Deformations of objects in -categories
Abstract
In this paper, we prove that the deformation theory of an object in an -category is controlled by the its -fold endomorphism algebra. This recovers Lurie’s results on deforming objects and categories. We also generalize a previous result by Blanc et al. ([BKP18]) on deforming a category and an object simultaneously to the case of -categories.
1 Introduction
In algebraic geometry, there is a notion of deforming various objects over local Artinian algebras. For example, take a scheme and a quasicoherent module over it. A deformation of over the dual numbers is the data of a quasicoherent module over
whose pullback along the inclusion gives . If one requires to be locally free, then is characterized wholly by its gluing data, which in this case is captured in the first cohomology group of . Hence locally free deformations over of a locally free module is characterized by classes in .
Lurie generalizes these examples to the case of deforming an object in a category ([Lur11, Section 5.2], [Lur18, Section 16.5]). Using the framework of formal moduli problems, he shows that the -formal moduli problem associated to deforming an object can be characterized by its algebra of endomorphisms:
There’s also the classical notion of deforming a category and relating it to its Hochschild complex, as explained in [Kon95, Sei02, KL09], which is important for example in the study of Mirror symmetry and Fukaya categories.
Lurie reformulates this result in the context of infinity categories ([Lur11, Section 5.3], [Lur18, Section 16.6]):
where here denotes the derived center of , which can be calculated via the Hochschild complex of .
In this paper we follow Lurie’s arguments to generalize and unify his results of deforming an object in a category and deforming a category in . Namely, given any -linear -category and an object , we construct a functor and show that the algebra characterizing the formal moduli problem ([Lur18, Definition 12.1.3.1]) associated to is the -iterated endormorphism space of , or the center of . We recover Lurie’s results for object deformations by taking to be a -category, and we recover his results for category deformations by taking to be .
More precisely, let be a field, be the -category of presentable -linear categories and -linear colimit preserving functors. It has a monoidal structure given by the -linear tensor of categories. In other words, , the category of presentable categories with action. Then inductively, we define as the -category of presentable linear categories tensored over (see 1.2.1), the objects of which we call ”-linear -categories”. In a similar vein, one can define for an -algebra .
We define a version of object deformations for a -linear -category. That is, given an -category and an object , we define a functor
from small -algebras to large spaces. The functor is intuitively given by the formula
This functor will have an associated formal moduli problem which is characterized by an augmented -algebra: the -fold endomorphism algebra of (thought of as a nonunital algebra). More precisely, we have the following definition:
1.0.1 Definition (-fold Endomorphism object).
Given . Let . This has a clear basepoint Inductively we can define
where (or sometimes ) is the identity of , with a new basepoint given by the identity . When the context is clear, we may drop the and from .
We may also use to denote where the basepoint is , which is an alternate base case for this induction. Here denotes the internal hom, see (1.3.1).
Our first main result is:
1.0.2 Theorem.
The formal moduli problem associated to is equivalent to
where is the -Koszul duality functor ([Lur17, Section 5.2.5]).
This directly generalizes previous results: using we get exactly the classical result for deforming objects in categories [Lur11, Section 5.2], [Lur18, Section 16.5]. Using and and letting be a given category in , we get Lurie’s result for deforming categories [Lur11, Section 5.3], [Lur18, Section 16.6]. The proof is given in 2.4.1.
We next consider the problem of deforming an object and -category simultaneously. We follow Blanc, Katzarkov, and Pandit ([BKP18, Section 4]) and Lurie ([Lur18, Remark 16.0.0.3]), who previously considered the case of .
More precisely, let for the category of presentable pointed -linear -categories:
Given an -category and an object , we can define a simultaneous deformation functor as follows: given a small -algebra , we let
where the map
is using the augmentation , and for consistency with the our other section, we let
be the category of left -modules in (as opposed to [BKP18] which uses right modules). We show that the formal completion of this functor is characterized by the nonunital -algebra
(1.0.3) |
where is the center of , is the center of , and the fiber is taken at . Explicitly, we can let , and the map between them is given by evaluation at .
Our second main result is:
1.0.4 Theorem.
There is an equivalence of formal moduli problems:
The proof is given in (3.4.1). For example, using , the center of is represented by —in other words natural transformations from to itself—and the center of is represented by . The map is given by evaluation of the natural transformation at . This recovers Proposition 4.7 of [BKP18].
