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What else do we have to know before we can move on to Galois descent?
Nothing! So, I'll make this a new topic.... though eventually it will loop back to Galois cohomology.
So, descent is fundamentally a question like this: you have a functor
and you take an object of and you ask "did it come from an object of "?
Of course it might have come from more than one object of , so instead of asking about the property of whether it came from an object of it's better to think of this as a structure!
So, the question of descent becomes "how can we nicely describe the structure on objects of that says how they came from a object of ?"
Get it?
It's pretty clear how fibrations connect to descent now.
John Baez said:
So, the question of descent becomes "how can we nicely describe the structure on objects of that says how they came from a object of ?"
is this backwards?
It's backwards, let me fix it in my original comment.
Yes, fibrations are connected to descent.
And here's another way they're connected to descent - maybe it's a different way than what you were thinking of, but maybe it's connected.
Suppose you have a map of spaces . Say you've got a category of bundles or sheaves up on and a category of bundles or sheaves down on . Can you say how descent, as I've described it, shows up here?
(Just pick bundles or sheaves of any kind you like; it doesn't matter much.)
(Btw, for people joining, I like to teach math by asking lots of questions, which are usually supposed to be fairly easy for my intended audience - in this case @Joe Moeller.)
well, there's an adjunction between the categories of sheaves on E and B—are you talking about descent from sheaves on E to sheaves on B, or vice versa? :thinking:
or is that the puzzle? :)
That's half the puzzle. You can push forwards and pull back sheaves, so you could in theory study descent going either way.
I think you want the functor from bundles on E to bundles on B given by composing with p. Then the question of descent for that functor is when does a bundle on B factor through p? Right?
Right!
ooooh right, that's exactly what pullback of bundles is
Wait, wrong!
and then that's exactly what lifting problems are
oh oops lmao
Joe said something sorta wrong.
It sounded so much like the right answer that at first I assumed he'd gotten it right.
I'll let you two clear it up.
oops
I'll just say this: when Sarah said "that's exactly what a pullback of bundles is", it didn't match what Joe had just described. Why not? Sort it out!
yeah i kinda started to notice something wrong when i went back to see what you were complaining about...
What I described is not pulling back.
You were "pushing forward" a bundle.
i always super super hate how it's contravariant to go from p to p⁻¹ and then it's contravariant again to go from p⁻¹ to certain topos functors
If your "bundle" means just a map of spaces, you can push it forward. But most people want bundles to be slightly nice, like "locally trivial".
Then you can't push them forward, in general. You can only pull them back.
For example, suppose I have a Mobius strip bundle over a circle - that's a certain locally trivial bundle whose fibers are lines.
the double contravariance trips me up every goddamn time when i forget one of the two flips
So if we're talking about pulling back bundles from B to E, then the descent question is when is a bundle on E a pullback of a bundle on B.
Say I map the circle to a point. What happens if I try to push forward this Mobius strip bundle? What do I get?
You're right, Joe - and that's why it's called DESCENT and not ASCENT.
You're trying to see if a bundle "up on " descends to one on the "base" . This is the same as seeing if it's a "lift" of a bundle on .
But please answer my latest question, just to make sure we know what's going on....
ooh, a whole bundle, not just a section of a given bundle?
:eyes:
Surely there's only one bundle on a point with a given total space, so it will just be that
So what's that?
The map from the Mobius strip to the point
The bundle should be the line over the point.
Oh, goody! The great thing about having more than one student is that they give contradictory answers and learn by fighting it out.
So we've got two answers to what happens if you push forward the Mobius strip bundle over the circle along the map from the circle to the point.
Joe gave a clear recipe for how this pushing forward should work, so one can just follow that recipe and see what it gives.
The line over the point is what you would get if you pulled back the bundle along an inclusion of the point into the circle
meanwhile im sitting here unsure what it means to push a bundle forward :sob:
What it "means" in a deep philosophical way, or how to do it?
the latter!!
The most general concept of a "bundle" over a space is just a map .
well, i know that
im pretty happy with pulling bundles back and what that means
Can you guess how to push it forward along a map ?
.........is it a pushout :face_palm:
noooo wait that doesnt even
You can't draw a pushout with the data I gave.
the arrows go the wrong way what am i saying
Right - wrong!
yeah im not sure
other than to wildly guess it's what direct image of sheaves does
So what do you do? You gotta do what you can do with the stuff you've got.
