Chevalley relations for Kostant root-subgroup scheme morphisms #
The divided-power construction represents a root action by an affine group-scheme morphism
𝔾ₐ → GLₙ. This file proves the commuting and class-two Chevalley relations on the
scheme-valued points of those actual morphisms. It transports the universe-polymorphic matrix
relations from ChevalleyRelations.lean through the point comparison proved in Scheme/Basic.lean.
The longer exceptional relation is developed separately in Scheme/Relations/G2/Basic.lean.
Main declarations #
TauCeti.UniversalEnvelopingAlgebra.commute_schemePointsMulEquiv_kostantRootSubgroup: commuting root vectors give commuting scheme-valued root-subgroup points.TauCeti.UniversalEnvelopingAlgebra. commutatorElement_schemePointsMulEquiv_kostantRootSubgroup_of_lie_eq: the class-two Chevalley commutator relation for scheme-valued points.TauCeti.UniversalEnvelopingAlgebra. commutatorElement_schemePointsMulEquiv_kostantRootSubgroup_of_lie_eq': the same relation with the third scheme-valued point written out.
The representation carrier is universe-zero because the current group-scheme reconstruction API requires the base, coordinate Hopf algebra, and comodule to inhabit the same universe.
References #
- R. W. Carter, Simple Groups of Lie Type, Theorem 5.2.2.
- J. E. Humphreys, Introduction to Lie Algebras and Representation Theory, Sections 26--27.
- J. C. Jantzen, Representations of Algebraic Groups, II.1.
Scheme-valued points of represented Kostant root subgroups attached to commuting root vectors commute.
The class-two Chevalley commutator relation on scheme-valued points of represented Kostant
root subgroups. Suppose ⁅eᵢ, eⱼ⁆ = c • eₖ, with eₖ commuting with eᵢ and eⱼ, and
let r have additive parameter c times the product of the parameters of p and q. Then the
matrix commutator of the represented i- and j-root values is the represented k-root value
at r.
The class-two Chevalley commutator relation on scheme-valued points with the third point
written out at parameter c times the product of the parameters of p and q.