#point-set-topology
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AG? RG?
Oh rly
wait UCLA REU apps started?
it's gangbo's program also
Ah. Gangbo is an interesting guy
I believe it's open
David Harold Blackwell Summer Research Institute A collaboration between the UC Berkeley Electrical Engineering and Computer Sciences (EECS) department, the UCLA Math department and the Stanford bioengineering department. Lawrence Berkeley Natโl Lab โ Roy Kaltschmidt, photographer about the program David Harold Blackwell (1919-2010) David Harold...
I applied sometime late march or early april last year lol
Not the best as a professor, but super chill
I would be applying to hopefully work on "Calculus of Variations" I think
He has a thick north african accent
Sounds like the warlords in documentaries
I know it's immature, but I couldn't stop laughing
this seems to be some special program
the usual UCLA REU apps open in march I think
wait thats rutgers lmao
why is it on the ucla sitr
yeah idk I just put everything that seemed vaguely interesting on a big spreadsheet
and am applying to all of them
2 down ^_^
are you applying to chicago
yup
one of my friends went there last year
didn't get in last year but I think my app is stronger now
he said it was fun
yeah it seems really cool
otoh I would like to do something more researchy
but I wouldn't hate u chicago's program either lol
I dont want to do researchy stuff
I'd prefer reading a shit ton and doing an expository paper of some kind
is it usually people at a knowledge level comparable to you all that apply to REUs
this makes me think applying to some is a waste of time
nope
You should apply bacono - they factor in potential and who your letter writers are
there are a couple things to consider
several people in my reu last year had only done like, an intro proofs class
or like linear algebra
they weren't on my project because that project requires more mathematical knoweledge/experience
what was your reu on shamrock?
but similarly I didn't apply to the other projects because I wanted something more advanced
so people self select
which of these do you have knowledge about?
(1) braid groups
(2) braided monoidal categories
(3) operads
(4) hopf algebra
(5) quantum groups
none
oh okay sick
sorry Im not trying to flex or anything
I just like, want to know where to target my explanation
okay so you have knots, yeah?
this is at its heart a knot theory project
knots are not nice algebraically
you can't like, compose two knots
also it's sort of arbitrary to restrict to embeddings of just one circle, so instead lets look at links, which are like knots with multiple components
following so far?
yup
well there is a closely related object which is nice algebraically
braids
idk what the arrows are I stole this from wikipedia
a braid on n strands is like, you fix two sets of n points and then let n disjoint copies of the unit interval connect them
cool i ddin't really look at it lol
(the embeddings are subject to some dumb regularity conditions or whatever so that they're not super wild. just imagine physical strands connecting n points to n more points)
oh nice, so do you compose in the obvious way?
yup!
cool!
here's some examples from wiki
and you can like, twist and untwist
if you think about two strands
crossing them one way and then the other
and stacking those on top of eachother
you can untwist to get the identity
so the inverse is like, reverse all crossings and reverse the ordering
so it's geometrically kind of clear that like, the nth braid groups is generated by the operations of crossing the ith and (i+1)th strand
with some relations that you have to stare at but can convince yourself make sense
so the last one holds for i, j not adjacent
crossing far away strands commutes
and then the first one is a weird kind of twist
also more examples
and here's the braid relation
you just sort of pass the middle strand through
so the second important thing
you can close up a braid to get a link
just connect the top and bottom dots
yeah?
alright so
this is our connection between geometry and algebra
the equivalence relation "closes to the same links" can be described as the reflexive transitive closure of some simple things called markov moves
which I won't go through
but in principle you can determine that like, if you have an invariant of braids you can check that it descends to links
hmm ok
just by checking it's invariant under these three moves
okay so
new perspective
stop caring about knots
care about braids
(and then eventually bring it all back to braids)
we're going to look at systems of representations $B_n \to \mathrm{Aut}(X_n)$
no problem, never did
shamroc$\overline{k}$
lol
alright so
there are two paths
are you a noncommutative algebraist or a category theorist at heart?
uuh
aight lets go cats for now
maybe "representation theorist" instead of noncommutative algebraist
okay cool
that one is a nicer story
even though i personally prefer/worked on the other
so here is an idea
hmm lemme think about how to phrase this
do you know the definition of a monoidal category?
symmetric monoidal?
yup
alright sick, so say $(\mathscr{C}, \otimes)$ is a symmetric monoidal category
shamroc$\overline{k}$
then for any $x \in \mathscr{C}$ we get a sequence of representations $S_n \to \mathrm{Aut}(x^{\otimes n})$
shamroc$\overline{k}$
do you see how this works?
yup
right so this also plays nice with the tensor product of maps
and a certain operation on Sn
which i think of as the direct sum
if you have a permutation in Sn and one in Sm you get one in S_{n+m}
do the first permutation on the first n things you're acting on and the second on the last n
yeah?