Draw the diagram:
Come on, you're "overthinking" it Sarah. Usually people say that when they're underthinking it, but here you are really overthinking it.
\>.>
omg oscar
literally just compose?
Yeah!
for fucks sake
You have reinvented "composition of morphisms" :tada:
I figure I can be a bit sarcastic without permanently damaging you...
:O cant believe i managed to do what took eilenberg and mac lane previously .....
That's what he meant when he said that I gave a recipe for it, I said you get a functor by composing with p.
Right!
well, i wasnt even wrong about direct image of sheaves then was i?
So this very general concept of "bundle" easily pushes forward.
My answer came from saying "vector bundle" in my head. So I was trying to think what should the vector space over the point be when I compose with the map from the circle to the point. I think this is an error. The answer should be the mobius strip over the point.
Right!
So this way of pushing forward bundles is pretty bad if you like bundles with a fixed fiber, like "line bundles".
Or even more generally "vector bundles".
We took a vector bundle over the circle, pushed it forward to the point, and got something that wasn't a vector bundle.
So geometers generally consider pushing forward bundles to be a horrible thing to do.
It's not to be discussed in polite society.
Henceforth we will only pull back bundles.
And it sounds like y'all know how that works. It's literally just a pullback in the categorical sense.
You've got your bundle and a map and you do the pullback you can do with that data.
This is nice because line bundles pull back to give line bundles, vector bundles pull back to give vector bundles, principal -bundles pull back to give principal -bundles, blah blah blah.
The reason is that the fibers of your new bundle over points in your new base are just copies of fibers over the the points of your old base .
So the fun starts when you ask: given a bundle over my new base , could it be the pullback of a bundle over the old base ?
I see my letters have changed by now.
But this is the "descent" question.
Let me see if you get it. Say is a circle but is the 2-1 cover of the circle by itself.
Say is the Mobius strip bundle over . Does it descend to ?
One condition is that points of that go to the same place in should have the same fiber
I'll say no. I think the double twist would descend to the Mobius strip though.
wait wait i wanna think about this
i havent visualized it yet
Yes, all of you should visualize it. A couple of comments: 1) "the same" is a very tricky concept.
2) "the double twist" line bundle over the circle is a funny thing to talk about.
so this is sort of an extension problem, huh
if we assume that there's a classifying space for the kind of bundle we're talking about
right?
The fibers of the Mobius bundle are all homeomorphic. But I think Joe's right, there's some 'global' obstruction.
People would usually call this a "lifting" problem not an extension problem.
i wanted to say it was a lifting problem but i think the arrows go the wrong way around??
they call it ... a "descent" problem
Classifying spaces are too fancy for what we're doing right now, btw. This is just pictures of circles and stuff.
classifying spaces are great for pictures of circles >:(
How I'm visualizing this is that the question is whether there's a space over the circle such that if you un-doublecover the circle, and you bring along the space for the ride, it turns into the Mobius strip.
yeah
Yeah, my comment about a lifting problem was backwards. I guess it is an extension problem, abstractly - I got confused because we're "extending" along a 2-1 map, not an inclusion!
if you want to think of it in terms of classifying spaces, though, you have a map from to some fancy classifying object and you want to "descend" the domain of the map to .
I really don't want to talk about classifying spaces now.
But yes, you are right.
why, does it make the answer too easy >:)
It's too fucking abstract!
:cry:
We're doing stuff that could be done in kindergarten!
I think un-doublecovering any line bundle over the circle should double the number of twists.
Joe is saying the right kind of stuff... let me actually focus on it.
no yeah im trying to think about that sort of concurrently
What the hell is "un-doublecovering"? :upside_down:
pulling back over the double cover
Okay.
but it's what I made up to convey my visualization
So you're saying: if I have a line bundle over the circle with n twists, and I pull it back along the 2-1 cover of the circle by itself, I get a line bundle with 2n twists.
yes
What do the rest of y'all think about that?
hmmmmmmmmmm
That's very true, Sarah.
Joe: what's funny about the line bundle over the circle with 2 twists? I asked this before...
i suspect it may be topologically indistinguishable from the trivial line bundle
You can make one out of paper...
