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Orbit dimension and closed orbits for complex group actions

Statement

Assume the Axiom of Choice inherited from the orbit and dimension suppliers. Let G be a complex affine algebraic group acting algebraically on a classical variety X (Classical complex affine algebraic actions and rational modules), and let x∈X. Then: (a) Gx and (G∘)x have the same dimension, the orbit Gx is a finite union of G∘-orbits of common dimension dim⁡G∘−dim⁡Gx, and dim⁡G=dim⁡Gx+dim⁡Gx; (b) every irreducible component of the orbit closure Gx‾ has dimension dim⁡Gx, and Gx‾ is the union of Gx and of orbits of strictly smaller dimension; (c) every orbit of minimal dimension in X is closed, and every orbit closure contains a closed orbit. Assertion (c) is the input used later for the unique closed orbit in a quotient fibre.

Facts & Assumptions

Given: AC; a complex affine algebraic group G acting algebraically on a classical variety X; a point x∈X with orbit Gx and stabilizer Gx.

[F1]

Stabilizer and orbit map fibres. For a finite-type group scheme G acting on a separated finite-type scheme X and a closed point x, the scheme-theoretic stabilizer H=Gx is a closed subgroup scheme, and for g0∈G(k) the fibre of the orbit map over g0x is g0H with Ggx=gHg−1 (Fibres of the orbit map and the scheme-theoretic stabilizer as a closed subgroup scheme). Read in the classical register, Gx is a closed subgroup of the complex affine algebraic group G.

[F2]

Local closedness and connected orbit dimension. Assume AC, let G be a connected smooth finite-type group over an algebraically closed field acting on a classical variety X, and let x be a closed point. The orbit Ox is a locally closed smooth subvariety and the orbit map is faithfully flat, hence surjective (Smooth orbits are locally closed and their orbit maps are faithfully flat over every field). The connected dimension supplier gives the following conclusions: every fibre of the orbit map over a closed point is a left translate of the stabilizer Gx and has dimension dim⁡Gx; dim⁡G=dim⁡Gx+dim⁡Ox; the orbit closure Ox‾ is the union of Ox and of orbits of strictly smaller dimension; and consequently every orbit of minimal dimension in X is closed and Ox‾ contains a closed orbit (Fibre dimension and orbit dimension add to the dimension of the group, Fibres of the orbit map and the scheme-theoretic stabilizer as a closed subgroup scheme).

[F3]

Dimension of classical varieties. For a classical variety, dim⁡ is the chain dimension, dim⁡xX is the maximum of the dimensions of the irreducible components through the closed point x, and pure dimension d means that every irreducible component has dimension d (Global and local dimension of classical varieties).

[F4]

Finite unions. If a Noetherian space T is a finite union of closed subsets T1,…,Tm, then dim⁡T=max⁡idim⁡Ti (Dimension of a finite closed union).

[F5]

Classical and scheme conventions. For a finite-type scheme over a perfect field, classical smoothness, scheme smoothness and regularity of all local rings agree (Classical and scheme smoothness over a perfect field); every complex affine algebraic group is smooth and has regular local rings (Complex affine algebraic groups are smooth).

[F6]

Dimension of a dense open and its boundary. A nonempty open subset of an irreducible classical variety has the same dimension as the variety, and every proper closed subvariety has strictly smaller dimension (Nonempty opens preserve irreducible dimension).

[F7]

Components at regular points. Every classical variety is Noetherian and has finitely many irreducible components (Classical varieties have finite irreducible decompositions). Under AC, a regular point of a reduced Noetherian scheme lies on exactly one irreducible component (A regular point lies on one irreducible component); apply this to the associated reduced finite-type complex scheme and read its components in the classical register through [F5].

