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Equality, inclusion and intersection of spherical cosets, and the quotient poset

Statement

Let (S,m), W, ℓ, S, the parabolics WT and the poset WS be as in Spherical subsets, the nerve, the poset of spherical cosets, and the Davis realization; keep the convention that S(w) is the set of letters of any reduced expression of w (Support, intrinsic parabolic presentations, minimal coset representatives and length additivity, with the type-A identification (1)). Let T,T′∈S and w,w′∈W.

(1) Equality. wWT=w′WT′ if and only if T=T′ and w−1w′∈WT. Hence the projection π ⁣:WS→S, wWT↦T, is well-defined, the members of WS are exactly the left cosets of the subgroups WT (T∈S), and the left cosets of any one WT are pairwise disjoint while cosets of distinct parabolics are distinct.

(2) Inclusion. wWT⊆w′WT′ if and only if T⊆T′ and w−1w′∈WT′ (equivalently w∈w′WT′, equivalently wWT′=w′WT′). In particular WT⊆WT′ if and only if T⊆T′.

(3) Intersections are parabolic cosets. If wWT∩w′WT′≠∅, then wWT∩w′WT′=uWT∩T′for every u∈wWT∩w′WT′; moreover wWT∩w′WT′≠∅ if and only if w−1w′∈WTWT′, where WTWT′={ab:a∈WT, b∈WT′}. Thus the meet of two spherical cosets in the inclusion order, when their intersection is nonempty, is that intersection coset, of type T∩T′; disjoint spherical cosets have no common lower bound in WS.

(4) The quotient poset. The left action of (4) of Spherical subsets, the nerve, the poset of spherical cosets, and the Davis realization is order-preserving and π-invariant, and it is transitive on the cosets of each fixed parabolic; the induced map of posets W\WS→S is an isomorphism. Consequently the action on WS is free on the minimal elements wW∅.

Facts & Assumptions

Given: A finite Coxeter matrix (S,m) with presented group W and length ℓ; spherical subsets T,T′∈S; elements w,w′∈W.

[F3]

Intersections of standard parabolic subgroups: WI∩WJ=WI∩J for all I,J⊆S (Intersections of standard parabolics, the parabolic root subsystem, and global minimality of coset representatives (1)).

[F4]

Multiplication in W is associative, has identity 1, and every element has a two-sided inverse (Group and abelian group).

[F5]

The spherical subsets are downward closed and W∅={1} (Spherical subsets, the nerve, the poset of spherical cosets, and the Davis realization (1)).

[L1]

Coset membership and equality: for a subgroup H≤G and a,b∈G, one has b∈aH if and only if a−1b∈H, and aH=bH if and only if a−1b∈H (x∈aH iff a−1x∈H, and aH=bH iff a−1b∈H).

[L2]

A left coset of H≤G is the set gH={gh:h∈H} (Left and right cosets gH and Hg of a subgroup).

[L3]

Every subgroup contains the identity and is closed under products and inverses (Subgroup).

Proof

technique · direct
1.1givenF2L1L2L3algebra

Suppose wWT=w′WT′. Since 1∈WT and 1∈WT′ by [L3], the element w lies in wWT=w′WT′ and w′ lies in w′WT′=wWT; by [L1] this gives w−1w′∈WT′ and w′−1w∈WT. Left-multiplying the coset equality by w−1 and using (w−1w)WT=WT and (w−1w′)WT′=uWT′ with u:=w−1w′ gives WT=uWT′; since u−1=w′−1w∈WT by [L3], also WT′=u−1WT=WT. Intersecting with S and applying [F2] yields T=T′, and w−1w′=u∈WT′=WT.

1.2givenL1algebra

Conversely, if T=T′ and w−1w′∈WT, then w′∈wWT by [L1], so w′WT=wWT by [L1]; together with T=T′ this is wWT=w′WT′.

1.3givenF2L1L2L3algebra

Suppose wWT⊆w′WT′. Then w∈w′WT′, so w−1w′∈WT′ by [L1]; left-multiplying the inclusion by w−1 gives WT=w−1(wWT)⊆w−1(w′WT′)=(w−1w′)WT′=WT′ by [L3]. Hence T=WT∩S⊆WT′∩S=T′ by [F2].