These deformation problems are related to the deformation problem of an -monoidal category: Given an -monoidal category , its deformations can be identified with deformations of the pointed category . These ideas are discussed in section 3.5. This uses the fully faithful embedding of -monoidal categories into -pointed categories (categories with an object together) via the rule
Hence one can study the deformation theory of by studying the deformations of the pair . This also recovers the deformations of algebras (which can be thought of as single-object -categories -cells are trivial for ). Toën, in theorem 5.1 and 5.2 of [Toë14], also relates deformations of -monoidal categories to -Hochschild cochains as defined in [Fra13].
The deformation theory of -monoidal categories is incredibly important for various theories of quantization. In section 2 of [Toë14], Toën explains the connection between different variations of quantization—namely quantum groups, skein algebras, and Donaldson-Thomas invariants—to deformations of (monoidal) categories. For example, Toën relates quantum groups (see [Dri87]) to deforming the category of sheaves of the moduli space of -bundles on the point.
1.1 Acknowledgements
I’d like to thank my advisor, David Nadler, from whose guidance I have benefited enormously. In addition, I’d like to thank Germán Stefanich for many insightful conversations and ideas. Lastly, this work was partially supported by NSF RTG grant DMS-1646385
1.2 Set theoretic issues
For this section, let’s hypothesize for now an increasing sequence of universes We let ”small” mean -small and ”large” mean -small. We will only need two universes and .
To solve the set theoretic issues of even defining (and by analogy), we follow [Ste21]. There are two solutions.
First we can define as the category of -linear categories with cocontinuous -linear functors between them. Then to be the -small category of all -linear -small categories with -linear cocontinuous functors. We can continue the induction, producing larger and larger categories which is -small. Notice there is no presentability here.
The other idea is to only use two universes, one small and one large . Then one can define inductively, following chapter 12 of [Ste21].
1.2.1 Definition (Presentable -linear -categories).
Let’s define and inductively: For , we define
Next we inductively define:
In other words, is the category of -modules in the large category of cocomplete categories and cocontinuous functors. Finally we can define to be the full subcategory of -compact objects of . We will also denote this category by , see (2.1.5).
1.2.2 Remark.
Notice that agrees with the usual definition of as the category of presentable -linear categories with cocontinuous -linear functors between them.
1.2.3 Remark.
We will make use of mainly because like in [Ste21, Remark 8.4.3], we don’t know if the hom objects for are presentable. They may only exist in . However it is true that for any category , its hom objects are in .
Despite which approach we take, our fmp is perhaps large in general, in contrast to [Lur18, Section 16.5, 16.6]. The point is that our -categories as defined could have large -fold endomorphism objects, unlike the category deformation and object deformation problems that Lurie considered. The author doesn’t know whether these presentable -categories have presentable hom objects or not.
However, if our given -category had small -fold endomorphism objects, then we have the following easily using our main result 1.0.2:
1.2.4 Proposition.
Given an -category (or ) with small -fold endomorphism objects. Then the formal moduli problem associated to is a functor that lands in , the category of -small spaces.
In this paper, we will by default use the second method of restricting to presentable categories for concreteness, but the arguments don’t really differ regardless of which method one chooses.
1.3 Conventions
Our notational conventions are listed here. First, unless otherwise mentioned, we are working over a field and all mentions of -linear objects are infinity categorical. For example, ”finite dimensional vector space” will mean a compact object in the infinity category of -modules.
We will also occasionally use the abbrevation ”fmp” for ”formal moduli problem”.
By default, categories of algebras will be large due to being large. Notice that is still a small category due to the finiteness conditions placed on small algebras!
1.3.1 Notation
Here is some basic notation and conventions. We will have more notation later which will be introduced as needed.
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•
describe categories in (1.2.1). We also just call these -categories for short.
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Similarly pairs denote objects in .
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denotes the category of small spaces. denotes the category of -small spaces, or ”large” spaces.
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•
is the space of maps between and .
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denotes the hom object in , as given by the right adjoint to the tensor action on .
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denotes the center of which can be calculated via .
-
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denotes the center of which can be calculated via
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•
denotes the large category of -algebras (or more precisely, -fold iterated algebras), following [Lur17]. denotes the large category of -algebras over .
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–
denotes the (large) category of augmented algebras over .
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–
denotes the category of artinian/small augmented -algebras. Notice that this is always a small category due to the definition of small algebras.
-
–
- •
- •
-
•
denotes for and .
-
•
denotes .
-
•
denotes .
- •
2 Deformations of objects
Throughout this section, we assume we’re given and an object . We’d like to show that the deformations of in the -category is characterized by the -algebra . The argument follows four steps, generally following Lurie’s ideas in [Lur11, Section 5.2, 5.3] or [Lur18, Section 16.5, 16.6]:
-
1.
Construct the functor characterizing deformations of .