yup
this is not a group homomorphism, but it's something for sure
seems to be some kind of "join"
so this system of representations turns "join" into "tensor"
does that make sense?
hmm ok
if you think about the like, n = 4 case
and S2
this is just saying
take two permutations in S2
then we have $x \otimes x \otimes x \otimes x$
shamroc$\overline{k}$
the join will do the first permutation on the first $x \otimes x$ and the second permutation on the second $x \otimes x$
shamroc$\overline{k}$
right so
there's some niceness to this representation
this isn't like, super relevant I think
but I just want to point out we have nice systems of representations
okay so
slogan: braids are permutations with more memory
makes sense
right
just trace the permutation of the dots
and this gives a homomorphism Bn -> Sn
also we have a sort of join on braids too, right?
right
literally just stack them next to one another horizontally
okay so we want a different flavor of monoidal categories
instead of being able to act on tensor products by permutations, we want to act on them by braids
and then permute according to the underlying permutation of the braid
so the definition is what I said, plus some coherence conditions on the isomorphisms
In mathematics, a commutativity constraint
ฮณ
{\displaystyle \gamma }
on a monoidal category
C
{\displaystyle {\mathcal {C}}}
is a choice of isomorphism
ฮณ
A
...
we have an isomorphism $\sigma : A \otimes B \to B \otimes A$
called the "braiding"
shamroc$\overline{k}$
but unlike in the symmetric case, $\sigma^2 \neq id$
shamroc$\overline{k}$
(i mean it can, every symmetric monoidal cat is braided too, but in general this equality fails)
and then you have ugly axioms like the pentagon axiom (edit: but for the braiding)
making sure coherence theorems work
lol
yeah haha
but they ensure that
this one family of isos
gives a system of braid group actions
like, $\sigma$ represents the generator of $B_2$
shamroc$\overline{k}$
the thing where you flip one strand over the other
and then all braids decompose as compositions of braids where you just flip one strand over an adjacent one
and a braid like that is just a trivial braid joined with $\sigma$ joined with another trivial braid
shamroc$\overline{k}$
pictures are useful here lol
if you look at the left braid here, that's $(\sigma \oplus e)(e \oplus \sigma)(\sigma \oplus e)$
shamroc$\overline{k}$
so basically the point is all that matters is this generator $\sigma \in B_2$, all other braids are built up from that, so for a braided monoidal category as long as we have this one braided we can act by the braid groups
shamroc$\overline{k}$
akin to how the single flip AxB -> BxA in a symmetric monoidal cat gives you an action of all the Sn on length n products
okay cool
so in particular this kind of category produces loads of braid group representations
yeah?
pick any object and look at the automorphism groups of its tensor powers
๐
Alright so
How do I even know these things exist?
Like, braided monoidal categories
Well it comes down to that braid relation $(\sigma \oplus e) (e\oplus \sigma) (\sigma \oplus e) = (e\oplus \sigma) (\sigma \oplus e)(e\oplus \sigma)$
shamroc$\overline{k}$
completely unrelated to all of this (in the sense of like, how things developed historically) physicists were interested in solution to the "yang-baxter equation"
these are matrices $R \in \mathrm{End}(V \otimes V)$ such that $(R \otimes I)(I \otimes R)(R \otimes I) = (I \otimes R)(R \otimes I)(I \otimes R)$
shamroc$\overline{k}$
wait a minute...
....
...
those are the same equation!
so people had already come up with these things called quantum groups
hmm
quantum groups (or "quasi-triangular hopf algebras") are certain kinds of hopf algebras $H$ along with a special element $R \in H \otimes_k H$, satisfying axioms which make multiplication by $R$ on $V \otimes_k V$ a solution to the yang-baxter equation for any representation $V$ of $H$
shamroc$\overline{k}$
(the element R satisfies some weird properties that you stare at for a couple days and think really hard about and then realize are a really clever way to state that it gives solutions to the YBE)
so if you have a quasi-triangular hopf algebra, its category of representations is braided monoidal, with braiding $A \otimes_k B \to B \otimes_k A$ given by "multiply by $R$ and then use the usual swap iso $A \otimes_k B \to B \otimes_k A$ in $k-Vect$"
shamroc$\overline{k}$
okay so i feel like I am brushing a lot of details under the rug here
but it's really not useful to talk about what quasi triangular hopf algebras are lol
That's quite a lot
they are things that had already been extensively studied and their category of representations is braided monoidal
is the point
so now we have a pipeline
ok
quasi-triangular hopf algebras -> braided monoidal categories -> braid group representations -?> knot invariants
thats a lot isn't it
but wait
what's that?
