In this section, we apply the results of Section 4 to
calculate the centers and traces (and their higher
-analogues) of symmetric monoidal -categories of
quasi-coherent sheaves. We also
calculate centers and traces of -categories of linear endofunctors
(equivalently by Corollary 4.10,
quasi-coherent sheaves on fiber products)
with monoidal structure given by composition (equivalently, convolution over the base).
5.1. Centers and traces
We begin with a discussion of the general notions of centers and traces
of associative algebra objects
in closed symmetric monoidal -categories. This is a general version
of the approach to topological Hochschild homology developed in [EKMM, Sh].
We then calculate the center and trace of the symmetric monoidal -category
of sheaves on a perfect stack (where we think of
as an associative algebra object in the closed symmetric monoidal -category
of presentable -categories).
Let be a symmetric monoidal presentable -category.
Recall that an associative
algebra structure on is an object is equivalent to the structure of algebra over the operad.
We briefly recall the -category versions of
two familiar facts from classical algebra.
First, there is the notion of the opposite associative algebra .
For this, recall that there is a map of operads determined by the action of the symmetric group on the two contractible subspaces of , and such that is equivalent to the identity. Given an -algebra ,
the pullback is by definition the opposite -algebra .
Second, given two associative algebras ,
their monoidal product
carries a natural
associative algebra structure.
For this, recall that given two algebras , over any topological operad , we have the structure of an -algebra on the monoidal product .
Since the term-wise diagonal map gives a map of operads ,
we obtain an -algebra structure on
by restriction along the diagonal.
Furthermore, any associative algebra is a left (as well as a right) module object over the associative algebra
via left and right multiplication.
Now assume further that is a closed symmetric monoidal -category.
Then we have internal hom objects
[L4, 2.7], and given -modules , we can define the -linear
morphism object .
Likewise, given left and right modules
we have a pairing defined by the two-sided
bar construction [L4, 4.5] over .
Definition 5.1.Let be an associative algebra object in a closed symmetric monoidal
-category .
(1)
The derived center or Hochschild cohomology
is the endomorphism object of as an -bimodule.
(2)
The derived trace or Hochschild homology is
the pairing object
of with itself as an -bimodule.
In general, the center is again
an associative algebra object in , and the trace is an -module object in .
Furthermore,
comes with a canonical central morphism
while comes with a canonical trace morphism
coequalizing left and right multiplication.
When is in fact symmetric, and are again naturally symmetric
algebra objects in , though the symmetric algebra structure on
is different from its general associative algebra structure.
5.1.1. Cyclic bar construction
It is very useful to have versions of the Hochschild chain and cochain
complexes which calculate the trace and center.
In the setting of an associative algebra object in a monoidal -category
, they will take the form of a simplicial object
and cosimplicial object such that the geometric realization
is the trace and the
totalization is the center .
(Note that simplicial and cosimplicial
objects here are taken in the -categorical sense, and so the diagram identities
hold up to coherent homotopies as in, e.g., [A], where the cyclic bar
construction for H-spaces is developed.)
We construct the simplicial object
and cosimplicial object
as follows.
Consider the adjunction
where is the induction, and is the forgetful functor.
It determines a comonad acting on .
As in classical algebra,
for any -module , the comonad provides a canonical augmented
simplicial object with terms
such that the geometric realization of is naturally equivalent to .
We will say that is a simplicial resolution of .
We can apply this technique to produce the familiar cyclic bar construction.
Consider the special case of the above adjunction
where again is the induction, and is the forgetful functor from -bimodules to right -modules.
Using the comonad ,
we obtain a simplicial resolution of the -bimodule
whose terms
are -bimodules which are free as left -modules.
Now recall that the trace is defined by the self-pairing
. Since the tensor product commutes with colimits, in particular geometric realizations, we calculate
Thus the geometric realization of
calculates the trace .
We write
for the simplicial object and refer to it as the Hochschild
chain complex.
Since is free as a right -module, the terms of the simplicial object
are free as -bimodules. Thus we can evaluate the terms of the Hochschild
chain complex
In particular, there are equivalences and , and the two simplicial maps are
the multiplication and the opposite multiplication of .
Similarly, recall
that the center is defined by the endomorphisms
. Since morphisms take colimits in the domain to limits,
in particular geometric realizations to totalizations, we calculate
Thus the totalization of
calculates the center .
We write
for the cosimplicial object
and refer to it as the Hochschild cochain complex.
As before, we can evaluate the terms of the
Hochschild
cochain complex
In particular, there are equivalences and , and the two cosimplicial maps are induced by
the left and right multiplication of .
5.1.2. Centers and traces for monoidal -categories
We will apply the above constructions in the following setting.
We will always take to be the -category
of presentable -categories (with morphisms left adjoints).
Then a monoidal presentable -category
is an associative algebra
object in .