-
2.
Prove is -proximate.
-
3.
Construct the comparison map
-
4.
Prove that is an equivalence.
2.1 Constructing the functor
First let’s define how to take -fold modules for an algebra. We have functors
via . We also get induced functors by applying to get
Composing these functors, we can define:
2.1.1 Definition (Iterated left modules).
Let denote the composite functor given by
(2.1.2) |
We denote the evaluation of this functor on by . We will also use the variant functor
(2.1.3) |
which ends one step early as compared to above.
2.1.4 Remark.
Clearly there are variants where one can take iterated right modules, or even switch between taking left and right modules. Notice that if is an -algebra, then these constructions are all equivalent, and we may denote the category by .
2.1.5 Remark.
For , notice that we get for . We can show this by induction: For , clearly . Next, if the result holds true for , then we notice that
since every object of is already an -module, by definition (1.2.1). Since is an -algebra, we may also denote by .
Recall that we define (1.3.1), hence we have a cocartesian fibration
We pull back along to get the left modules whose action is given by an -algebra.
2.1.6 Definition (Left Modules).
Let to be the following pullback:
Here the left vertical map is the cocartesian fibration and the lower horizontal map is the -fold functor.
We can also further pull back along to get
Intuitively, objects of consists of triples where , (or ), and is a left action of on .
2.1.7 Remark.
Dually, we can use right modules instead by replacing the right vertical leg by
where we’re using the fact that since is symmetric monoidal, so we can choose to either use left or right modules to define .
In other words, we can pull back along the cocartesian fibration
So we can analoguously define and . This has objects where , (or ), and is a right action of on .
Now we’re finally ready to construct our functor. To do this, we construct first the associated fibration, then use straightening/unstraightening to get the functor we need. Recall we have a cocartesian fibration . Let be the subcategory whose morphisms are the cocartesian arrows of this map. Then
(2.1.8) |
is a left fibration. Our given object has a natural action. This gives us an object .
2.1.9 Definition (Deformation fibration).
Let be the slice of over the object . In other words:
We have an induced left fibration by taking slices of 2.1.8:
2.1.10 Construction ().
classifies a functor . Here is the category of not-necessarily -small spaces. Finally, by restricting to small algebras, we get the functor we wanted:
2.1.11 Remark.
Notice that given an algebra , , where the map is given by the augmentation map . Here (2.1.5), so since is -linear , every object is a -module.
2.2 Proving is -proximate
Let’s begin with a generalization of fully faithfulness. Here we let for brevity. For the following definiton and proposition, we’ll need to use non-presentable -categories (in other words, we consider categories in ) because we’ll induct by taking repeated hom spaces (1.2.3).
2.2.1 Definition (-fully faithful).
Given a functor of -categories. Then we say
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•
is -fully faithful if is an equivalence.
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•
is -fully faithful if for all . the induced functor is -fully faithful.
This is an inductive definition for . Notice that the case agrees with our usual notion of fully faithfulness.
Now we prove that is an -proximate fmp. We recall the following result:
2.2.2 Proposition ([Lur18] Prop 16.2.1.1).
Let be an -ring and a -linear category. Suppose we’re given a pullback:
in . Then the induced functor is fully faithful.
2.2.3 Remark.
Using the hypotheses of the above proposition (2.2.2), let , and let for any -algebra . Then, as explained in the proof of [Lur18, Prop 16.2.1.1], the conclusion of the above proposition (2.2.2) is equivalent to the unit map
being an equivalence for any . This is an easy application of the result that left adjoints are fully faithful if and only if the unit map is an equivalence.
Using this result, we’ll prove the following result by induction:
2.2.4 Proposition.
Given a pullback in ,
and . Given , write for
Then the comparison map
is representably -fully faithful.
Here ”representably” -fully faithful means after taking homs out from any object , the result is a -fully faithful functor.
Proof.
The case is explained in remark (2.2.3). This is the base for our induction.
For the inductive step, we prove it for , assuming it’s done for . Then given our pullback square along with , we are trying to show that
is representably -fully faithful. This means that given any , we must show
is -fully faithful. Let denote as with , and let denote . Then by the extension of scalars adjunction, we see that
so our above map is equivalent to
To show this map is -fully faithful, we take any two objects and we try to show the induced map
is -fully faithful (using the inductive definition of -fully faithfulness).
This last map, once again by the extension of scalars adjunction, can be identified with
But since by induction, we assume is representably -fully faithful in ! This implies that the comparison morphism—the image under of —is indeed -fully faithful, as desired. ∎
Using this we prove
2.2.5 Proposition.
is an -proximate fmp.