you think it's too simple?
not enough category theory for you?
oh I should note at this point, none of this is my work
this is all already known
so here's where the idea for my project starts off
what if instead of regular knots we consider *singular* knots
where we allow self intersections
and these have a notion of "singular braids" analogous to braids, where the strands are allowed to intersect and come apart
so literally just like, let the strands collide
does that make sense?
uuuh sorta
you can still concatenate singular braids
but once you've created a singularity you can never pull it apart
so we no longer have groups, only singular braid monoids
examples of singular knots
monoid presentation of the singular braid monoid
we still have those usual twists si
and their inverses
but now we also have collisions/self intersections/singularities ti
๐
so once again these look scary
but like
most of those are not actually weird
first half is commutativity stuff
"far away things don't matter"
(3) is interesting and geometric, it says you can twist a singular braid to move a crossing above a singularity
hard to show you without a physical model lol
(4) is the braid relation and then two singular versions
this but the top left and bottom right crossings are now singular
you just sort of twist to move it up
(and the mirrored version)
anyways, if we want to find singular knot invariants we might start with singular braid monoid representations
oh but wait! we saw earlier that those naturally come from braided monoidal categories
(oh also thing I forgot earlier: all of the basic knot invariants you'd learn in a first course on knot theory arise from quantum groups/braid group representations in the way I described earlier)
so what's the analogue of a braided monoidal category for the singular braid monoid?
oh well, clearly what we need to answer this question is
O P E R A D S
see, (strict) braided monoidal categories are algebra over the fundamental groupoid of the little 2-disks operas in Cat
(general braided monoidal categories are of course a modified weak version of all of this)
(also that fundamental groupoid is pretty easy to write down explicitly and you don't need to know about the little 2-disks operad or anything, Im just meming)
so the moral is there's a nice operad people already care a lot about
and it somehow parameterizes braided monoidal categories
okay moonbears keep in mind
i had to fucking generalize all of this
like
this was my first week or two of summer
learning ALL OF THIS
and I haven't even stated our goal yet!
okay so back on track
the idea of the project is to find an analogue of the paranthesized braid operad (the thing I mentioned above) for singular braid monoids, so that it's algebras give a notion of singularly braided monoidal categories, then look for the right singular version of a quasi-triangular hopf algebra so we can find explicit singular braid monoid representations/singular knot invariants
it took me like a week to understand what the project was about lmfao
I think you secretly really love LDT sham
lol
well the thing is like
it's an algebra/category theory project for which I can draw pretty pictures
and reason with braids
that's like the perfect thing
abstract nonsense+geometry (actual geometry, not AG)
sorry for the long explanation brofib
but there is a lot of setup required to explain the project lol
lol it was fun listening
ng is also into this stuff
ng?
thing i am thinking of
ah okay
ngroupoid, sorry
Braid relations are interesting
anyways, turns out an operad/notion of singularly braided monoidal category can't exist
They describe dehn twists!
ah just catching up, I was taking a nap 
and I ended up working out some of the hopf algebra generalization stuff
someone asked what my reu was
and I needed to explain this
oh yeah you asked what came of our reserach
here's the talk jonathan gave
paper is still WIP
cool I'll check it out
oh btw, did you end up going to Olivia's talk on this cactus operad stuff?
oh no I missed it!
I think I meant to go there
but forgot
oh also did you see this https://www.ias.edu/math/events/quantum-groups-seminar ?
Likewise. I'm really interested in what she's working on (we had quite a few conversations about this early on while she has been working on this)
oh no I did not see this!
incidentally there are a good handful of quantum groups people at my university ๐
She's super close to the stuff I was doing this summer but also has left the uw lmfao
so
I could've worked on stuff with her maybe
if not for that
sadge

oh right I just remember what I was thinking before brofib's question
"I should get dinner"

Mistakes were made

I think there's a couple of grad students over here who work on quantum groups stuff
I know that my freshman year algebra TA does for sure
I'm taking homological algebra this semester from one of the quantum groups/geometric rep theory people here
excited for that
time to actually learn spectral sequences properly ๐
everyone's doing homological algebra lmao
yeah haha
I use spectral sequences all the time I just
happen to only work with cases where I never have to think about what the differentials are doing
if I have to actually think about what the differentials are doing then uhhh

ah geometers
spectral sequence that immediately degenerates on the E_2 page
haha yea I know how to use spectral sequences
or like spectral sequences but there's only like one column of nontrivial entries ๐
I haven't learned about spectral sequences, they haven't come up for me yet. I'm a very concretely focused mathematician
alright now back to this thing about 2 functors
how did you prove the snake lemma then 
lol you don't need a spectral sequence for that 
(it's a joke)

lmfao
sorry I'm tired as hell
We did it the standard way dude

We watched "It's My Time"
ye im super excited to get better with spectral sequences too
just learned how the adams SS is set up a couple of days ago
aaaa
that's a thing I used to know
what an utterly horrifying thing to try to compute
someday I want to learn how to actually compute things in algebraic K-theory
someday I will learn what algebraic k theory is about
hmm okay it is Tortellini Time
or pigs in a blanket?