Proof

technique · direct
1.1F1F4F5F7

For any complex affine algebraic group K, [F5] and [F7] imply that distinct irreducible components are disjoint. The finitely many components are therefore open and closed; since each is irreducible and hence connected, they are exactly the connected components. Let C be the component containing the identity. Translation by c∈C carries the unique component through the identity onto the unique component through c, so cC=C. Inversion and conjugation fix the identity and permute components, hence preserve C. Thus C=K∘ is a closed normal irreducible open subgroup, and translation by any k∈K identifies C with the component through k. Its finitely many cosets are precisely the components, all of the same dimension; [F4] gives dim⁡K=dim⁡K∘. Apply this also to the closed classical subgroup H=Gx: its identity component H∘, being connected and containing the identity, lies in G∘. Since H∩G∘ is open and closed in H, it is a nonempty union of components of H, each of dimension dim⁡H. Hence [F4] gives dim⁡(G∘)x=dim⁡(H∩G∘)=dim⁡H=dim⁡Gx.

2.1F1F2F5step 1.1

Suppose first that G is connected. Then Gx=(G∘)x is a closed subgroup by [F1], and [F2], read through [F5], makes Gx a locally closed subvariety. By step 1.1 the connected group G is irreducible, so its image under the surjective orbit map is irreducible. The connected dimension supplier in [F2] gives dim⁡Gx=dim⁡G−dim⁡Gx, hence dim⁡G=dim⁡Gx+dim⁡Gx.

3.1F2F6step 2.1

Still with G connected, put Z=Gx‾. By step 2.1, Gx is irreducible and locally closed, hence open dense in Z. Thus Z is irreducible and dim⁡Z=dim⁡Gx by [F6]. The orbit-closure clause of [F2] makes every orbit in Z∖Gx strictly smaller in dimension. This proves the connected case of (b).

4.1F1F2F3F4F6step 1.1step 2.1step 3.1

For arbitrary G, step 1.1 writes Gx as finitely many distinct pairwise disjoint G∘-orbits Oi=giG∘x, permuted transitively by G. That step also gives dim⁡(G∘)x=dim⁡Gx and dim⁡G=dim⁡G∘. Hence every Oi has dimension d=dim⁡G∘−dim⁡Gx=dim⁡G−dim⁡Gx by step 2.1 and translation. Each Oi is irreducible and locally closed, so it is open dense in its irreducible closure Zi, with dim⁡Zi=d by step 2.1. If i≠j and Oi∩Zj≠∅, the G∘-stability of Zj implies Oi⊆Zj and then Zi⊆Zj. Equal dimensions and [F6] force Zi=Zj, whose two nonempty open subsets Oi,Oj would intersect, a contradiction. Thus Oi∩Zj=∅ for i≠j. Consequently Z=Gx‾=⋃iZi has Z∖Gx=⋃i(Zi∖Oi) closed, and Oi=Zi∩Gx is closed in Gx. By [F4], dim⁡Gx=d; the irreducible components of Z are exactly the distinct Zi, each of dimension d. Every G∘-orbit in the boundary has dimension less than d by [F2]. For any full G-orbit there, apply the same finite-union construction to its finitely many connected-group orbits, which are translates of one another: its dimension is their common dimension, also less than d. This proves (a) and (b).

5.1F3step 4.1

If Gx has minimal dimension among the orbits in X, step 4.1 leaves no boundary orbit of smaller dimension, so Gx is closed. For an arbitrary orbit closure Gz‾, choose an orbit Gy in it with least dimension, which exists because the nonempty set of orbit dimensions is a subset of the nonnegative integers. This closure is closed and G-stable, so Gy‾⊆Gz‾. A boundary orbit of Gy would have smaller dimension by step 4.1 and still lie in Gz‾, contradicting the choice. Thus Gy is closed, proving (c).

6.1step 1.1step 4.1step 5.1∎

Steps 4.1 and 5.1 prove all the stated conclusions, with the inherited Axiom of Choice. The component argument was proved locally in step 1.1 using the stated regular-point and finite-component suppliers.

Remarks

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