1.4givenF1F2L1L2algebra

Conversely, if T⊆T′ and w−1w′∈WT′, then WT≤WT′ by [F1], so wWT⊆wWT′=w′WT′ by [L2]. This also covers the two reformulations: w∈w′WT′ is equivalent to w−1w′∈WT′ by [L1], and wWT′=w′WT′ is equivalent to w−1w′∈WT′ by [L1] applied with T=T′. Taking w=w′=1 gives WT⊆WT′ if and only if T⊆T′.

1.5givenF3F4L1L2algebra

Assume u∈wWT∩w′WT′. Then uWT=wWT and uWT′=w′WT′ by [L1]. Left multiplication by u is a bijection with inverse left multiplication by u−1, by [F4], so it takes intersections to intersections; hence wWT∩w′WT′=uWT∩uWT′=u(WT∩WT′)=uWT∩T′, the last equality by [F3].

1.6givenF4L2L3algebra

The intersection is nonempty if and only if w−1w′∈WTWT′: indeed wWT∩w′WT′≠∅ means that wa=w′b for some a∈WT, b∈WT′, which is equivalent by the group laws [F4] to w−1w′=ab−1∈WTWT′ because WT′ is closed under inverses by [L3].

2.1step 1.1step 1.2L1

The projection π is well-defined by [step 1.1]; for fixed T the criterion wWT=w′WT  ⟺  w−1w′∈WT is [step 1.1] and [step 1.2] together; and two cosets of WT are disjoint when they are unequal, since if u lies in both then wWT=uWT=w′WT by [L1]. Thus the members of WS are exactly the left cosets of the subgroups WT (T∈S).

2.2step 1.5F5givenalgebra

The meet statement of (3): by [step 1.5] the intersection p=wWT∩w′WT′ of two cosets is a member of WS when nonempty, with π(p)=T∩T′ (spherical, since T∩T′⊆T∈S and S is downward closed by [F5]); it is contained in both cosets, so it is a lower bound. If r=vWV∈WS satisfies r⊆wWT and r⊆w′WT′, then r⊆p by definition of intersection. Hence p is the greatest lower bound, and no member of WS is contained in two disjoint cosets because members of WS are nonempty.

2.3step 1.1step 1.3step 1.4F4algebra

The quotient poset of (4): left multiplication is order-preserving and π-invariant because (v⋅wWT)=(vw)WT has type T ([step 1.1]); it is transitive on the cosets of a fixed parabolic, as v:=w′w−1 sends wWT to w′WT by [F4]. The induced map πˉ ⁣:W\WS→S is well-defined by π-invariance, surjective because the orbit of WT has type T, and injective because two cosets of type T are wWT and w′WT, and v:=w′w−1 carries the first to the second. It preserves order: if orbits satisfy [q]≤[q′] with representatives vq⊆v′q′, then [step 1.3] gives π(vq)⊆π(v′q′) in S; it reflects order: if T⊆T′, then WT⊆WT′ by [step 1.4], so the corresponding orbits are comparable. Hence πˉ is an isomorphism of posets.

3.1F2F4F5L2L3step 1.1step 1.3step 2.3given∎

The minimal elements of WS are exactly the singletons wW∅={w}. If T≠∅, choose s∈T. By [F2], s∈WT and W∅∩S=∅; with [F5] and 1∈WT by [L3], this gives s∉W∅ and W∅={1}⊊WT, hence wW∅⊊wWT. Conversely, if vWV⊆wW∅, then [step 1.3] gives V⊆∅, so V=∅; the inclusion of singletons is equality, and [step 1.1] gives v=w. The action is free on them because v⋅wW∅=wW∅ forces vw=w and hence v=1 by [F4]. This completes (1)-(4). No Choice is used: every argument is set algebra in the fixed group W and the finite set S.

Depends on

Used by

Cited to discharge well-definedness by Spherical subsets, the nerve, the poset of spherical cosets, and the Davis realization.

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