We are now ready to start our geometric study of D-stacks. We will define in this Section a notion of (1)-geometric D-stack, analogous to the notion of algebraic stack (in the sense of Artin). We will also present the theory of tangent D-stacks, as well as its relations to the cotangent complex.
A 1-geometric D-stack is a quotient of a disjoint union of representable D-stacks by the action of a smooth affine groupoid. In order to define precisely this notion, we need some preliminaries.
). We say that f is a representable morphism,
if for any cdga A, and any morphism
SpecA-®F', the homotopy pull-back F ×F'h
SpecA
is a representable D-stack (see Definition 3.2).
SpecA-®F
from a representable D-stack is a representable morphism.
![-------------
A| B
| |
----- |
A Ä C[X1,...,Xn] B'](HagV346x.gif)
[X1,...,Xn]-®B' formally étale; here
[X1,...,Xn] is the usual polynomial ring,
viewed as a cdga concentrated in degree zero. This is an extension of one of the many equivalent
characterizations of smoothness for morphisms of schemes (see [Mil, Prop. 3.24 (b)]); we learn
it from [MCM] in which smooth morphisms (called there thh-smooth) between
-algebras are
defined.
SpecA-®F', the induced morphism

) is called a covering (or an epimorphism), if the
induced morphism p0(F)-®p0(F') is an epimorphism of sheaves.
Note that definition (4) above makes sense because of (1) and because the functor A
SpecA is fully
faithful on the homotopy categories.
Using these notions, we give the following
Remark 4.2 Objects satisfying Definition 4.1 are called strongly 1-geometric D-stacks as there exists a more general notion of strongly n-geometric D-stacks, obtained by induction as suggested in [S1]. The notion of strongly 1-geometric D-stacks will be enough for our purposes (except for our last example in section 5), and we will simply use the expression strongly geometric D-stacks.
The following proposition collects some of the basic properties of strongly geometric D-stacks.
In particular, Proposition 3.5 and point (3) above, tell us that the derived stack
BG of G-torsors is a
stongly geometric D-stack for any linear algebraic group G.
We are not going to present the theory in details in this work, but we would like to mention that standard notions in algebraic geometry (e.g. smooth or flat morphisms, sheaves, cohomology ...) can be extended to strongly geometric D stacks. We refer to [La-Mo] and [S1] for the main outline of the constructions. The reader will find all details in [HAG-II].
Let
a be the additive group scheme (over
) and consider the object i
a Î Ho(D - Aff
). It has a nice
model in D - Aff
which is Spec
[T] that we will denote by O (note that
[T] as a cdga in degree 0 is a
cofibrant object). The D-stack O is actually an object in commutative
-algebras, explicitly given
by
![Dop
O : CDGA -® (C - Alg)
A '® ([n] '® Gn(A)0),](HagV350x.gif)
Let us now fix a D-stack F, and consider the comma category D - Aff
/F of D-stacks over F; this
category is again a model category for the obvious model structure. We define the relative structural D-stack
by

-algebra object, we deduce immediately that OF is also a
-algebra object in the comma model
category D - Aff
/F.
Then we can consider the category OF -Mod, of objects in OF -modules in the category D -Aff
/F. If
one defines equivalences and fibrations through the forgetful functor D - Aff
/F-®D - Aff
,
the category OF - Mod becomes a model category. It has moreover a natural tensor product
structure ÄOF. The model category OF - Mod is called the model category of O-modules on
F.
Let A be a cdga and M be an (unbounded) A-dg module. We define a OSpecA-module
in the following
way.
Let G be a fibrant resolution functor on the model category CDGA. For any cdga B, and any integer n,
we define
(B)n as the set of pairs (u,m), where u is a morphism of cdga's A-®Gn(B) (i.e. u Î SpecA(B)),
and m is a degree 0 element in M ÄAGn(B) (i.e. m is a morphism of complexes of
-vector spaces
m :
-®M ÄAGn(B)). This gives a simplicial set [n]
(B)n, and therefore defines an object in
D - Aff

Clearly, the projection (u,m)
u in the notation above induces a morphism
-®SpecA. Finally, this
object is endowed in an obvious way with a structure of OSpecA-module.
This construction, M
induces a functor


Lemma 4.4 The functor 
defined above is fully faithful.
The construction M
described above also has a dual version, denoted by M
Spel(M) and defined
in a similar way.
Let A be a cdga and M be an (unbounded) dg-A-module. For a cdga B and an integer n, we
define Spel(M)(B)n to be the set of pairs (u,a), where u : A-®Gn(B) is a morphism of cdga,
and a : M-®Gn(B) is a morphism of dg-A-modules. This defines a D-stack B
Spel(M)(B)
which has a natural projection (u,a)
u, to the SpecA. Once again, Spel(M) comes equipped
with a natural structure of OSpecA-module. Also, this Spel construction can be derived, to get a
functor