If your line is sufficiently short...
sure, but that's an embedding into R³
the horned sphere is a thing too
They are not homeomorphic.
as an abstract space, u get the möbius strip from a square by just gluing one side to the opposite side w/ a reversing map
Oh, good, a fight! Are they homeomorphic or not?
the reversing map is the only thing that distinguishes from the untwisted bundle
but a double-twist strip doesnt have a reversing map
Notice there are two questions: are the total spaces homeomorphic, and are they isomorphic as bundles.
wait
god dammit
I don't know what a reversing map is.
well, whats yr argument joe? im kinda charging in w/o full thought :upside_down:
reversing map—sorry, i mean you quotient one copy of [0, 1] to another by 1 - x
where these copies of [0, 1] are the edges
So, we've got two questions on the burner now:
1) Is Joe's idea true: if we have a line bundle over the circle with n twists, and we pull it back along the 2-1 cover of the circle by itself, we get a line bundle with 2n twists.
2) Is the bundle with 2 twists isomorphic to the bundle with 0 twists?
I take it back, I think the double twist is homeomorphic to the cylinder.
So have you changed your mind too, Sarah, so you can keep arguing with Joe but on opposite sides?
It's always fun when that happens.
I was thinking too much about the embedding before.
on a möbius strip there is only one side
I think I can imagine a homeomorphism between the double twist bundle and the no-twist one.
It's easiest to describe this way. I can make both these bundles out of a rectangle of paper.
The obvious "identity map" between rectangles of paper gives a homeomorphism between these bundles.
(...how are you defining the double twist bundle?)
I'm taking a long thin rectangle of paper, twisting it twice, and attaching the two ends in the sorta obvious way.
yes, but critically, you can evaluate the map on two chunks, away from the gluing area, and around the gluing area.
@John Baez a dangerous thing to rely on when making the leap to formal claims :flushed:
In topology if you can't prove things with twisted pieces of paper and pictures you're on really shaky ground.
this is also true :thinking:
i await your picture proof that locally compact spaces are exponentiable :)
Once people start scribbling weird letters they can get in all sorts of trouble. :upside_down:
Anyway, I'm claiming the total space of the the double twist bundle is "obviously" , where now I'm making the line compact just for fun...
end compactification :eyes:
I make it by taking a long thin rectangle of paper, twisting it twice, but then identifying points using the identity map on [0,1].
use the open interval instead.
True, cheap paper leaves out the edges.
having a compact total space seems nice :>
Anyway, so please classify "line bundles with n twists over the circle", for all n.
cylinder, Mobius.
Right: Z gets mapped to Z/2.
Okay, so you've classified real line bundles over .
You got Z/2.
For fans of classifying spaces, this is because of the relevant classifying space is Z/2.
Or better: we've proved that of the relevant classifying space is Z/2.
is it rp2
It's , actually.
O:
It's the Eilenberg-Mac Lane space of Z/2.
Classifying spaces tend to be ginormous.
right that sounds familiar
Okay. Now that you understand all line bundles over the circle, describe the process of lifting a line bundle on the circle to one on its double cover!
This is how to completely crush this example of "descent": completely understanding lifting.
Lifting anything gives the cylinder.
thats what id guess as long as you really do double the number of twists
Can you say it nice in terms of Z/2?
:eyes:
Z/2 is annihilated by uh
2Z
multiply by 0
There's actually a group of line bundles on the circle, and it's Z/2.
The reason is that you can "tensor" line bundles - the tensor product of two 1d vector spaces is a 1d vector space.
So there's always a group of line bundles over any space.
And we've seen this group is Z/2 for the circle.
Yes, I'm imagining doubling the twists, but now that we established you can cancel two twists, I'm simplifying.
I don't like how you're simplifying.
It's okay, but I have something else in mind.
We have a map Z/2 -> Z/2.
The zero map.
You can call it "multiplying by 0", but I'd rather not.
Do you want us to say the word 'homomorphism'?
Well, we've been lifting along a double cover.
'Doubling'?
What if we lifted along the triple cover of the circle by itself?
We'd get some map Z/2 -> Z/2 again...
coprime
doesnt annihilate
i think
All these words are good, but I like what Joe said.
~_~
Lifting along an n-fold cover gives a map Z/2 -> Z/2, and it's just multiplication by n.
So I wanted Joe to say "multiplying by 2", but he said "multiplying by 0".