Oven is borked

we need to get it fixed
the prof teaching my hom alg class does algebraic k theory
no
Well he kept hearing this rumor
Like at conferences
That Weibel was writing a book on algebraic k theory
Like people asked him how it was going and when it would be finished
and he at no point had intended to write a book on algebraic k theory
But (I assume) felt peer pressured
the fact that K_{2n-1}(Z) has rank 1 for nโฅ3 odd and rank 0 otherwise has something to do with the conjectured transcendence properties of the odd zeta values \zeta(n)
However he felt like before he could do that, he needed to write a book on homological algebra
Since there weren't any good enough ones
And then after that he eventually wrote an algebraic k theory book
Imo a hilarious story
I might get to start reading some algebraic k theory next quarter 
Hype!
nice!
some people might present some of Quillen's foundational stuff in my topology class
oooo
which hopefully should give me the background required
I am hoping my bundles class talks about k theory but it doesn't seem like it will :(
Even after seeing the foundational stuff for like the tenth time I have never walked away from that stuff thinking "great, now I know how to compute this!"
hatcher's book is good
yee, it's just one of those things I don't really have the time for
yea it's stupidly hard 
This was supposed to be a lighter quarter, and yet so far...
my analysis class is very very very stupid
btw Shamrock given your stuff about knot invariants do you know much about the Kontsevich integral of knots?
no, sorry
Ah it's super cool and I've had quite a few project ideas related to it for a while that I probably will never get around to
it's conjecturally a complete knot invariant ๐

:PogChamp:
it's also EXTREMELY related to the whole Drinfeld associators/parenthesized braids/parenthesized chord diagrams picture
yeah I didn't learn the knot theory stuff very well
because I was trying to learn everything else and actually do new stuff lol
Also is extremely related to quantum invariants, you can read every quantum knot invariant off the Kontsevich integral if you set things up carefully
ooh
(in fact you can read literally any Vassiliev invariant off the Kontsevich integral, which is related to the whole singular knots picture)
Yeah, interesting
also related, Jonathan is many things but he is not a knot theorist
Which I mean, he was very open about in our project
I'm sad he deleted his twitter ๐ฆ
So if I had to ask knot theory questions I would have to go to another mentor
Yeah
I mean I have him on facebook and I get why he deleted twitter
but I miss having him around there

I should hopefully be meeting to talk about simplicial stuff and dold kan
In the near future
nice 
oh lol this reminds me, we had to define the notion of a natural transformation for our grad student mentor
Who was great at knot theory/low dim top
but uh, that made things awkward considering how categorical our project was
Ooo thanks! Will I need to understand perfectoid stuff for the scholze?
The biggest thing to understand right now is condensed mathematics
This is how Scholze sidesteps some of the foundational issues trying to correctly define the derived category of the moduli of G-bundles on the Fargues Fontaine curve
Perfectoid space stuff is very necessary yes, as is the more general notion of diamonds
It seems like the main technical inputs are like
etale cohomology of perfectoid spaces and diamonds and Artin stacks in the sense of diamonds
The Fargues-Fontaine curve and the moduli of G-bundles on the Fargues-Fontaine curve, and the geometrization of p-adic Hodge theory
condensed mathematics, especially solid modules
(Condensed mathematics has a lot of appeal that is independent of all of this and is probably the easiest of these three items to learn: for instance condensed sets are in a lot of ways preferable to working with topological spaces)
"Indeed, unlike in classical topologies such as the Zariski or ยดetale topology, sheaves on the pro-ยดetale
site of a point are not merely sets. What seemed like a bug of the pro-ยดetale site is actually a feature
for us here, as Clausen explained to the lecturer."
I already want to die haha
They are a little funny to set up
The point is that they give you more or less the correct framework for doing algebra in a topological setting
E.g. the category of topological Abelian groups or the subcategory of locally compact Abelian groups are very poorly behaved and arenโt well suited for homological algebra and other categorical constructions
Condensed Abelian groups form a much nicer category that faithfully includes the classical picture
"If S is a profinite set, then all cohomology
groups vanish for i > 0, and H0
sheaf(S, Z) are the continuous maps S โ Z, while H0
sing(S, Z) are all
maps S โ Z"
scratches head Well there's nothing left to study...