Lemma 4.6 The functor
Spel defined above is fully faithful.
SpecA is called representable if it is equivalent to
some
Spel(M) as above.
SpecA-®F, the pull-back u*M is a representable
O-module on
SpecA.
One can prove that the homotopy category of perfect O-modules on
SpecA is naturally equivalent to
the full sub-category of Ho(A - Mod) consisting of strongly dualizable modules, or equivalently of
dg-A-modules which are retracts of finite cell modules (in the sense of [Kr-Ma, §III.1]). In particular, if A
is concentrated in degree 0, then the homotopy category of perfect O-modules on
SpecA is
naturally equivalent to the derived category of bounded complexes of finitely generated projective
A-modules.
This notion of perfect O-modules can be used in order to define the K-theory of D-stacks. For any D-stack F, one can consider the homotopy category of perfect O-modules on F, that we denote by DPerf(F). This is a triangulated category having a natural Waldhausen model WPerf(F), from which one can define the K-theory spectrum on the D-stack F, as K(F) := K(WPerf(F)). The tensor product of O-modules makes K(F) into an E¥-ring spectrum. Of course, when X is a scheme K(iX) is naturally equivalent to the K-theory spectrum of X as defined in [TT].
A related problem is that of defining reasonable Chow groups and Chow rings for strongly geometric D-stacks, receiving Chern classes from the K-theory defined above. We are not aware of any such constructions nor we have any suggestion on how to approach the question. It seems however that an intersection theory over D-stacks would be a very interesting tool, as it might for example give new interpretations (and probably extensions) of the notion of virtual fundamental class defined in [Be-Fa]. For this case, the idea would be that for any strongly geometric D-stack F, there exists a virtual fundamental class in the Chow group of its truncation h0F. The structural sheaf of F should give rise, in the usual way, to a fundamental class in its Chow group, such that integrating against it over the entire F is the same thing as integrating on its truncation h0F against the virtual fundamental class. However, even if there is not yet a theory of Chow groups for D-stacks, if one is satisfied with working with K-theory instead of Chow groups, the obvious class 1 =: [OF ] Î K0(F), will correspond exactly to the class of the expected virtual structure sheaf.
Let Spec
[e] the spectrum of the dual numbers, and let us consider iSpec
[e] Î Ho(D - Aff
).
Note that the zero section morphism Spec
-®Spec
[e] and the natural projection Spec
[e]-®Spec
induces natural morphisms

An important remark is that for any D-stack F, the truncation h0
TF is equivalent to the tangent stack
of h0F (in the sense of [La-Mo, §17]). In other words, one has

TF and iT(h0F) have the same classical points. However, it is not true in general
that iTF 
T(iF) for a stack F. Even for a scheme X, it is not true that
T(iX)
iTX, except when X is
smooth.
Definition 4.9 If x : iSpec
-®F is a point of a D-stack F, then the tangent D-stack of F at x is
the homotopy fiber of p :
TF-®F at the point x. It is denoted by

Let us now suppose that F is a strongly geometric D-stack. One can show that
TF is also strongly
geometric. In particular, for any point x in F(
) the D-stack
TFx is strongly geometric.
Actually much more is true. For any strongly geometric D-stack F, and any point x in F(
), the D-stack
TFx is a linear D-stack (over iSpec
) as defined in 4.7. Let us recall that this implies the existence
of a natural complex
WF,x1 of
-vector spaces (well defined up to a quasi-isomorphism and
concentrated in degree ] -¥,1]), with the property that, for any cdga A, there exists a natural
equivalence

HomC(
) denotes the mapping space in the model category of (unbounded) complexes of
-vector spaces.
Symbolically, one writes

WF,x1)* is the dual complex to
WF,x1. In other words, the tangent D-stack of F at x "is" the complex
(
WF,x1)*, which is now concentrated in degree [-1,¥[.
Definition 4.10 If x : iSpec
-®F is a point of a strongly geometric D-stack, then we say that the
dimension of F at x is defined if the complex
WF,x1 has bounded and finite dimensional cohomology.
If this is the case, the dimension of F at x is defined by

This linear description of
TFx has actually a global version. In fact, one can define a cotangent complex
WF 1 of a strongly geometric D-stack, which is in general an O-module on F in the sense of Definition 4.5,
which is most of the times quasi-coherent. One then shows that there exists an equivalence of D-stacks over
F

TF is a linear stack over F in the sense of Definition 4.7.
An already interesting application of this description, is to the case F = iX, for X a scheme or even an
algebraic stack. Indeed, the cotangent complex
WiX1 mentioned above is precisely the cotangent complex
X of [La-Mo, §17]. The equivalence