Proof.
We seek to prove that given a pullback:
in , the comparison is -truncated.
Using our above result, we know that the comparison map
is representably -fully faithful.
Thus, by extension of scalars, we have that given any (borrowing notation from the last proof), we have
is -fully faithful. Plugging in , we get that
is -fully faithful. However, notice that using the basepoint for , we see that can be identified with the fiber of . Hence, the above -fully faithful map descends through fibers and taking cores, and we get that
is -faithful. It’s easy to show that this is equivalent to the map being -truncated as we actually have a map of spaces. For example, when , we know -fully faithful maps between spaces are equivalent to -truncated inclusions.
Hence, removing the loop spaces, we see that the map
must be -truncated, as desired. ∎
2.3 Constructing the comparison map
We construct the map
2.3.1 Construction (Duality functor ).
Let be the pairing of categories inducing -Koszul duality ([Lur17, Construction 5.2.5.32]). Objects of intuitively consist of two algebras along with an augmentation of their tensor product: .
Let be an -pairing between (so it’s an object of ). Suppose we’re given the data where and is an equivalence, so this data can be thought of as an object in . Notice that
Thus we have
where the equivalence uses the given pairing and . This construction gives a right action on . This construction produces a functor:
This is a left representable pairing of categories, which induces a duality functor (by [Lur11, Construction 3.1.3])
as required.
Now, we can easily get our compairson .
2.3.2 Construction (Comparison map ).
We have a square:
Here the top horizontal functor is the duality functor defined just above, the bottom functor is -Koszul duality functor. The left and right vertical maps are canonical Cartesian fibrations.
We restrict to small algebras:
Note that the bottom morphism is an equivalence. This morphism of the vertical left fibrations gives us a comparison morphism of the two induced functors
(2.3.3) |
as desired.
2.4 Proving induces an equivalence
We would like to show:
2.4.1 Theorem.
Given any -category with an object , the map (2.3.3) induces an equivalence
To do this, we first use Lurie’s Proposition 1.2.10 in [Lur11] to reduce to the cases where the input algebra is for , as values on these algebras determine the tangent complex in our current deformation context.
Then we have a square:
Since is an -proximate fmp, we can reduce our task to showing that the bottom map is an equivalence.
So we’ve reduced our problem to proving the following:
2.4.2 Proposition.
Let be an -category with an object. Then the bottom leg of the square
is an equivalence for all .
We start with some preliminary lemmas. First we need a lemma about functors out of , a Morita style result. This is just an -categorical version of [Lur17, Theorem 4.8.4.1], and indeed it follows from that result.
2.4.3 Theorem.
Let be an -algebra where and be an -category. Then the composition
is an equivalence. The second map uses the functoriality of , and the third map is evaluation at the bimodule .
2.4.4 Remark.
Of course by reversing left and right, there is an analoguous dual version of 2.4.3. Note the difference between and is that while they are both -linear, functors in the former also have to preserve colimits.
Proof.
We just use [Lur17, Theorem 4.8.4.1] directly to prove this one. Let contain all small simplices. If is an -algebra, then is an -algebra in . is also right tensored over (as left and right modules over are equivalent). So we directly apply the dual of [Lur17, Theorem 4.8.4.1] using the category , the right module , and the algebra . This gives us exactly what we needed. ∎
The considerations in [Lur17, Section 4.8], show that the categorical dual of is . If we apply this here where , we see that the reason that
shows up is because it’s the categorical dual of . This motivates the following notation:
2.4.5 Notation (Duality).
Let
denote the categorical dual of in . So in the case that , we get
In the case that , we would get the -linear dual of , if it exists.
Now we can do some simple calculations of endormophism spaces. First one about endormorphisms of the unit object in . For the next few results, recall that we have the convention that and .
2.4.6 Corollary.
Let be an -algebra, where . Then:
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1.
The evaluation map
is an equivalence sending the identity to .
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2.
The composite map of evaluations
is an equivalence that sends the identity to .
2.4.7 Remark.
Notice for the case that , this corollary gives the simple result that
is an equivalence.
Proof.
The domain of is
by definition. We use the free-forgetful adjunction between and , which gives us
Then the Morita result 2.4.3 then let’s us simplify the second mapping space via evaluation to
But this can clearly be identified with when precomposing with the free-forgetful adjunction, thus we’re done.
For the second statement, it follows from a simple induction and reduction of various endomorphism spaces using the first result. ∎
We can secondly calculate a result about endormophisms of the augmentation module in .
2.4.8 Corollary.
Let be an augmented -algebra where . Then:
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1.