You really do get a double twist bundle when you lift the single twist bundle along the double cover, but it just happens that 2 = 0.
I'm getting a bit worn out, but I'll wrap up.
We've seen that descent quickly gets us into some algebra... some algebraic topology for example.
Bundles over the circle are particularly simple because they're completely described (up to iso) by a "twist", which is an element of some group.
So descent in this case boils down to stuff about group homomorphisms - what's their image, and how many group elements map to one (so what's their kernel).
We saw that 2: Z/2 -> Z/2 was two-to-one and half-onto, so only half the line bundles "descend" along the double cover of the circle by itself, and the one that does *descends in two different ways".
As soon as we leave the circle and work with more fancy spaces, we'll need to think about "transition functions" also known as "2-cocycles".
So this gets us pulled into sheaves and sheaf cohomology pretty quick...
But where I really want to go is algebraic geometry, where we think of fields as fields of functions on certain spaces called "schemes"; then the fundamental group we were just playing around with - the fundamental group of the circle was hiding in what we did - will be called a "Galois group".
isnt the only kind of space whose ring of functions is a field, a point
The question "does an algebraic gadget defined on a big field K come from extending an algebraic gadget defined over some subfield k" turns out to be another case of descent.
Yeah, it's funny: fields are like points, but they still have holes in them, leaving a fundamental group.
This is one of the enduring mysteries of algebraic geometry.
hmmmmmmmmmm
James Dolan spoke of "voodoo mathematics" - the study of spaces that have been poked so full of holes that every point is a hole.
The "etale fundamental group" of a field is its absolute Galois group - this is what Artin and Mazur showed, I guess.
/me opens the nlab page on galois theory again
Anyway, this is just a taste of stuff... I basically prefer to move sort of slowly, so we all have time to really get all the concepts clearly, and so I have time to study enough to continue seeming smart.
OH NO THE NLAB IS DOWN
me but with nlab https://xkcd.com/903/
Ugh. It's the 0Lab now, eh?
Btw, @Joe Moeller - one fun part is how all the stuff I just toured at the very end is connected to Brauer groups. Brauer groups are really connected to descent and "bundles".
Great! How?
That's for later...
Okay, last time we discussed a nice example of descent. We looked at pulling back real line bundles from the circle to its double cover (which happens to also be a circle). We studied the "descent" question: when is a line bundle on the double cover the pullback of a line bundle on the circle?
We kinda roughly saw that there was an abelian group of line bundles on any space, which for the space is just . We saw that pulling back line bundles gives a homomorphism between such groups.
Thus, the descent problem in this case is just about figuring out the image and kernel of a group homomorphism! The image tells us which line bundles are pullbacks. The kernel tells us how many different line bundles pull back to give a given bundle.
In our example the homomorphism was
which Joe called
I called it multiplication by 2 because pulling back a line bundle to the double cover of the circle doubles the number of twists it has: you can see this very clearly.
But a real line bundle over the circle has either 0 or 1 twists, and we're working mod 2, so doubling the number of twists is the same as getting rid of all the twists!
The image of our homomorphism is so the only line bundle that "descends" - the only one that's a pullback - is the untwisted bundle.
The kernel of our homomorphism is so if a line bundle descends, it does so in two ways.
Now, how should we go further? We could look at real line bundles on all possible spaces, not just the circle. This is still pretty manageable. It would get us into a little bit of sheaf cohomology.
We could go further and look at all vector bundles over all spaces.
We could go further and look at all principal bundles over all spaces.
We could go further and look at all sheaves over all spaces.
We could go further and look at all sheaves over all sites.
We could then specialize and look at sheaves over schemes with their etale topology.
We could then specialize even more and look at schemes that come from fields. Then we'd be doing "Galois descent".
Or, we could head straight for Galois descent - this is a subject people study without necessarily knowing all the more general cases I've just listed!
I guess someone should say what they want to do.
i would say something except i have some loose ends ive been procrastinating on tying up that ive finally gotten around to trying to look at so i cant pay attention right now
Okay, no problem! I've got some other customers...
It might be a longer journey, but I would love to understand how the descent that's been discussed so far relates to the theory of descent in topos theory (perhaps this is the "all sheaves over all sites" option). There seems to be a comparable motivation of wanting to identify how data descends from the domain of a geometric morphism, but (in the Elephant, at least) there is an extra step: we construct a category of "things which behave as if they are in the image" and call a geometric morphism "descent" if the codomain is equivalent to that category.