Thus we have the notion of its
center (or Hochschild cohomology category) , and its trace (or
Hochschild homology category) .
Now we will specialize further to a geometric setting.
Let be a perfect stack, and take
to be the presentable stable -category
equipped
with its (symmetric) monoidal tensor product.
To calculate the center and trace of ,
we introduce the loop space
where the fiber product is along two copies of the diagonal
map.
Corollary 5.2.Let be a perfect stack,
and equip with its (symmetric) monoidal algebra structure given by tensor product.
Then there are canonical equivalences (of symmetric monoidal) -categories
Theorem 5.3.Suppose is
a map of perfect stacks satisfying descent.
Then there is a canonical equivalence
such that the forgetful functor is given by the correspondence
.
The proof occupies the remainder of this section. We break up the argument
into a general discussion and then its specific application.
At the end of the section, we also explain an analogous description of traces,
conditional on a still to be developed version of Grothendieck duality
in the derived setting. Namely, assuming further that
is proper with invertible dualizing sheaf and
Grothendieck duality holds,
we explain how to deduce an expected canonical equivalence
such that the trace
is given by the
correspondence .
5.2.1. Relative cyclic bar construction
For the proof of Theorem 5.3,
it will be useful to introduce relative versions of the Hochschild chain and cochain
complexes.
In general, the setup for the construction will be a map of
associative algebra objects in a monoidal -category
. The usual Hochschild chain and cochain
complexes introduced in the previous section will correspond
to the case when is the unit .
Consider the adjunction
where is the induction, and is the forgetful functor from -bimodules to
-modules.
Using the comonad ,
we obtain a simplicial resolution of the -bimodule
with terms
To reduce the notation, we will denote the above expression by .
As before,
the geometric realization of
calculates the trace ,
and
the totalization of
calculates the center .
We write
for the simplicial object and refer to it as the relative Hochschild
chain complex.
Similarly,
we write
for the cosimplicial object
and refer to it as the relative Hochschild cochain complex.
Continuing as before, we can evaluate the terms of the relative Hochschild
chain complex
Similarly,
we can evaluate the terms of the relative
Hochschild
cochain complex
Now we will apply the preceding formalism to calculate the center
of the monoidal -category . Recall that our aim is
to show that there is a canonical equivalence
where is the loop space of .
Consider the
symmetric monoidal -category , together with the monoidal
functor
obtained via pushforward
along the relative diagonal .
Set , and .
By the preceding discussion, the center
is the limit of the relative Hochschild cochain complex .
Furthermore, its terms can be calculated
Applying the results of Section 4, we can
rewrite each term in the form
Here we have used the elementary identification
where the left hand side has copies of , and the right
hand side has copies of .
We conclude that the terms of are nothing more than the
terms of the cosimplicial -category obtained by applying
to the C̆ech simplicial stack induced by the map
obtained by base change from the original map . It
is straightforward to check that under this identification the coboundary maps
are given by the usual C̆ech pullbacks. By assumption, satisfies descent,
hence satisfies descent, and thus the totalization
also calculates the -category .
Finally, note that under this identification,
the composition corresponds
to the composition
which is precisely the central functor .
This concludes the proof of Theorem 5.3.
5.2.3. Traces and Grothendieck duality
Finally, we explain here an analogous description of traces,
conditional on a still to be developed version of Grothendieck duality
in the derived setting. Namely, assuming further that
is proper with invertible dualizing sheaf and
Grothendieck duality holds,
we explain how to deduce an expected canonical equivalence
such that the trace
is given by the
correspondence .
We continue with the notation from the proof of Theorem 5.3
and the preceding sections.
We will show that the geometric realization
of the relative Hochschild chain complex also
calculates the -category .
As before, applying the results of Section 4, we can
rewrite the terms of in the form
Furthermore,
it is straightforward to check that under this identification the boundary maps
of
are given by the pushforwards which are right adjoints to the usual C̆ech pullbacks
.
To reduce notation, set with copies of .
Now suppose that is proper and
has an invertible dualizing complex (Gorenstein).
Then we expect Grothendieck duality to hold in the following form:
the pushforwards are also
left adjoints to the pullbacks
where denotes the relative dualizing sheaf of
.
Under this assumption, we find that the limit
of the
cosimplicial -category
admits the following alternative description.
First, we can identify the cosimplicial -category
with the
cosimplicial -category
via tensoring by the inverse of the relative dualizing sheaf on each simplex.
In particular, we obtain an identification of their limits.
Second, we can consider the cosimplicial -category
as a diagram
in the -category of presentable -categories (with morphisms right adjoints).
By [L2, Theorem 5.5.3.18],
the calculation of the limit of the diagram does not depend on this choice
of context.
Then we can pass to the opposite -category of presentable -categories (with morphisms left adjoints). To calculate a limit in
is the same as to calculate a colimit in .
