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Let be a skeletal 2-group with strict inverses. Then by Eckmann-Hilton is abelian. Since the map is an isomorphism, all automorphism groups are isomorphic, and hence abelian. Since is skeletal, all morphisms of are automorphisms and thus elements of these automorphism groups.
Given arbitrary morphisms , the naturality of the associator tells us that , in other words (since all automorphism groups are abelian). So tensor is strictly associative on morphisms just as it is strictly associative on objects.
The above considerations lead me to the conclusion that the associator "stands apart" from the rest of the structure of the skeletal 2-group as "extra garbage" [cf. the extra garbage discussed here.
What am I missing? In what way does the associator "matter"?
Perhaps the associator only really starts to matter once we consider non-special 2-groups in the equivalence class of ?
But if "equivalence" is the right notion of sameness for 2-groups, we should be able to see all the relevant structure just looking at special 2-groups and in a special 2-group all the actual operations , , , etc. seem to take place without involving the associator at all!
It's a cohomology class!
I know but what does it tell you?
I'm not sure what kind of answer you want.
Since you said "I know" I guess you are familiar with the classification of 2-groups in terms of the group of objects, the abelian group , the action of on by conjugation, and the class in group cohomology determined by the associator?
Yes I am familiar with that classification
That classification is my first exposure to cohomology which might shed light on my confusion
From that perspective, it's part of the data that determines the 2-group. What else do you want it to tell you?
I am surprised that it doesn't make any computation in the 2-group happen differently, other than in a tautological sense (the computation "compute the associator")
I would think 2-groups with different associators would be different in some meaningful way
I wouldn't say that. There are plenty of real calculations that can be done in a 2-group that involve the associator. It's true that in the skeletal case you could do the same calculation by omitting the associators, but that wouldn't be doing the calculation in the 2-group you had, but rather a different one with a different associator (which happens to be the identity in the skeletal case).
How can I witness the (non-tautological) ramifications of choosing a different associator on the structure of a 2-group?
Pick anything you can do in a monoidal category involving three or more objects, it will probably involve the associator.
well if we just consider skeletal 2-groups, it seems like you can do everything you want to even involving three or more objects without using the associator...
My point is that any kind of "thing you can do in a monoidal category" must be phrased in a way that involves the associator. When you specialize such a thing to a monoidal category that happens to be skeletal, the associator is still there; it doesn't magically disappear because you could have performed the same construction in a different monoidal category that happens to have the same underlying category.
I guess my question is, if we hold the triple constant, what are the stakes of choosing one associator rather than another?
Your responses make me think that to understand the significance of the associator, I need to think about possibly non-skeletal 2-groups
But that also strikes me as strange, as if (1) we are using the right notion of equivalence of 2-groups, and (2) every 2-group is equivalent to a special 2-group, then we should be able to understand 2-groups in general by thinking only about special 2-groups
It's certainly possible, but I think this may be a case of where working in more generality is actually easier, because accidental coincidences in a special case can make some things typecheck that really shouldn't.
Joshua Meyers said:
What am I missing? In what way does the associator "matter"?
In mych the same sort of way that the multiplication in a group matters. For example, groups correspond to connected pointed homotopy 1-types (very roughly, connected pointed topological spaces whose homotopy groups vanish above the first homotopy group). Similarly, 2-groups correspond to connected pointed homotopy 2-types. So, two special 2-groups that are the same except for their associator will give different-looking spaces.
How do I contruct the space corresponding to a special 2-group?
First read my papers...
I've read (most of) these papers:
Hoàng Xuân Sính’s Thesis: Categorifying Group Theory, by John Baez
Lectures on n-Categories and Cohomology, talks by John Baez, notes by Michael Shulman
Are they the ones you mean or did I miss one?
You could also point me to a particular section of one of these papers, maybe I skipped it or didn't understand when I read it...
One way to construct the space corresponding to a 2-group is as follows. Define it as a simplicial set and then take the geometric realization. In the simplicial set:
So you can see how the associator gets used.
Joshua Meyers said:
I've read (most of) these papers:
- Higher-Dimensional Algebra V: 2-Groups, by John Baez
Hoàng Xuân Sính’s Thesis: Categorifying Group Theory, by John Baez
Lectures on n-Categories and Cohomology, talks by John Baez, notes by Michael Shulman
Are they the ones you mean or did I miss one?