"Mumford writes in Curves and their Jacobians: โ[Algebraic geometry] seems to have acquired
the reputation of being esoteric, exclusive, and very abstract, with adherents who are secretly
plotting to take over all the rest of mathematics. In one respect this last point is accurate.โ
For some reason, this secret plot has so far stopped short of taking over analysis. The goal
of this course is to launch a new attack, turning functional analysis into a branch of commutative
algebra, and various types of analytic geometry (like manifolds) into algebraic geometry. Whether
this will make these subjects equally esoteric will be left to the readerโs judgement."
-Scholze
@honest narwhal Looks like we can merge a few channels 
@cedar pebble do you work on the langlands or geometric langlands?
Just classical Langlands stuff for number fields
Oh right. Need someone I can discuss the new stuff with.
The Arinkin et al paper is a lot more familiar in its language. I can read this paper at least.
Clausen and Scholze... I don't know if I can handle it
Have you read Arinkin et al?
my Prof said this holds if phi is diffeo
and thus we can have a notion of 'pullback of a vector field'
here omega is a vector field
how can this be true?i'm a bit confused
Denoting a vector field by omega is some sicko stuff, but other than that, this seems gรผd I believe
but how can we pullback vector fields
i thought we can only pullback forms
prof said its crucial that phi is diffeo
but i cant see why would that give a pullback of a vector field
think about why pullback for vector fields doesn't make sense usually and then think about what a diffeo is
Yes, it's very important that you have a smooth inverse map
Philosophically, this is fine, because if you have a diffeomorphism between two manifolds, this basically means that the two manifolds and their respective smooth structures are "the same", so everything you can do on one manifold you should be able to do on the other
so if I had a diffeomorphism could I push forward forms too?
And, I mean, your screenshot from up there is just a definition, anyway, right? So there's nothing to check in terms of "whether it's true or not"
similarly?
I'd say so, ye
well
think about why the pullback of a vector field isn't well defined to begin with
then you can see why you need a diffeo
ye that sounds like a healthy exercise
my problem is i've never seen/heard this
i only heard definition of pullback for forms
i can't imagine what would change if i try to do it for vector fields
like it's not even defined
Yeah you never talk about this because the pullback of forms and the pushforward of vector fields are the only canonical operations; i.e. they are the only ones which are always okay to do
no that thing you posted was your definition
see what happens when you remove the condition that phi is a diffeo
then it's not invertible
and i can't go to RHS
yes well what happens if \phi issn't injective
you could get multiple vector fields on your domain manifold for the same point
and if it isn't surjective then you don't even have a pullback for at least one point in the target
yes,makes sense
and so the map has to be smooth and bijective for the pullback of vector fields to be well defined
which means it needs to be a diffeo
@tough imp am I just dreaming or were there notes for the stacks course that were much longer than the current version?
Can someone explain why the highlighted part is true?
Isnโt it precisely what it says in the formula
If you discard the christoffel part
?
TTerra
Thanks that makes sense!
Yeah they used to be longer
For pullback of vector fields itโs only necessary for F to be a local diffeomorphism, if I am not wrong? So neither injectivity nor surjectivity are strictly required
To pull back vector fields it's enough to have a local diffeomorphism
is someone familiar with rep theory
im missing a crucial point
this
so my main trial is that i have SU(2) and SO(3) as groups, I try to do rep of this by using their lie algebras,which are isomorphic,i.e. su(2) iso so(3). I know how to do rep theory for so(3) now I can use the fact that the rep from the lie algebra level can be lifted to the covering lie group ( I can't prove this so help would be appreciated)
but unfortunately the covering lie group is SU(2) not SO(3) and I would need to make the transition
what is the representation D^(j) here?
okay sure SU(2) is simply connected so representations of su(2) lift to representations of SU(2) like this
if you have half integer spin then D^(j)(2ฯ) is minus the identity
so this can't form a representation of SO(3): rotation through an angle 2ฯ has to be sent to the identity
you still get a projective representation in this way
I mean you're forced to map the identity to the identity in such a representation
half integer spin would be forcing you to map minus the identity to the identity, which you can't do unless you pass to the corresponding projective representation
@cedar pebble Oh, scholze has a really nice lecture series on condensed maths on youtube. Though at 20 hours... it could not be said to be condensed. ๐
20 hours is just under a day, get watching
you can do them all in a sitting with a coffee or two!
yea it's a good lecture series!
You are trying to scramble my brain, TTera ๐ฎ
Maybe if I leave it on when I go to bed, his soothing german accent can lull me to sleep and then I can learn by osmosis and have downloaded everything when I wake up? 
Oh, he basically covers basic AG at the start. Perhaps people could watch this and skip hartshorne in future? 
