Standard parabolic subgroups of a Tits system #
For a subset J of the simple reflections of a Tits system (B, N), the standard parabolic
P_J is generated by B and the simple Bruhat cells indexed by J. Its Bruhat decomposition
consists exactly of the cells B w B with w in the subgroup W_J generated by J in the
Weyl group. In particular, its intersection with N is the inverse image of W_J under
N → W. These statements connect parabolic subgroups of a BN-pair to Weyl-group combinatorics.
The indexing set has type Set T.simple, so every selected generator is a simple reflection.
No finiteness, field, or algebraic-group hypothesis is needed. The empty set gives B, and
the set of all simple reflections gives the ambient group; consequently B is the ambient group
exactly when there are no simple reflections (TauCeti.TitsSystem.subgroupB_eq_top_iff). This
file does not classify all subgroups containing B or identify these abstract subgroups with
subgroup schemes.
The Bruhat cells and their uniqueness are those of
TauCeti.GroupTheory.TitsSystem.Bruhat.Basic and Bruhat.Uniqueness.
References #
- J. E. Humphreys, Linear Algebraic Groups (1975), Section 29.
- T. A. Springer, Linear Algebraic Groups, second edition (1998), Section 8.3.
The standard parabolic subgroup generated by B and the simple Bruhat cells selected by
J. Equivalently, one can adjoin any normalizer representative of each selected reflection.
Instances For
The standard parabolic is the subgroup closure of B and its selected simple cells.
Every standard parabolic contains B.
A selected simple Bruhat cell lies in the standard parabolic.
A standard parabolic is the least subgroup containing B and the selected simple cells.
Enlarging the selected set of simple reflections enlarges the standard parabolic.
Every cell indexed by the Weyl subgroup generated by J lies in P_J.
The Bruhat decomposition of a standard parabolic: an element lies in P_J exactly
when its Bruhat cell is indexed by the Weyl subgroup generated by J.
The standard parabolic is the union of the cells indexed by its Weyl subgroup. The cells
are pairwise disjoint by disjoint_bruhatCell_iff.
On any given Bruhat cell, parabolic membership is exactly membership of its Weyl index in the subgroup generated by the selected simple reflections.
An element of N belongs to P_J exactly when its Weyl class belongs to W_J. Thus
P_J ∩ N is the inverse image of W_J under N → W.
The standard parabolic for the empty set of simple reflections is B.
Selecting every simple reflection gives the whole ambient group.