The evaluation map
is an equivalence which sends the identity map to the augmentation module .
-
2.
The composite map of evaluations
is an equivalence which sends the -fold identity to the augmentation module when .
2.4.9 Remark.
As a special case, when we get
is an equivalence.
Proof.
Let’s use the extension of scalars along the augmentation map to identify
Now if , we see the last mapping space simplifies directly to . Otherwise if , we use the Morita result 2.4.3 to get
as required! Tracing the identifications, we see it indeed corresponds with , which by definition sends the identity map to the augmentation module.
For the induction we just iteratively use the first result. Notice that even if we replace with it’s dual , the identification above
can basically go unchanged, which is why the induction works past the second step (which requires calculating endomorphisms of the augmentation module in the category when ).
Lastly when , the final dual that we take is not a categorical dual but just a -linear dual, thus giving us at the end. ∎
2.4.10 Remark.
Note that given , ie an -fold augmented algebra, we can take it’s opposite in -different ways given its -commuting multiplications. If we choose the very first multiplication to take , then we get . However, regardless of which factor we take on, we get (not canonically) equivalent algebras because any of these -funtors correspond to choosing an element on the determinant connected component of , which naturally acts on . Such an identification relies on a path between these two elements of .
We could also take the Bar construction on various multiplication levels of . Notice that if we choose to take and on the first level (as we do in the above argument), we get that , where we need to take the opposite of the second multiplication of . This is because in , after taking Bar on the first multiplication, it is removed (or turned into a comultliplication), hence taking op afterwards affects the second multiplication of our original algebra .
By using the standard calculation
on -algebras, we can see that
which finally let’s us identify with . So as long as in the argument above, we didn’t really need the categorical duals in the endomorphism space formula in the above lemma. Using this result would have made the induction after the second step a little more symmetric-looking, however this identification relies on a choice of a path in between the two different opposites that we take and isn’t canonical.
Next we need some results on endomorphism spaces and tensor products. These results could have been proven directly without the above corollaries, but we separated out the arguments for clarity.
2.4.11 Lemma (Endomorphisms and tensors 1).
Let be a small -algebra, and be an -category with an object. Let denote and denote . Then the canonical tensoring map
is an equivalence for . In this equivalence goes to .
Proof.
We prove it by induction. For , the result is obvious: the map defaults to the comparison map
which is an equivalence that also sends to , as required.
Next let’s assume it’s true for , where and we’ll prove that it’s true for . We can simplify our codomain through a series of steps. First, by definition we have
Our inductive hypothesis says is an equivalence. Using the functoriality of , combined with 2.4.6, gives us an equivalence between and
Next, using the free-forgetful adjunction, we can simplify the above mapping space to
Now we know that is dualizable for using results on in [Lur17, Remark 4.8.4.8]. For , the simplifies to just . Since is small, it is dualizable as a -module!
Thus for all , we know that is dualizable, so we can pull it out of the mapping space:
which again using 2.4.6 we can identify with
We can trace this comparison map backwards and we’ll see it clearly sends a pair of maps to their external tensor. In other words it induces the map . Thus we’re done, we’ve show is equivalent to a composition of equivalences. ∎
The second endomorphism result is about the augmentation module instead of the ring itself.
2.4.12 Lemma (Endomorphisms and tensors 2).
Let be a free -algebra on a finite-dimensional vector space, and be an -category with an object. Let denote and denote . Here denotes the augmentation module. Then the canonical tensoring map
is an equivalence for . In this equivalence goes to .
Proof.
We follow the last proof and start by induction. For , the result is by definition:
is clearly an equivalence sending to .
Next let’s assume it’s true for . Let’s simplify our codomain through a series of steps. We have
Our inductive hypothesis says is an equivalence, thus it’s also an equivalence on mapping spaces. This result combined with our calculation 2.4.8 gives
Now we use the extension of scalars along to simplify the right mapping space to get
which simplifies to
Since is dualizable (for we’re using is free on a finite-dimensional vector space, thus is dualizable [Lur17, Proposition 5.2.3.15]), we can pull it out of the mapping space:
But using our calculation 2.4.8, we can clearly identify this with our domain
If you trace this calculation, you can see that this chain of equivalences is equivalent to the tensoring map . ∎
Now we’re ready to prove the proposition.
Proof of 2.4.2.
We’d like to show the bottom leg of
is an equivalence.
First let (which is a small algebra), so our bottom leg is now
(2.4.13) |
First we identify with the following map
by using two observations:
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For the domain, . In the pullback, the map is given by the augmentation map.