If people can skip Hartshorne by watching only a few hours of Scholze I will destroy the video as I annoy handle others spending < hundreds of hours on Hartshorne and learning AG
annoy handle
(they can't, they are totally orthogonal topics)
I think going through the standard grad books/courses is good to give a broad and deep understanding where a lot of things come from
But in research you can kinda just pick a branch in a tree to jump up to
And hope the branch will support you
Without going up the trunk and exploring branches that will support you
I say this with some degree of cheek. After spending all the time on grad studies, it's easy to watch a category theory explanation of something and go, "this is so clear and concise, why wasn't it explained like that the first time?". But back in my grad student days, an explanation with "left adjoint" and "right derived functor" would have been opaque.
To leanr Algebraic topolgoy what pre-reps are required?
is it just Point-Set and Group Theory?
is there anything else?
yeah basically, but knowing more algebra will make it easier
@tough imp did you actually do most of Hartshorne's exercises
I've done exactly 1/2 of the ones from chapters II and III
That is impressive
What else besides GT in algebra is good to know?
sanity check
Let $E, F$ be vector bundles. Do we have $E^* \otimes F^* \cong (E \otimes F)^*$?
shamroc$\overline{k}$
Pretty sure this is true...
You have a natural iso of this kind for vector spaces, right? So just apply that on fibers
also do we have an adjunction of the tensor/hom bundles? Feels like we should since they're all defined fiberwise...
Define globally check locally
ยฏ_(ใ)_/ยฏ
For locally free sheaves I found the hardest part is figuring out the way to define it globally and once you can do that you go local and it's just a linear algebra statement that's obvious
yeah I think I see how you can do this
It's like
Define the map on fibers
via the result for fd vector spaces
Then by naturality, the local coordinate representation should just be the thing applied to that local coordinate representation
idk lol
Still do not see this isomorphism of bundles...
Ugh I hate this problem it feels like there's some really beautiful geometry that I'm just not seeing
Maybe I need to read about symplectic stuff
alright so
if I have an oriented real bundle $E$ over a paracompact $X$ of rank $2$
shamroc$\overline{k}$
There's a way to find a complex line bundle $E'$ on $X$ whose underlying real bundle is $E$
shamroc$\overline{k}$
I see how to construct it, but it's bad and doesn't seem at all canonical
by Gram Schmidt you can cover by oriented orthonormal frames
Then transition functions land in SO(2) โ U(1) <= GL(1, C)
Why is Mayโs book bad @cedar pebble?
hello tolaria
Hi
Yeah this confuses me
Like
The complex multiplication depends on the choice of frame, eight?
*right
Ooh maybe orientedness saves us here....
Right okay you can like, scale and rotate
Rotation is well defined independent of basis
right??
You're given an orientation of each fiber
which is an equivalence class of bases
the complex multiplication you define will not depend on the choice of rep from that equivalence class
and then the fact that all the transitions are in GL+ ensure that whatever you defined on trivilaizing open sets will be compatible on intersections
all the choices are made for you when you assume the bundle is oriented
I think
Right, this is my thinking too
the orientation on each fiber gives us a way to rotate vectors without a choice of basis
and so you can define complex multiplication
I think the extra confusion I was having is that Lee chooses a fiber metric and says all the transitions lie in SO(2)
and then SO(2) is the circle
But adding the fiber metric is actually adding even more apparent noncanonicity
When really there's a high level description of the complex bundle
alright so what I believe is
hmm
hmmmmm
I'm no longer certain this works
Orientability gives us that all the stuff has positive determinant, sure
But rotations do actually preserve distance, which is not invariant...
so I think maybe you do need to start with an oriented bundle which has a metric on it
Ugh maybe this isn't true? I'm no longer sure
ooh but my actual problem involves looking at this for S^2 = CP^1
Where I have a very nice metric (round metric or fubini study, pretty sure these are the same?)
Okay yes so I still need some noncanonical choice of fiber metric I think
But given that and an orientation you get a complex multiplication
aha, so I think this is actually really intuitive for the sphere
rotation is given by the right hand rule
With axis the normal vector
Any ideas on how to do part b
hm if we have f: X -> Y, g: Y -> X a htpy equivalence, A subset X, B subset Y, and f | A: A -> B, g | B: B -> A
is f | A, g | B a htyp equiv from A to B
mhm yea pretty sure thats true
Don't you need something like thy homotopy extension property?