However, the choice of data here is still quite mysterious to me, and is not arrived at very organically in that text.
If that option is too much of a tangent for this topic, I'm happy to move it to #theory: topos theory.
Morgan Rogers said:
It might be a longer journey, but I would love to understand how the descent that's been discussed so far relates to the theory of descent in topos theory (perhaps this is the "all sheaves over all sites" option).
That's a fun journey. We'd been studying descent for real line bundles: i.e. given a map , when is a line bundle over the pullback of one over ? In fact we just did it when is the double covering of a circle by itself.
But line bundles over space are a special case of vector bundles over spaces, so we can ask the same question for those.
And vector bundles over spaces are a special case of sheaves on spaces, so we can ask the same question for those.
And sheaves over spaces are a special case of sheaves on sites, so we can ask the same question for those.
And sheaves on sites are a special case of objects in elementary topoi, so we can probably ask them question for those, though here my understanding gets very fuzzy.
Category theorists might be tempted to quickly jump to the highest level of generality and then climb on down. Normal people might prefer climbing up the ladder of generality one rung at a time. But either way, each level has its own special features that are worth understanding!
category theorists VS normal people :thinking:
I think I'm more comfortable near the bottom of the ladder, since I've spend lots of time thinking about line bundles and vector bundles, and less about sheaves on spaces, and so on.
Normal people: "what is an example of this?" Category theorists: "what is this an example of?" They are dual.
Anyway, I'm happy to explain anything I actually understand.... and happy to try to understand anything anyone else explains, in the subject of "descent".
Maybe one place to start is this very brief snippet on descent for vector bundles:
Here is an open cover of a topological space by a bunch of open sets , so .
Does everyone get the idea here?
Ooh expressions in terms of pullbacks are starting to appear, and the description of "being able to glue the bundles together into a bundle over " feels a lot like an extension of the sheaf condition
Morgan Rogers said:
Ooh expressions in terms of pullbacks are starting to appear, and the description of "being able to glue the bundles together into a bundle over " feels a lot like an extension of the sheaf condition
This is why the category of bundles over a space is a stack (or 2-sheaf). The descent condition is roughly the same as the sheaf condition, after replacing by .
Funny story about this:
I was in Bonn for 1 year as a MSc student, and one of the algebraic geometry exam questions was something like:
"Let F be a sheaf on an irreducible topological space X, such that F is locally the constant sheaf. Show that F is a constant sheaf itself."
I already spent too much time on the other questions, and I was incredibly confused by this. If it is locally equal to the constant sheaf, then of course it is also globally equal? Of course, what was meant is "F is locally isomorphic to the constant sheaf" (because equality is an "evil notion").
My problem was that the professor was working in the 2-sheaf of sheaves on X, while I was working in the sheaf of sheaves on X. :smiley:
i have made the exact observation before that uh
the reason why locally constant sheaves on a connected space can be nontrivial even tho locally constant functions on a connected space are always constant
is precisely b/c you generally assume contractibility of your notion of "equality" for the codomain of a "function on a space"
whereas stalks of sheaves can be isomorphic to one another in different ways
so u get monodromy.
All this is nice. Maybe I'll ask a lowbrow concrete question or two just to keep us from floating into the stratosphere and dying of oxygen deprivation.
Puzzle. Say we have an cover of a topological space by open sets and a trivial -bundle on each . What data do we need to choose to glue these together and get a vector bundle on ?
Puzzle. If I choose some data of this sort and so do you, when do they give isomorphic vector bundles on ?
So, the first question asks for the descent data in this situation. The second asks when two choices of descent data are isomorphic. When we answer these we'll be well on the road to having a groupoid of descent data - though knowing when two things are isomorphic is not as good as knowing what's an isomorphism.
hmm :thinking:
oooooooooh! i see how this relates to higher sheaf stuff now 🤯
but uh thinking thru what the concrete situation actually looks like...
we definitely at least need , where means the restriction of our trivial bundle over to the subset , and means
Right!
and i think we want a clique condition
like
no wait
no wait do we
yeah i think we do
Yes, we do!
i was thinking that would make the bundle trivial, but
right, this only applies to like... shrinking down an intersection to include intersecting more pieces
not zipping over to some distant place
Can you tell me how to build the Mobius strip bundle this way?
no im hungry and cant think at full capacity im gonna go get a snack
We can cover the circle with just two contractible pieces of we want.
