Proof that is an Algebraic Stack
We prove that if is a smooth algebraic group acting on an algebraic space , then the quotient stack is an algebraic stack. This is one of the most fundamental and frequently-used results in the theory of algebraic stacks. The proof consists of two main parts: verifying that is a stack, that its diagonal is representable, and that it admits a smooth atlas.
Statement
Let be a scheme, a smooth algebraic group scheme over , and an algebraic space over with a -action . Then:
- is a stack over .
- The diagonal is representable by algebraic spaces.
- The natural morphism is a smooth surjection (and is a -torsor).
In particular, is an algebraic (Artin) stack over , with as a smooth atlas.
Part 1: is a stack
Recall that is the category fibered in groupoids over whose objects over a scheme are pairs where is a -torsor over and is -equivariant.
We verify the two stack axioms: descent for morphisms and descent for objects.
Axiom 1 (Descent for morphisms): Let and be two objects over . We need to show that the presheaf is a sheaf in the fppf topology on .
An isomorphism is a -equivariant isomorphism over with . Consider the algebraic space where is the sheaf of -equivariant isomorphisms from to (which is an algebraic space since -torsors are algebraic spaces and isomorphisms between them form algebraic spaces) and the fiber product imposes .
Since is represented by an algebraic space, its functor of points is an fppf sheaf. Hence is a sheaf.
Axiom 2 (Descent for objects): Let be an fppf cover and let be objects with descent data: isomorphisms satisfying the cocycle condition on triple overlaps .
Since -torsors satisfy fppf descent (a fundamental result in descent theory -- the stack is a stack for the fppf topology), the torsors with the descent data glue to a -torsor over .
The equivariant maps are compatible (since the respect the maps to ), so by descent for morphisms of algebraic spaces, they glue to a -equivariant map .
Thus is the descended object. This proves is a stack.
Part 2: Representability of the diagonal
We must show: for any scheme and any two objects , the sheaf is represented by an algebraic space over .
Step 2a: Reduce to trivial torsors. An isomorphism from to is a -equivariant isomorphism over with .
First, consider the sheaf of all -equivariant isomorphisms (without the condition on ). This is represented by the contracted product: where is with the opposite -action ( acts by ). Explicitly, this is where acts diagonally by .
Since and are -torsors (hence smooth over ), and acts freely on , the quotient is an algebraic space, smooth over (in fact, it is a -torsor twisted by the "difference" of and ).
Step 2b: Impose the compatibility with . The condition cuts out a closed subspace. More precisely, consider the two morphisms: The isomorphism sheaf is the fiber product:
Now, (equivariant maps from a torsor to correspond to sections of the associated -bundle). This is an algebraic space over . The map is a section of the structure map, hence a locally closed immersion.
Therefore, the fiber product is an algebraic space over (as a base change of algebraic spaces). In fact, if is separated, the map is a closed immersion, so is a closed subspace of .
Explicit description: Locally trivializing and , the isomorphism sheaf becomes: which is the "transporter" from to in . This is a closed subscheme of (the fiber product ), hence an algebraic space.
Part 3: The atlas is smooth and surjective
We prove that the natural morphism is representable, smooth, and surjective.
Definition of : The morphism sends a point (i.e., a -valued point of ) to the object of . That is, is the trivial -torsor with the equivariant map determined by the orbit of .
Representability of : We need to show that for any scheme and any object , the fiber product (via and the classifying map ) is an algebraic space.
The fiber product parametrizes pairs: a point and an isomorphism between and in . Such an isomorphism is a -equivariant isomorphism with .
This is equivalent to: a section (given by ), which is the same as a trivialization of over . The condition means .
So: (the total space of the -torsor ). Indeed, a point of over is a pair (base point in , point in the fiber of ), and the map to sends it to of that point.
is a -torsor: The above shows , which is a -torsor over by assumption. Since is smooth (as is smooth), the morphism is smooth.
is surjective: For any algebraically closed field and any object , the -torsor over is trivial (by Hilbert 90, since is algebraically closed and is smooth). A trivialization gives a point with . Hence is surjective on geometric points.
By the definition of surjective morphisms of stacks (surjective on geometric points), is surjective.
Conclusion: is a smooth, surjective, representable morphism from an algebraic space . This is a smooth atlas for , proving that is an algebraic (Artin) stack.
Verification of the groupoid structure
The smooth atlas gives rise to the groupoid: with:
- Source: .
- Target: .
- Composition: .
- Identity: .
- Inverse: .
This is the action groupoid of the -action on . Both and are smooth (since is smooth and is a morphism of algebraic spaces), confirming that is a smooth groupoid and in the groupoid notation.
Special cases and refinements
If acts freely on (i.e., the stabilizer is trivial for all geometric points ), then the diagonal of is a monomorphism (since is at most a singleton). This means is an algebraic space, not just a stack.
The proof: the transporter is either empty (if are in different orbits) or a single point (if they are in the same orbit, by freeness). So is represented by a monomorphism, and is a sheaf of sets.
When the action is free and proper, is a separated algebraic space, and in fact agrees with the geometric quotient .
If is a finite group scheme (e.g., a constant group ), then is etale (in characteristic zero or when is invertible), and the atlas is etale (since is etale implies -torsors are etale covers). Hence is a Deligne--Mumford stack.
The groupoid has etale source and target maps, confirming the etale groupoid structure.
For acting on by scaling, the atlas is smooth (but not etale, since has dimension 1). The stabilizer at the origin is (positive-dimensional), so is an Artin stack but not DM.
The groupoid is with and . Both source and target are smooth.
If the action map defined by is proper, then the diagonal of is proper (since the diagonal fibers are the stabilizers, which are the fibers of along the diagonal). In particular, is a separated algebraic stack.
For reductive acting on a proper variety : the action is always proper (since is affine and is proper), so is separated.
Let (the additive group) act on by . The orbits in are the horizontal lines , while consists of infinitely many fixed points (each is fixed). The action is not proper (the map is not proper along ).
The quotient stack is an algebraic (Artin) stack, but it is not separated: the stabilizer at points is (which is not proper).
The role of smoothness of
The proof crucially uses that is smooth over :
- -torsors are smooth: A -torsor is a smooth morphism (locally on , , and is smooth).
- The atlas is smooth: is smooth over since is a -torsor.
If is not smooth (e.g., in characteristic , which is not smooth), then -torsors are not smooth morphisms -- they are only finite flat. In this case, is flat and surjective but not smooth, and may fail to be an Artin stack (in the sense requiring a smooth atlas).
However, is still a stack, and for finite flat group schemes, it is an algebraic stack under a generalized definition (where the atlas is allowed to be fppf rather than smooth). The theory of algebraic stacks is sometimes extended to accommodate this.
Summary
The proof that is an algebraic stack consists of three independent parts:
- Stack axioms: Verified using descent for -torsors and equivariant morphisms.
- Representable diagonal: The isomorphism sheaf is an algebraic space, constructed as a fiber product involving the contracted product .
- Smooth atlas: The map is smooth and surjective because its base change along any test morphism is a -torsor (hence smooth).
The smoothness of is essential for the atlas to be smooth. The result applies to all smooth group actions and produces the most important class of algebraic stacks in practice.