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For the codomain, . In the pullback, the map is given by the forgetful functor.
as well as just unpacking the definition of (2.3.3). Notice here we are suppressing the in the tensor product , using the fact that
is monoidal and fully faithful, and thinking of the Koszul duality pairing as giving the algebra two commuting central actions by and [Lur17, Proposition 5.2.5.33, Lemma 5.2.5.36]. After taking we get exactly the correct tensoring that defines .
We have a triangle
which gives after taking fibers at —for the domain along the forgetful functor to , for the codomain along the extension of scalars of the augmentation map to . This triangle commutes because if you take left adjoints everywhere, you get the classical calculation that the Koszul dual of a square-zero algebra is a free algebra [Lur11, Proposition 4.5.6]
Now the horizontal map in the triangle can be identified with
For notational convenience, given any augmented algebra , let and , and . For the last definition, is the augmentation module, induced by the augmentation map .
We want to analyze (2.4.13). Our domain can be identified with the fiber of
and the codomain can be identified with
The asymmetry here is because in the domain, the basepoint is while in the codomain, the basepoint is .
Our map is induced by the -functoriality of . Indeed on -cells, induces a functoriality map
As this map is induced by the tensor product , we have a natural square
The left and right legs come from the from the identification and . Notice is induced by the functoriality of the map
(2.4.14) |
on the left factor and identity on the right factor (since it’s functoriality of the identity on the right factor).
We would like to show that are all equivalences, which would then show is an equivalence. This would let us conclude is an equivalence by taking fibers.
First, showing and are equivalences is just our calculation of endomorphism spaces in 2.4.11, and 2.4.12.
Next we try to show is an equivalence. Since the right hand factor of is identity, we only have to focus on the left hand factor of :
which is induced by the functoriality of
on -cells. By Morita equivalence 2.4.3, any -linear colimit preserving functor
corresponds uniquely to a bimodule structure on (we are again suppressing notation: in reality we have ).
The forward direction of this equivalence takes the functor and evaluates it on , which gives with its action. The action comes from looking at -fold endomorphism spaces, ie exactly the functoriality map on -cells:
This clearly gives a bimodule .
Applying this to our functor , we note that clearly corresponds to the bimodule given by Koszul duality, . Also notice that
This map can be identified with a map
(2.4.15) |
using our calculations in 2.4.6 and 2.4.9. This map MUST be the adjunct to the Koszul duality pairing
since it must give the Koszul duality structure by what we said above. In other words, 2.4.15 is the unit of the self-adjuntion of . Since is small, this unit is an equivalence (just combine [Lur11, Theorem 4.5.5] with [Lur11, Proposition 1.3.5]). Thus , and thus , is an equivalence, as needed.
We’ve finally proved that is an equivalence. Finally we can conclude that is an equivalence because is induced by taking fibers of the vertical maps in the square
∎
2.4.16 Remark.
Note that since we can identify and , our last square can be simplified to be
which after taking fibers (which gives , just says that .
2.4.17 Remark.
We can alternatively follow [Lur11, Proposition 5.3.19], to prove this last step instead. We’ll use the fiber sequence instead of the more restricted , to get the following:
We can identify the domain of with
and the codomain with
Using the functoriality of in —the input for —and the Yoneda lemma, it follows that is induced by a map
This is equivalent to having a map after passing to Koszul duals (for small algebras ) which gives
If one can show that this map is an inverse to the natural comparison map
then we’d be done. Here we’re using the fact that is actually square zero, so is an equivalence.
2.5 Examples
Here we list several example deformation problems that our theorem 2.4.1 characterizes.
2.5.1 Example (Object in a 1-category).
Taking a -category and an object , we see that we recover Lurie’s result about deforming an object in a category ([Lur11, Section 5.2], [Lur18, Section 16.5]).
Thus our theorem 2.4.1 recovers many classical results, like deforming a quasicoherent module on a scheme over the dual numbers . We can use , and we see that deformations of over are given by maps
where is the free associative algebra generated in cohomological degree . Taking of the hom space
thus gives the first cohomology , recovering the classical result.
3 Simultaneous deformations
Throughout this section, we assume we’re given and an object . We now shift our study to the situation of deforming an object and a category together, considered as an object of . We aim to show such deformations are characterized by the -algebra , which can be described as the fiber of (see 1.0.3).
The argument again follows four steps, following ideas in [Lur11, Section 5.2, 5.3] and [BKP18, Section 4.1]:
-
1.
Construct the functor .
-
2.
Prove is -proximate.
-
3.
Construct the comparison map
-
4.
Prove that is an equivalence.
This idea is very similar to the case of deforming an object in an -category and we hope to unify these two approaches in the future.