:sob:
Okay. Either you or someone else should see how what you just said works in our good old example.
(People who know all this stuff too well should stay quiet.)
We can wait for Sarah to eat.
For the mobius strip, don't you just repeat what you would do with the paper strip ? Like if we cover the circle by two contractible covers, we take 2 strips of papers (our trivials bundles) and glue them "normally" on one side and with a twist on the other side
Right!
We discussed it earlier in this thread; now we're trying it again with a bit more math.
I think I want to get Sarah to work through the details.
But it'd be great to have you join this "class".
Sorry to barge in suddenly, I have been silently following this thread with a lot of attention, it really helps making these things clearer :)
Great! I'm glad you barged in! Since I have no idea how many people are paying attention, I tend to feel almost nobody is, which makes me unhappy.
With so many users in the server, there are certainly many more silent watchers for any given topic than you would imagine.
hello i got distracted after coming back
mobius...
Did you ever watch Mobius strip?
so your base space is S¹. say it's covered by U₁ and U₂, defined by intersecting with half planes
is mobius strip the name of a show or something
No, he was actually a strip-tease artist in his spare time.
:weary:
Anyway, yes, you're doing great! Two open subsets!
i feel like maybe thats not an appropriate joke for this community
<.<
but, uh
Okay, I'll try to be more serious in the future.
(idk about failure to be serious being the problem, more the risque-ness)
we need f₁₂ and f₂₁, and the clique condition (i shouldve included a clause about f_{ii} = id) says they're inverse, so that's just f₁₂
so a vector bundle automorphism of
has two connected components, so we can just define this piecewise—on one, it's the identity; on the other, it's negation on the coordinate
hmm, giving the data like this kinda reminds me of the tiny tiny bit ive read about čech methods...
Great! By the way, this "clique condition" is exactly right now, and it's exactly what people call the 2-cocycle condition.
i always forget the 0-ary clause in definitions like that >_<
i need to remember to use unbiased versiosn more often
Right! But you seem to know the 0-ary thing has to be in there.
i mean
it always is
in things like this
Good! So, what you've just given is called a 2-cocycle in Cech cohomology.
HA i was right about the čech thing
🇨🇿
Yes, you can čech that off your bucket list now.
Was that a suitable joke for this forum?
🪣
That symbol doesn't display for me, which may be all for the best.
Let's mine this example a bit more. You said was 1 or -1. What's the deal with these numbers?
i said no such thing
You said "on one, it's the identity; on the other, it's negation on the R coordinate."
That's a long-winded way of saying 1 or -1.
that was all a single :)
but i'm being obnoxious, i know what you're getting at
we can refine the cover until the intersections are connected, right?
Okay, fine. But my question was: what in general could your take values in?
Yes, on a tolerably nice space you can always use a "good cover", where all the the opens and all their intersections are contractible (or empty).
https://en.wikipedia.org/wiki/Good_cover_(algebraic_topology)
well, we're giving automorphisms of trivial line bundles, so that's a continuous function to GL(1) right
Great!
So yes, you gave me a "Cech 2-cocycle valued in the sheaf of continuous GL(1)-valued functions"... I think that's what the experts call it.
hmm..... something something do we only need a homotopy class to determine the bundle up to isomorphism :thinking: isn't that a condition that appears in the theory of classifying spaces
Right, and that sort of thing shows up in this Cech story too.
Now, you'll notice that while your cocycle took values in GL(1), it actually took values in something smaller!
What's that?
S⁰
cuz we can homotope anything in GL(1) to something in S⁰
what is GL(2) shaped like
Great! In this game is usually called .
dammit
and here i was feeling good about noticing it was S⁰ and not just {-1, +1} :D
It's okay; I just want to be able to generalize to higher dimensions!
mostly being tongue in cheek :)
is the group of rotations/reflections of .
One great thing is that it's a maximal compact subgroup of .
oh cool
An amazing fact about Lie groups is that they're all homotopy equivalent to any maximal compact subgroup!