But we have seen that the trace
is precisely the colimit of the dual simplicial diagram .
Thus we conclude that the geometric realization
also calculates the -category .
Finally, note that under this identification,
the composition corresponds
to the composition
which is precisely the trace .
5.3. Higher centers
Unlike in classical algebra, for an
algebra object in an -category, commutativity is an additional structure rather than a property.
More precisely, the forgetful functor from -algebras to -algebras is
conservative but not fully faithful.
Given an -algebra in a symmetric monoidal -category ,
the center that we have studied to this point does not involve the commutativity of .
More precisely, it only depends upon the -algebra underlying .
In this section, we discuss higher versions of the center where we
forget less commutativity. For a perfect stack , we calculate the
-center of the -category underlying the
-category . A detailed treatment of the foundations
of the subject may be found in Chapter 2 of [F1]. Here we
summarize only what is required for our consideration of the
-center of .
Remark 5.4. As noted in the introduction, after the completion of this manuscript,
the paper [L5] was revised to include a thorough treatment of
-categorical operads and their algebras, and the paper
[L7] treats in great detail the specific case of the
-operads. We refer the reader to these preprints for further
details.
Let be a topological operad. We define a topological category
with objects finite pointed sets and morphism spaces given by
We then obtain an -category, also denoted by ,
by applying the singular functor to the mapping spaces to get a simplicial category and then taking the simplicial nerve.
Definition 5.5([F1]).An -monoidal structure on an -category consists of a functor with an identification such that the natural maps
resulting from a choice of a point is an equivalence.
We will refer to the -category equipped with an
-monoidal structure as an -category. This construction will
be of particular interest to us when is the little -disks
operad .
To discuss Hochschild cohomology, we must next introduce the notion of operadic modules.
To this end, let be the category of finite based sets.
Let be the category of “doubly-based sets”
with objects finite based sets and ,
and morphisms of the underlying based sets such that
, and either or .
Given a topological operad , recall the -category introduced above.
We also define the -category to be the fiber product of -categories
Definition 5.6.Let be an -category. An --module structure on an -category is a functor extending the -monoidal structure on
, together with an identification such that the natural map is an equivalence for any .
Example 5.7. When is the operad, the notion of an --module coincides
with that of a -bimodule: it is an -category left and right tensored over . When is the operad, the notion coincides with that of a left (or equivalently right) module.
There is a similar definition of an -algebra and an --module in a symmetric monoidal or -monoidal -category generalizing the definition given above. This requires the notion of an -lax monoidal functor (see [F1, Chapter 2, Definition 3.10]). The simplification of the previous definition is available because is equipped with the Cartesian monoidal structure. We will avail ourselves of this greater generality in the following definition, although the only case that will concern us in the following is when is
either or .
Now let be a presentable symmetric monoidal
-category whose monoidal structure distributes over colimits.
Let be an -algebra in , and let be the -category of --modules in (see [F1, Chapter 2, Definition 4.3]). Under the above assumptions,
the -category is naturally tensored over .
Definition 5.8.For an -algebra in , we define the -Hochschild cohomology
to be the object of representing the endomorphisms of as an object of .
In particular, when ,
the -Hochschild cohomology of an -category is the -category of --module functors
We now specialize to the case where is the -operad. Intuitively, an -algebra structure on an object is equivalent to a family of associative algebra structures on
parameterized by such that antipodal points are associated to opposite multiplications on
. An --module structure on admits a similar intuitive interpretation
as a family of compatible left -module structures on
parameterized by . This intuition leads to the following (to appear in [F2], see also [L7]).
Proposition 5.9([F2]).Let be a presentable symmetric monoidal -category
whose monoidal structure distributes over colimits.
To an -algebra in there is functorially assigned associative algebra such that there is a canonical equivalence between --modules and left -modules.
If is the operad, and the -algebra structure on is obtained by restriction from an -algebra structure, then there is a canonical equivalence of
associative algebras .
For , the proposition
reduces to the familiar statement that for an -algebra ,
an -module structure (in the form of an --module structure)
is equivalent to an -module structure (in the form of a left -module structure).
For our current purposes, one can interpret the proposition as furnishing the definition of an
--module.
Namely, the reader uncomfortable with the abstractions can take
left -modules as the definition of --modules
Example 5.10. Let be an -algebra in
(so is a presentable monoidal -category whose monoidal structure distributes over colimits). Then left modules for the monoidal -category are equivalent to -bimodules.
In particular, we have an equivalence , where here denotes the -category equipped with the opposite monoidal structure. As a consequence, we see that in this case,
the preceding general definition of -Hochschild cohomology recaptures the notion of the Drinfeld center introduced earlier.
Let be an -algebra and be as above. We have a companion definition of -Hochschild homology.