of affine group schemes #
This file compares geometric connectedness of a commutative Hopf algebra with Mathlib's
scheme-theoretic GeometricallyConnected predicate on its Hopf spectrum.
Main declarations #
TauCeti.geometricallyConnectedAffineGroupSchemeProperty: geometric connectedness of the structural morphism as an object property on affine group schemes.TauCeti.geometricallyConnectedCommHopfAlg_iff_geometricallyConnected_hopfSpec: compatibility of the coordinate-ring and scheme-theoretic predicates.TauCeti.geometricallyConnected_iff_geometricallyConnected_coordinate: geometric connectedness of a finite-type affine group scheme in terms of its coordinate algebra.TauCeti.geometricallyConnected_hopfSpec_iff_idempotent_eq_zero_or_one: the idempotent characterization of geometric connectedness for a Hopf spectrum.
References #
- J. S. Milne, Algebraic Groups (2017), §2.a.
This is the geometric-connectedness prerequisite for Layer 3, "Identity component and component group", of the ReductiveGroups roadmap.
The object property on affine group schemes selecting those whose structural morphism is geometrically connected.
Equations
Instances For
Membership in the geometrically connected affine-group-scheme object property.
Geometric connectedness of the structural morphism is invariant under isomorphism of affine group schemes.
Geometric connectedness agrees across the affine-group-scheme and coordinate-ring models. The structural morphism of a Hopf spectrum is geometrically connected if and only if its coordinate algebra is geometrically connected after every field extension.
Under the affine Hopf/group-scheme anti-equivalence, the inverse image of geometric connectedness on affine group schemes is geometric connectedness of coordinate Hopf algebras.
A finite-type affine group scheme has geometrically connected structural morphism exactly when its coordinate algebra supplied by the affine anti-equivalence is geometrically connected.
The structural morphism of a Hopf spectrum is geometrically connected exactly when, after
every extension K / k of the base field, every idempotent of H ⊗[k] K is zero or one.