yeah moth what about like, X = R^2, Y = pt, A = S^1, B = pt
f squashes everything to a point and g includes the pt into the circle
@fading vale
yea ur right
in this context it was fibers so it works out
but def not in general lol
otherwise everything would be htpyically trivial by embedding into its cone
ugh this construction is really confusing
the section about homotopies in Top^K or Top_B being normal homotopies with H_t morphisms
tammo tom dieck
the H_t morphisms bit makes sense when im thinking about homotopies between maps f, g : X -> Y
say with i : K -> X, j : K -> Y
but when i try to think about it in the context of homotopy equivalences it starts being pretty confusing to me
like if i have f: X -> Y, g : Y -> X we need fg simeq id_X and gf simeq id_Y
but i dont understand how the homotopy from fg to id_X works because i dont get what spaces under the K H_t between them are supposed to be morphisms between
sigh
like the problem im having makes sense right
cuz we have fg: X -> X, gf : Y -> Y, ok sure
where does the K come in though?
i guess fg is a morphism from i : K -> X to itself and likewise the identity so is that what the point is here??
that kind of makes it work out because when verifying the deformation retract stuff you would get H_t(k) = H_t(i(k')) = i(k') = k so the htpy is rel K...
Any ideas for part b
Can you imbed a bouquet of 3 circles in a torus?
yes
arrows are the circles, (identify opposite sides of a square to get a torus as usual)
Can you find a curve on the torus such that if you cut the torus along that curve you end up with two manifolds whose connect sum is the torus?
nice cup
the only way two manifolds have connect sum to be the torus is if one of them in a torus and the other is a sphere
this is a corollary of the classification of surfaces
without using the classification of surfaces
C'mon
You're ruining the fun
Try drawing a curve
why does it always fail?
but the torus is a curve moonbears
this post was made by the complex geometry gang
that was pure genus
fjdka;
Yeah, can you prove it for all ways that you can draw a disk?
I mean draw a simple closed curve?
BOO
?
You can start by trying to draw curves
and see what it property it violates
There's only a few ways you can draw curves
Up to isotopy
well yeah, they're all in the same homology class as one of the standard generators or contractible
So lame
lame because I used the word homology class?
yA
yA
Proofs using homology is better because then youโre using algebra
i hate algebra
it's okay, lots of mathematicians live a full life while hating algebra
being wrong is not a crime
Are single points 0-dimensional submanifolds of R? e.g. take the set {-1,1}, it's the image of phi: {-1,1}->R, phi(x)=x. If phi is an embedding then {-1,1} is a submanifold...is phi an embedding?
yes.
Ok, thank you! Is that because phi: {-1,1}->phi({-1,1}) is a homeomorphism? I'm trying to sort out all of the terms
And there should be a diffeomorphism such that {-1,1} map to a point on the axis, in this case one needs two diffeomorphisms, one for each point? Or is there a way to define single diffeo that fits the definition
I think it would be useful if you shared your understanding/definition of what an embedding and a manifold are
@sleek thicket did you ever work out the 2-category meme ๐ฐ
hoping to get it finished over the weekend

twitter voted 26 to 25 so I have to now
oh nice
I can post here or smth, will probably put it up on my website
actually I have an AG-related bundles question you might be able to help with, but I think @hazy stratus was asking a question
We defined a manifold by 3 different characterizations, I was trying to match {-1,1} being a manifold to two of them
(sorry for the late answer)
So the first one was that M is a manifold if all points in M have an open neighborhood V s.t V is the image of an embedding
An embedding being an injective immersion that's also a homeo
is a manifold an abstract topological space for you or a certain kind of subset of R^n for some n?
That was this
Oh hm
From what you're saying I'm assuming M is a priori contained in R^n
It doesn't have to be n dimensional though
well my n there could be anything
I'm not saying n = dim M
just that it sits inside some euclidean space
Oh I meant it does't have to have the "full" dimension
Yeah the thing about the derivative having to be continuous as well isn't really intuitive to me
That it has to be differentiable, sure
have you seen the example with corners of a square?
err wait sorry that's for why we require immersion
I was thinking about derivatives not having to vanish, sorry
you can find a C^1 function R -> R^2 whose image is square (so not "smooth"), but its derivative must vanish
Ah yeah that was one of the 3 definitions we had
That one I haven't understood entirely though
Why does the image have to be square?
nah this is just an example of how things can go badly if you weaken the definition
if we don't require that there's an immersion (just that there's a C^1 map which is a homeomorphism onto the image) then a square is a manifold too, which is intuitively bad
since it has sharp corners
I'm trying to think of a convincing reason for why we don't want all differentiable maps
at a high level, discontinuous derivatives can be really weird and bad
but it would be nice to say something more concrete
Because the derivative on the corners isn't well defined?
sort of, yeah. Manifolds should look like smooth curves or surfaces or whatever
Like the derivative of abs in 0
but by making the derivative of your parameterization go to 0 as you approach the corner you can still get a C^1 map
think about like, moving along the top of the square
and slowing down as you approach the corner
slower and slower
so that your velocity reaches 0 when you hit the corner
then you turn around and speed up from there
we can ensure that the derivative does actually exist
since it's 0 as you approach from both sides
but we've created a corner
Is there a contradiction there?
no, sorry. I don't think I'm explaining this well
your definition includes that the parameterization be an immersion
yeah?