Yes. The paper about Sinh's thesis gives the clearest explanation of how to go back and forth between pointed spaces and 2-groups, I think. Near the end (but before the appendix.)
Mike just explained one direction. But that paper does the explanation with pictures, and I think they help.
You'll see how group elements give edges, multiplication gives triangles, 2-group morphisms and associators give tetrahedra, etc.
I see. So now it seems I need to understand Postnikov invariants
It would be great if there was a really tiny example where I could try out different associators and actually visualize the corresponding spaces.
Joshua Meyers said:
I see. So now it seems I need to understand Postnikov invariants
You are learning Postnikov invariants right now. The way the associator of a 2-group affects the corresponding space: that's the simplest example of a Postnikov invariant.
Then comes the pentagonator of a 3-group, etc.
Joshua Meyers said:
It would be great if there was a really tiny example where I could try out different associators and actually visualize the corresponding spaces.
For that I suggest taking and to be the smallest nontrivial group discovered by humanity so far. Then there are two really different choices of associator, giving two inequivalent 2-groups.
Here is what I got for and both the cyclic group of order 2 and the trivial action (it is indeed the only action). There are two possible associators, giving two inequivalent 2-groups, giving two inequivalent spaces.
2024-04-06-105352.jpg
In this picture, is "and", defined by iff and , btw
Now, what I don't know how to do, even in this simple example, is visualize the spaces enough to see what difference the circled makes. When I try, I start to think of each pair of 2-cells as a sphere with three points pulled out of it and joined together. But then I have no idea how to think of all eight 2-cells together, and that doesn't even get started on the tetrahedra. Is there a topology text I should study that would make me able to visualize spaces like this?
Or another possible answer is that people don't usually visualize these spaces, they just leave them as descriptions on the paper. But I would hope that in as simple a case as this, the spaces would be susceptible to some nicer description which I could begin to visualize.
People don't usually visualize these spaces except in a very subtle sense of "visualize", because they are infinite-dimensional.
There are things you can do to better understand them, though.
I'd start by pondering the famous 'Eilenberg-Mac Lane spaces' and .
is the connected pointed space whose only nonvanishing homotopy group is .
is the connected pointed space whose only nonvanishing homotopy group is .
Both the spaces you're talking about, say and are built from and .
In technical terms, we say both and aretotal spaces of bundles over , and both have the same fiber, which is called .
In other words we have a map
and this map looks locally like the projection from to . And the same is true for !
So your spaces and are very similar; the only difference is that one of them - the one with the trivial associator - actually is the product , while the other - the one with the nontrivial associator - is only locally a product.
(What I'm doing now is teaching you the theory of 'Postnikov towers' in an example, namely the example where and happen to be . Everything I'm saying works more generally.)
Now is an extremely important space, and there are lots of ways to visualize it and understand it. For one thing, we can show that this space is , the infinite-dimensional real projective space.
One way to understand this is to build it up using simplices and show that the -dimensional approximation to this space, where you go up to the -simplices, is , the n-dimensional real projective space.
This is tons of fun, but probably more fun if you've already thought a bit about real projective space.
One reason this stuff is tons of fun is that it involves an idea you've already invented: using logical operations on bits! Given what you've already done, it should not come as an utter and complete shock that we can describe using bit strings!
I will get to this in about a week and a half! I didn't forget about it, just preoccupied with other things
I will work out the topology soon, but I just wanted to say I found another way of thinking about this, through strictifications. Let be a strict monoidal category whose objects are the monoid which is monoidally equivalent to our skeletal 2-group . Then is a groupoid and each object has exactly 2 endomorphisms. There are two connected components, even numbers and odd numbers. Let be non-identity, and let and be chosen to correspond to the identity on the unit of under the equivalence.
Then the morphisms of are generated by . This is easier to show with string diagrams, which can be used without guilt since is a PRO. We denote as a dot, as a cap, and as a cup. Because of the equivalence, we must have and inverse, so in the string diagrams, a circle can vanish, and a pair of vertical parallel lines can split into a cup and a cap. We then note that a dot is equal to a double-circled dot, so a circled dot must also be non-identity, and thus must be equal to a dot. We are then confronted with the question of the zigzag -- when you pull it straight to a vertical line, does a dot pop out beside it or not? It can be shown that this choice completely determines the rest of the structure of , and both choices are consistent.
I am confident that the two choices of the zigzag correspond to the two choices of the associator, but I have not proven the existence of these equivalences.
Update: I did prove their existence
Cool. I will have to think about this.