3.1 Constructing the functor
3.1.1 Definition (Left Module categories).
Let be the pullback
and let be the pullback
where the left leg is given by the usual cocartesian fibration [Lur17, Definition 4.2.1.13]. There’s a obvious projection that forgets the basepoint.
3.1.2 Remark.
Intuitively, objects of consists of -tuples where , , and is a left action of on .
3.1.3 Remark.
Dually, we can use right modules instead by replacing the right vertical leg by
So we can analoguously define . This has objects where , , and is a right action of on .
Similarly we can analogously define .
First, just like with ObjDef (2.1.9), we first define the associated left fibration to SimDef.
3.1.4 Definition (Simultaneous deformation fibration).
Now we’re ready to construct .
3.1.7 Construction ().
We look at our given pair , with natural action, which we’ll denote as , the action being implicit.
By straightening, the left fibration (3.1.6)
classifies a functor . Here is the category of not-necessarily -small spaces. Finally, by restricting to small algebras, we get the functor we wanted:
3.1.8 Remark.
Notice that given an algebra ,
as mentioned in the introduction.
3.2 Proving is -proximate
To prove this statement, we show the existence of a fiber sequence of deformation functors, generalizing Proposition 4.3 of [BKP18].
We begin with constructing the maps.
3.2.1 Construction (Comparison with ObjDef).
We construct the projection
which intuitively just forgets the ”point” and its deformation, ie it sends a simultaneous deformation and forgets the -deformation .
More precisely, first we use the projection
which commutes to the projections to , which induces a projection of slices
over . This induces a projection
(3.2.2) |
of functors
3.2.3 Remark.
The codomain of this projection, in the case that , is usually called .
Next we analyze the fiber of this projection.
3.2.4 Construction.
The fiber of the projection
at the category is equivalent to the Kan complex . The fiber map sends to . This induces a functor
commuting with the projections to . This induces a natural transformation
(3.2.5) |
By our construction, it’s directly obvious that we have a fiber sequence:
3.2.6 Proposition.
Now we show some consequences of having this fiber sequences. First, it proves what we wanted to show:
3.2.7 Proposition.
is an -proximate fmp.
Proof.
Since is -proximate and is -proximate (2.2), we see that since taking loop spaces and pullbacks preserve limits, that must also be -proximate. ∎
Since the completion functor from -proximate fmps to fmps is limit-preserving, we can also easily see
3.2.8 Proposition.
The fiber sequence we constructed descends to fmp completions, and we have a natural comparison of fiber sequences:
where the vertical maps are the units for the fmp-completion functor.
3.3 Constructing the comparison map
For this section, we’ll use the following notation:
3.3.1 Notation.
Given an -category with a left action by an -algebra (in other words, a left action by and a right action by an -algebra , we emphasize this structure as so:
Let be the pairing of categories inducing -Koszul duality ([Lur17, Construction 5.2.5.32]). Objects of intuitively consist of two algebras along with an augmentation of their tensor product: . This gives the structure of a module.
Let be an -pairing between (so it’s an object of ). Suppose we’re given a simultaneous deformation (where the actions and augmentation equivalences are suppressed). Notice that
Here we let stand in for the pointed category .
Thus we have
where the equivalence uses the given pairing and the augmentation equivalences. This construction gives a right action on . Notice we gave a right module structure using the augmentation.
In fact we have just a little more, we know that the action of on is ”trivial”: can be written as a map
The shorthand subscripts on the left denote left actions of and analogously, the right subscripts show right actions.
Then the above process can be seen as tensoring on the left by , this time seen as having a left and right action (which is equivalent to the right action of . All this distinction of -algebras only matters for the very trivial case ). Thus we get
where our tensors are over . This reduces to
which shows the right -action (or left -action). Notice that the action of on is ”trivial” since it is no longer coupled with the action of ! Hence it’s image, which points out , also has trivial action in this way.
This construction produces a functor:
(3.3.2) |
where is the category of pointed -categories with right actions by augmented algebras which are trivial on the given point. Each object is an object of with extra triviality data. In other words, with -action (where is augmented) is trivial when the map
picking out factors through the right -module map
where the action of on is given by the augmentation map. The explicit definition is given as follows:
3.3.3 Construction ().
We have a functor
sending an augmented algebra to the category with right augmentation -action . Let
be the natural projection. Finally, we have two maps from . First we have
taking to the augmentation functor , equipped with natural right -action and right augmentation -action respectively. Secondly we have
sending to the degenerate triangle
Finally we can define: Let be the pullback:
Of course, we can analogously define the version with left actions instead.