X and the geometric object
T(iX). In a sense, the usual
geometric intuition about the tangent space is recovered here, at the price of (and thanks to) enlarging the
category of objects under study: the cotangent complex of a scheme becomes the derived tangent space of the
scheme considered as a D-stack. We like to see this as a possible answer to the following remark of A.
Grothendieck ([Gr, p. 4]):
[...] Il est très probable que cette théorie pourra s'étendre de façon à donner une correspondance entre
complexes de chaines de longeur n, et certaines "n-catégories" cofibrées sur C; et il n'est pas exclus que par
cette voie on arrivera également à une "interprétation géométrique" du complexe cotangent relatif de
Quillen.
To finish this part, we investigate various non-equivalent natural notions of smoothness for geometric
D-stacks.
Strong smoothness. We have already defined the notion of a strongly smooth morphisms of cdga's in §4.1. We will therefore say that a morphism

SpecAi-®F as in Definition
4.1, such that all the induced morphisms of cdga's B-®Ai are strongly smooth morphisms of cdga's (see
§4.1). More generally, a morphism between strongly geometric D-stacks, F-®F', is called strongly smooth if
for any morphism
SpecB-®F' the morphism F ×F'h
SpecB-®
SpecB is strongly smooth in the sense
above.
Strong smoothness is not very interesting for D-stacks, as a strongly geometric D-stack F will be strongly
smooth if and only if it is of the form iF', for F' a smooth algebraic stack.
Standard smoothness. A more interesting notion is that of standard smooth morphisms, or simply smooth morphisms. On the level of cdga's they are defined as follows.
A morphism of cdga's A-®B is called standard smooth (or simply smooth), if there exists an étale covering B-®B', and a factorization

-vector spaces E. This notion, defined on cdga's, can be extended
(as we did above for strongly smooth morphisms) to morphisms between strongly geometric
D-stacks.
This notion is more interesting than strong smoothness, as a strongly geometric D-stack can be smooth without being an algebraic stack. However, one can check that if F is a smooth strongly geometric D-stack in this sense, then h0(F) is also a smooth algebraic stack. In particular, the derived version of the stack of vector bundles on a smooth projective surface, discussed in the Introduction (see also conjecture 5.4), will never be smooth in this sense as its truncation is the stack of vector bundles on the surface which is singular in general).
Nevertheless, smooth morphisms can be used in order to define the following more general notion of geometric D-stacks.
Essentially all we have said about strongly geometric D-stacks is also valid for geometric
D-stacks in the above sense. The typical example of a geometric D-stack which is not strongly
geometric is BG, where G is a representable group D-stack which is not a scheme. For example,
one can take G to be of the from
Spel(M) for a non-positively graded bounded complex of
finite dimensional vector spaces. Then, G is a representable D-stack (it is precisely
SpecL(M),
where L(M) is the free cdga on M), and BG is naturally equivalent to
Spel(M[-1]). When
M[-1] has non-zero H1 then BG is not representable anymore but is 1-geometric for the above
definition.
More generally, the definition above allows one to consider quotient D-stacks [X/G], where X is a
representable D-stack and G is a smooth representable group D-stack acting on X.
fp-smoothness. The third notion of smoothness is called fp-smoothness and is the weakest of the three and it seems this is the one which is closer to the smoothness notion referred to in the Derived Deformation Theory program in general. It is also well suited in order for the derived stack of vector bundles to be smooth.
Recall that a morphism of cdga's, A-®B is finitely presented if it is equivalent to a retract of a finite cell
A-algebra, or equivalently if the mapping space MapA/CDGA(B,-) commutes with filtered colimits (this is
the same as saying that
SpecA commutes with filtered colimits). We will then say that a morphism of
geometric D-stacks, F-®F' is locally finitely presented if for any morphism
SpecA-®F' there exists a
smooth atlas

Proposition 4.12 Le F be a geometric D-stack which is fp-smooth (i.e. F-®* = iSpec
is
fp-smooth). Then the cotangent complex
WF 1 is a perfect complex of O-modules on F.
In particular, for any point x Î F(
), the dimension of F at x is defined and locally constant for
the étale topology.
Of course, one has strongly smooth Þsmooth Þfp-smooth, but each of these implications is strict. For
example, a smooth scheme is strongly smooth. Let E be a complex in non-positive degrees which is
cohomologically bounded and of finite dimension. Then
Spel(E) is smooth but not strongly smooth as it is
not a scheme in general. Finally, any scheme which is a local complete interesection is fp-smooth, but not
smooth in general.
3 The expression smooth morphism will be used for a weaker notion in §4.4.