Arrow-Theoretic Differential Theory
Posted by Urs Schreiber
Using the concept of tangent categories (derived from that of supercategories) I had indicated how to refine my previous discussion of -curvature. Here are more details.
Arrow-theoretic differential theory
Abstract: We propose and study a notion of a tangent -bundle to an arbitrary -category. Despite its simplicity, this notion turns out to be useful, as we shall indicate.
1 Introduction … 1
2 Main results … 2
2.1 Tangent -bundle … 3
2.2 Vector fields and Lie derivatives … 4
2.3 Inner automorphism n-groups … 4
2.4 Curvature and Bianchi Identity for functors … 5
2.4.1 General functors … 5
2.4.2 Parallel transport functors and differential forms … 6
2.5 Sections and covariant derivatives … 6
3 Differential arrow theory … 8
3.1 Tangent categories … 8
3.2 Differentials of functors … 11
4 Parallel transport functors and their curvature … 12
4.1 Principal parallel transport … 12
4.1.1 Trivial G-bundles with connection … 12
Introduction
Various applications of (-)categories in quantum field theory indicate that (-)categories play an important role over and above their more traditional role as mere organizing principles of the mathematical structures used to describe the world: they appear instead themselves as the very models of this world.
For instance there are various indications that thinking of configuration spaces and of physical processes taking place in these as categories, with the configurations forming the objects and the processes the morphisms, is a step of considerably deeper relevance than the tautological construction it arises from seems to indicate.
While evidence for this is visible for the attentive eye in various modern mathematical approaches to aspects of quantum field theory – for instance [FreedQuinn], [Freed] but also [Willerton] – the development of this observation is clearly impeded by the lack of understanding of its formal underpinnings.
If we ought to think of configuration spaces as categories, what does that imply for our formulation of physics involving these configuration spaces? In particular: how do the morphisms, which we introduce when refining traditional spaces from 0-categories to 1-categories, relate to existing concepts that must surely secretly encode the information contained in these morphisms. Like tangent spaces for instance.
Possibly one of the first places where this question was at all realized as such is [Isham]. That this is a piece of work which certainly most physicists currently won’t recognize as physics, while mathematicians might not recognize it as interesting mathematics, we take as further indication for the need of a refined formal analysis of the problem at hand.
Several of the things we shall have to say here may be regarded as an attempt to strictly think the approach indicated in Isham’s work to its end. Our particular goal here is to indicate how we may indeed naturally, generally and usefully relate morphisms in a category to the wider concept of tangency.
For instance his “arrow fields” on categories we identify as categorical tangents to identity functors on categories and find their relation to ordinary vector fields as well as to Lie derivatives, thereby, by the nature of arrow-theory, generalizing the latter concepts to essentially arbitrary categorical contexts.
While there is, for reasons mentioned, no real body of literature yet, which we could point the reader to, on the concrete question we are aiming at, the reader can find information on the way of thinking involved here most notably in the work of John Baez, the spiritus rector of the idea of extracting the appearance of -categories as the right model for the notion of state and process in physics. In particular the text [BaezLauda] as well as the lecture notes [Baez] should serve as good background reading.
The work that our particular developments here have grown out is described in [S1, S2]. Our discussion of the Bianchi identity for -functors should be compared with the similar but different constructions in the world of -fold categories given in [Kock].
Main results
Our working model for all concrete computations in the following is , the Gray category whose objects are strict 2-categories, whose morphisms are strict 2-functors, whose 2-morphisms are pseudonatural transformations and whose 3-morphisms are modifications of these. It is clear that all our statements ought to have analogs for weaker, more general and higher versions of -categories. But with a good general theory of higher -categories still being somewhat elusive, we won’t bother to try to go beyond our model .
So we shall now set once and for all and take the liberty of using instead of 2 in our statements, to make them look more suggestive of the general picture which ought to exist.
Tangent -bundle
We define for any -category an -category which is an -bundle over the space of objects of . This we address as the tangent bundle of .
The definition of this tangent bundle is morally similar to but in detail somewhat different form the way tangent bundles are defined in synthetic differential geometry and in supergeometry:
we consider the category as an arrow-theoretic model for the “infinitesimal interval” or the “superpoint” in that it is a puffed-up version of the mere point to which it is equivalent, by way of the injection but not isomorphic. This suble difference, rooted deeply in the very notion of category theory, we claim usefully models the notion of tangency as “extension which hardly differs from no extension”. Concretely, we consider to be that subcategory of morphisms from the fat point into which collapses to a 0-category after pulled back to the point .
The characteristic property of the tangent -bundle is that it sits inside the short exact sequence
Finally, for later use notice that dual to its realization as a projection the tangent bundle may be thought of as an -functor which sends objects to the tangent categories over them and sends morphisms the the pullback of these along them
Vector fields and Lie derivatives
Let be a smooth manifold and let be the groupoid of thin homotopy classes of paths in .
Then ordinary vector fields on are in canonical bijection with smooth 1-parameter families of categorical tangent vectors to the identity map on :
On a general category , it may be useful to consider generalizations of this where is replaced by some other group . We speak of -flow on a category, in this general case.
The “arrow fields” on a category , considered by Isham in [Isham], are -flows on .