:o
i think i remember SO(3) being the same as RP³... is there something similar for O(n)
Even better, any Lie group is, as a manifold, a product of "the" (any) maximal compact subgroup and a vector space.
or at least SO(n)
wow i should learn some lie theory
that shit sounds crazy
Yes, SO(3) is diffeomorphic to .
There's a nice way to see it, by saying any rotation is a clockwise rotation around some axis... so rotations are described by points in a ball in 3d...
but a rotation by pi around one axis is the same as a rotation by pi around the axis pointing the opposite direction!
So we take the ball and identify opposite points on its boundary!
yeah thats how i remember it :)
Yes, so that gives .
So that means for some vector space , where the isomorphism is only of manifolds, not of groups.
And you can figure out how big needs to be just be figuring out the dimension of .
Oh, whoops, I lied.
SO(3) is just the rotations. O(3) is the rotations and reflections.
In fact O(3) SO(3) Z/2, as groups and as manifolds.
Anyway, I could ramble on about this stuff all day, since this is the bread and butter of mathematical physics.
I should probably get to work on a paper... but I think it's no surprise to you now when I wrap up and say "n-dimensional real vector bundles over a space can be described using Cech 2-cocycles on that space valued in the sheaf of continuous GL(n)-valued functions".
But we didn't get around (yet) to figuring out when two 2-cocycles give isomorphic bundles! That's the next step. I gotta quit now, but maybe you can think about that, if you want.
i was thinking earlier... the thign i said about seeing the connection to higher sheaves
so in an ordinary sheaf you have a set of sections for each open. in a higher sheaf you have a category of sections for each open
so im seeing how here you have a category of vector bundles over each open
Yes! That sort of "higher sheaf" is called a "stack".
so ive heard o:
and restriction functors would be given by pullback?
Yeah! One of the nice examples of a stack that's not a mere sheaf is the stack of vector bundles (say with some chosen fiber).
but so id heard that "descent" is what you have for stacks instead of the typical gluing condition and it gets hairier
Well, there's "descent" at all levels of hairiness.
and i think i get it—the issue is that you can no longer just require that sections be equal on the overlaps, you have to require that they be isomorphic on the overlaps, but
then you also need to require that the isomorphisms are coherent
Right!
:triumph:
but there was one other thing that occurred to me earlier—
if u have an ordinary sheaf given by continuous functions into some codomain, say
A lot of this stuff can be understood to some extent using Cech cohomology.
u can already upgrade it to some sort of stack, right, by just considering the set of functions as a category by the fact that they naturally have higher structure bc of homotopy
and what youre talkling about in this thread is like—establishign a correspondence between that and the directly-described stack of vector bundles?
I don't know if that's what I'm doing. I don't think it quite is.
But it might turn out to be, in the end.
I think it'll be good if you just figure out a really simple condition for when two choices of (with the same cover) give isomorphic bundles.
hmmmmmmm maybe later >.>
adhd engage
Yeah, later.
Then you'll be able to cook up a groupoid with 's as objects and some other things as isomorphisms.
And people usually just take isomorphism classes and call that "the 2nd Cech cohomology".
But yeah, we may be getting our hands on a stack here, secretly!
Okay, seeya! Gotta keep editing Kenny Courser's thesis.
thanks for the lecture :)
hmm, sorry i havent been around
been off my adderall... :upside_down:
and will be again.......
can you describe a stack as a pseudofunctor O(X) → Cat w/ a condition like... some kind of "turning certain diagrams into lax limits", maybe :eyes:
If denotes the category of pseudonatural transformations and modifications between pseudofunctors, then the condition for to be a stack is that is an equivalence for each covering sieve . Analogous to a sheaf, but one categorical dimension up.
What are some good examples of stacks over a site which are are not gerbes over ?
I think the stack of vector bundles and vector bundle morphisms over a topological space is an example.
Or simply the stack of (small) sheaves and either isomorphisms or all morphisms.
@John Baez @Ulrik Buchholtz Thank you Sir.
@John Baez I understand your point , I think you mean that "Existence of a global section does not ensure Triviality in vector bundles but ensures triviality in -torsors. Hence , local connectedness property of the gerbe holds for stack of -torsors over a space but fails in the case of stack of Vectors bundles over a space. Am I correct ?
I'm not an expert on this stuff, so I don't even remember what the "local connectedness property of a gerbe" is. But it's certainly true that existence of a global section does not ensure triviality in vector bundles but ensures triviality in a -torsor.