Now continuing our construction, the functor we constructed (3.3.2) is a left representable pairing of categories, which induces a duality functor:
(3.3.4) |
Notice the codomain of this functor is equivalent to , where is as defined in 1.0.3.
We have a square:
Here the top horizontal functor is the duality functor we just defined (3.3.4), the bottom functor is -Koszul duality functor. The left and right vertical maps are canonical Cartesian fibrations. By restricting to small algebras and using straightening/unstraightening, we finally get a comparison morphism of the two induced functors :
(3.3.5) |
3.4 Proving induces an equivalence
Now we can finally prove our main theorem:
3.4.1 Theorem.
We’ll use some notation here:
3.4.2 Notation ((Fmp associated to an algebra)).
Given an augmented algebra , let denote the -fmp associated to . In other words,
To do this, we only have to show that after taking -fold loop spaces, we have an equivalence
since is an -proximate fmp. We use Lurie’s Proposition 1.2.10 in [Lur11] to reduce to the cases where the algebra is , as values on these algebras determine the tangent complex in our current context.
So we’ve reduced the theorem to the following proposition:
3.4.3 Proposition.
Let and . Then is the -th loop space of . This induces the following diagram:
Then the bottom map of this diagram is an equivalence.
Proof.
We have the fiber sequence . Let and .
Notice that can be identified with the fiber of the augmentation map
We’ll suppress the and from now on. These two objects are both fibers:
where we suppressed the in the subscripts. Therefore, can be identified with the fiber of the comparison map of the square
(3.4.4) |
where by ”comparison map” we mean the map from the top left corner to the pullback of the bottom and right legs.
Notice that if we take the fiber of the left map in this square, we get
and if we take the fiber of the right map in this square, we get
This shows we have a fiber sequence
(3.4.5) |
which is natural in , or more generally, any algebra. Notice this sequence is closely related to the sequence we used in 3.2.6. The second map is induced by evaluation at , just as in the square 3.4.4.
Let denote the -fmp associated to the augmented algebra . In other words,
Clearly by using the various comparison maps for each fmp (2.3.3, 3.3.5), we get the following diagram
(3.4.6) |
If we can show that the bottom sequence is also a fiber sequence, we’ll be done, as the comparison on the left would have to be an equivalence.
Since the ’s are fmps, we can push in the loop spaces to act on , giving us this equivalent bottom sequence:
Next we can combine the identify with with the free-forgetful adjunction (with nonunital algebras) to identify the sequence with
where the second map is by evaluation at , just like in 3.4.4. This is clearly a fiber sequence since
is a fiber sequence in nonunital algebras (where the second map is evaluation at ). ∎
3.5 Examples
Now we give an application of theorem 3.4.1.
3.5.1 Example (Monoidal categories and algebras).
Our main example is deforming -monoidal -categories, which includes the case of deforming -algebras as the case. These are very important in the study of shifted sympletic structures. For example, [Pan+13] discusses the relation between -Poisson structures on derived affine stacks and the deformation theory of -monoidal categories. They are also important in the study of Quantization, as discussed in [Toë14].
Given an -monoidal -category , its deformation theory is the same as the simulatenous deformation theory of the pair . Namely, theorem 3.4.1 says that -monoidal deformations of the -monoidal -category are characterized by
In the -algebra case, we see that deformations of an algebra are characterized by
where denotes the Hochschild complex of (ie the derived center of ). We can recover the classical result that first-order deformations of are characterized by when is connective. See for example [Fox93] for the case that is concentrated in degree . Note that in this case,
since is connective, by using the long exact sequence of cohomology groups. Then we use our theorem 3.4.1 to see:
and hence
We sketch the argument for deforming -monoidal -categories. Given an -monoidal -category (note that we drop the superscript sometimes, especially when we need itself as a subscript), we let be the functor that assigns to each small -algebra to the groupoid core of
where denotes the category of -monoidal -categories with a central -action, and the map is given by the augmentation map . Observe that is now an -category as it’s a category consisting of -categories with a -central action. Hence notice that taking -fold endomorphism spaces in this category produces -categories. Notice one can define using a left fibration like we do with (2.1.10).
The key insight is that we have a comparison
given by taking a deformation to . Further there’s a map
which sends a deformation to . This is an -category by what we said above. Notice that the composition
is a fibration because the monoidal categories that get sent to the basepoint of are exactly characterized by objects by Morita-equivalence arguments.
One can construct a comparison map
in the following way: map to the pair
Then we have a comparison of fiber sequences
This is an equivalence after passing to fmp completions, as the left and right legs are equivalences.
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