On the other hand, the identitfication of itself (as opposed to ) with ordinary vectors for suitable choice of is both more subtle and more interesting than the above. This will be discussed elsewhere, once fully worked out.
Inner automorphism -groups
Of particular importance are the tangent bundles, in our sense, to -categories which are 1-object -groupoids , hence -groups . In our context these -groupoids must be thought of as 1-point orbifolds. Accordingly, they have just a single “tangent space” (tangent -category)
This turns out to have interesting properties [Roberts-S]:
For an ordinary group, one finds that is a 2-group, which we call . It sits inside the exact sequence of 1-groupoids. Here is the categorical center of (which coincides with the ordinary center of ), regarded as a 1-object groupoid. This identifies as the 2-group of inner automorphisms of . But also sits inside the exact sequence Moreover, it is equivalent to the trivial 2-group, hence “contractible”. This identifies as the categorical version of the universal -bundle.
For a strict 2-group, one finds that is a 3-group, which we call . It sits inside the exact sequence of 2-groupoids. Here is the 2-categorical center of , regarded as a 1-object 2-groupoid. This identifies as the 3-group of inner automorphisms of . But also sits inside the exact sequence Moreover, it is equivalent to the trivial 3-group, hence “contractible”. This identifies as the categorical version of the universal -2-bundle.
Curvature and Bianchi Identity for functors
General functors
Using the functorial incarnation of the tangent bundle, we may push forward any -functor to a connection on the tangent bundle of , simply by postcomposing The crucial point of this construction is that it extends uniquely (up to equivalence) to an -functor on the -category which is obtained from by replacing all Hom-()-categories by the corresponding codiscrete -groupoids over them.
By introducing the terminology
is the curvature of
is flat if is degenerate (sends all -morphisms to identities)
we obtain the technically easy but conceptually important generalization of the Bianchi identity: for any functor
is flat
or equivalently
is degenerate.
Parallel transport functors and differential forms
When is the smooth parallel transport functor \cite{transport} in an -bundle with connection [Bartels,Baez-S,S3], the arrow-theoretic notion of curvature described above does reproduce the theory of curvature forms of connection forms. The general Bianchi identity we have discussed then reduces to the ordinary Bianchi identity familiar from differential geometry.
More precisely, let be the strict 3-groupoid of thin homotopy classes of -paths in a smooth manifold . And let be a strict Lie 2-group coming from the Lie crossed module .
Then, according to [S-Waldorf,Baez-S,S3,Roberts-S] we have the following bijections of smooth -functors with differential forms
Now let be a smooth 1-functor with values in the Lie group . Then, under these bijections, we find that its curvatures correspond to the following differential forms at top level
This way the ordinary Bianchi identity for the curvature 2-form of is reproduced. Notice that for this result come out the way it does, just by turning our abstract crank for differential arrow-theory, the result of \ref{Inner automorphism -groups} is crucial, which says that the curvature -functor of a -transport is itself an -transport.
Sections and covariant derivatives
The curvature of a parallel transport -functor is typically trivializable, in that it admits morphisms for some “trivial” -transport. As with the inner automorphism -groups , this trivializability, far from making these objects uninteresting, turns out to control the entire theory.
(Compare this to the contractibility of the universal -bundle: while equivalent to a point, it is far from being an uninteresting object, due to the morphisms which go into and out of it. According to the above this comparison is far more than an mere analogy.)
A basic fact of -category theory has major implications here:
recall that for and -functors, a transformation is given in components itself by an -functor. Now if is trivial in some sense to be made precise, and if the transformation is an equivalence then this implies that the -functor is entirely encoded in the -functor .
We show that for the curvature -functor of a transport -functor , the latter essentially encodes the component map of the transformation In components this is nothing but a generalization of Stokes’ law
Moreover, it turns out that there may be other trivializations of , not by isomorphisms but by mere equivalences. On objects, the component functions of these correspond to sections of the original bundle. On morphisms it corresponds, under the identification of smooth functors and differential forms mentioned above to the covariant derivative of these sections.
In [S1] it is indicated how all these statements have a quantum analogue as we push our -functors forward. There it is indicated how the fact that transport have sectins which are themselves transport -functors translates in the context of extended functorial quantum field theory to essentially what is known in physics as the holographic principle. This needs to be discussed elsewhere, clearly.
Re: Arrow-Theoretic Differential Theory
Hi,
So just as a background I have a beginning graduate level knowledge of diff geo, am half-way through Saunders Mac Lane, and read Baez and Dolan’s Categorification only once. So I’m not exactly the target audience of this…yet.
That being said, there’s a couple of things early on that made my brain grind to a halt.
First, in what way are pt and pt equivalent? It looks like you are just including pt in as the first point of pt and then the equivalence is just given by lifting up or projecting down the first point. The context makes it sound more subtle and complicated than that though, so what am I missing?
Also, I feel like I’ve read the first section a few times and that I’m still not seeing the connection between tangent vectors/bundles from diff geo with what you’re doing here. I’m used to a vector field being a map from the smooth functions on a manifold to itself. I don’t really see how what we’re defining is equivalent to that for 0-categories (is it supposed to?). Is the answer related to the requirement of Mor(C) -> TC -> C being a short exact sequence? What exactly is Mor(C)?
Sorry for the questions, but I appreciate any help.