@John Baez Let be a stack over a site . Then we say that is locally connected if for each object in and for any , there exist a cover of such that is isomorphic to in for all . While proving this property for the stack of torsors over a space I used the fact that a -torsor is trivial if there exist a global section. So, I thought that the same procedure will not work for the stack of vector bundles over . Though I agree it does not ensure that the stack of vector bundles over is not a gerbe
If we consider two vector bundles over of different ranks, then we won't be able to make them isomorphic by pulling back to a cover.
But if we consider the stack of vector bundles of a fixed rank (and bundle isomorphisms between them) then I think it will be a gerbe. (We could allow to be a locally constant nonnegative-integer-valued function on .)
@Reid Barton But the category of vector bundles over a space is not a groupoid . Since Gerbes are always defined to groupoid valued stacks hence it will not be a gerbe I think.
That's right, that's why I specified that we consider just vector bundle isomorphisms and not all vector bundle maps.
@Reid Barton Ohh!! Sorry! I got it.. Thanks.
In my original remark I specified the stack of vector bundles and all vector bundle morphisms, and I was hoping all those non-invertible morphisms would prevent this stack from being a gerbe. I am a simple man given to simple counterexamples.
But okay, I guess even the stack of vector bundles and vector bundle isomorphisms is not a gerbe.
The stack of rank-n vector bundles is equivalent to the stack of GL(n)-torsors, so yes, that should be a gerbe.
Todd Trimble said:
If denotes the category of pseudonatural transformations and modifications between pseudofunctors, then the condition for to be a stack is that is an equivalence for each covering sieve . Analogous to a sheaf, but one categorical dimension up.
this is actually the only precise definition of the descent condition i remember lol
but i think it also moves some amount of difficulty into bicategory yoneda...
Yeah, for lowly folks like me who have mainly thought about stacks on topological spaces, it's probably some super-efficient way of saying you get an object of when you've got objects on each open set (or whatever) covering , and isomomorphisms between their restrictions to intersections , such that on intersections . And that last thing, that "coherence" law, looks like something you see whenever you replace equations by isomorphisms.
sarahzrf said:
but i think it also moves some amount of difficulty into bicategory yoneda...
The way I look at it, that's the kind of thing you can calculate to your heart's content, if you're motivated enough to pursue it. Bicategorical Yoneda is not after all difficult!
@John Baez Sir, I undersrtand your point. I should have directly said that the Stack of vector bundles over a space X is not a gerbe from the fact that it is not groupoid valued stack. But I was so much into understanding "what local connectedness property actually says about the gerbe" I forgot to check the most elementary one. For example in the case of stack of -torsors over a space, the local connectedness property tells that "Existence of a local sections ensure local triviality in -torsors".
John Baez said:
Yeah, for lowly folks like me who have mainly thought about stacks on topological spaces, it's probably some super-efficient way of saying you get an object of when you've got objects on each open set (or whatever) covering , and isomomorhpisms between their restrictions to intersections , such that on intersections . And that last thing, that "coherence" law, looks like something you see whenever you replace equations by isomorphisms.
this isnt the full condition, is the thing, cuz u need to know about how the object you get is related to the family
You're right.
I was just trying to figure out where the cocycle conditions comes from, if you start with Todd's definition in terms of .
They remind me both of "weak preservation of composition" in the definition of pseudofunctor, and the prism diagram in the definition of pseudonatural transformation, so I'm a bit confused, but also too lazy to straighten it out in my mind.
it's gonna be the latter, because a descent datum is a pseudonatural transformation
Okay, thanks. I used to know this stuff better, I think. I can't even remember what I forgot.
I would phrase local connectivity as say that locally, everything looks the same, and that local non-emptiness is what tells you things are locally trivial. Vector bundles are locally trivial, after all, but as discussed don't locally look the same.
just in case it's of any help to anybody, I'm now onto translating the parts of FGA that are about descent (which is really the vast majority of it...), and I think it's a pretty nice (albeit "Grothendieck-y") reference
(I'm about a third of the way through FGA 3.I : https://latexonline.cc/compile?git=https%3A%2F%2Fgithub.com%2Fthosgood%2Ftranslations&target=_in-progress%2Ffga%2Ffga-3-I.tex&trackId=1605454299350)