Yep
I'm trying to provide intuition for why we want that (ie, why we want to make sure the derivative is nonzero)
In fact
because you can have a smooth parameterization of a curve which doesn't look smooth
also I think my reason for why manifolds should have C^1 parameterizations is so that we can use the inverse/implicit function theorems. these are like the most important tools in smooth manifold theory
in fact I bet if you post your definitions then the IFT's will be how you go between them
Right, I was trying to get a diffeo from half of a circle to an interval and tried to check if it would work by calculating the jacobian
By the IFT, the function is only invertible if the jacobian is invertible if I'm not wrong
Much thanks for the intuition๐
oh yeah okay I had a question so
I am trying to understand the twisting sheaf
just in the simplest case
so we have $X = \mathbb{P}^1_\C$
shamroc$\overline{k}$
we can defined this as $X = \mathrm{Proj} \C[x,y]$
shamroc$\overline{k}$
we can cover by two "distinguished opens" $D(x), D(y)$, both of which look like $\mathbb{A}^1_\C$
shamroc$\overline{k}$
with coordinate y/x on the first and x/y on the second
so we can define the twisting sheaf on this base
$\mathcal{F} = \mathcal{O}(1)$ is defined by $\mathcal{F}(D(x)) = (S_x)_1$ and $\mathcal{F}(D(y)) = (S_y)_1$
shamroc$\overline{k}$
does this seem right?
we're basically like
hmm
so what would this look like if I were actually interested in bundles on the manifold CP^1 lol
$C^\infty(\C\mathbb{P}^1)$ is some weird ring
is it graded? probably not lol!
shamroc$\overline{k}$
so we have an injection into smooth functions on C^2{0}
as the homogeneous ones
err no
not homogeneous, just invariant under scaling
it might be easier to try to visualize O(-1) first
well yeah O(-1) is what I actually care about
it's the tautological bundle
I'm trying to understand why
so like, my understanding is that in the algebraic case we the tautological bundle equals O(-1)
I'm trying to figure out if we can make sense of O(n) in the smooth case
via a twisting kind of definition
you mean you want to try do define it in terms of graded modules?
Right
I could define O(-n) as the nth tensor power of the tautological bundle
and then O(n) as the dual of O(-n)
but I want to understand the global sections of these bundles/what happens when you tensor them with another bundle
so that's not really giving me anything new
you can define it explicitly in terms of transition functions
aren't half of those global sections empty
is this different from defining it in terms of the tautological bundle @tight agate?
and also zef im working on a smooth manifold
the global sections capture all of the data of the sheaf
idk how different do you want it to be, but it isnt just 'take tensor powers'
I guess I don't see what transition functions you're thinking of
I mean define it to be trivial over each of the standard opens
and then for the m'th twisting sheaf, the transitions are given by something like (x_j/x_i)^m
hmm okay I think I see what you mean
this thing I said earlier
but in the smooth case
that might work
I havent really thought about the smooth case so idk
I guess what I want to do is understand $\Gamma(E \otimes_{\C} L)$ in terms of $\Gamma(E)$ for a complex vector bundle $E$
shamroc$\overline{k}$
where L is the tautological line bundle on CP^1
and I thought thinking of it as the twisting sheaf might help me do that
but if you use the transition function definition for the holomorphic case, then the fact that O(-1) and the tautological bundle are the same is pretty straightforward to derive
hm okay
another way to identify O(-1) and the tautological bundle is using blow-ups
i will take it one AG concept I barely understand at a time
Btw you can also define (if I recall correctly) O(m) as the quotient $\frac{(\mathbb{C}^{n+1} - {0})\times \mathbb{C}}{\mathbb{C}^*}$
Where C* act on the first n+1 components via multiplication for t and on the last via multiplication for t^m
alehmannbis
This makes it sort of easier to see how the section should work
mildly related to that construction: the complement of the zero section of O(-1) can be identified with C^n - {0}
on P^n
ye it's also an exercise in huybrechts
So an exercise has asked to show the skew-symmetric part $$S_{ij}=\frac{\partial T_i}{\partial Z^j}-\frac{\partial T_j}{\partial Z
^i}$$ of the variant $\frac{\partial Ti}{\partial Z^j}$ is a tensor. Transforming, we get
$$S_{i'j'}=S_{ij}J^i_{i'}J^j_{j'}+T_i\frac{\partial^2 Z^i}{\partial Z^{i'} \partial Z^{j'}}-T_j\frac{\partial^2 Z^j}{\partial Z^{i'}\partial Z^{j'}}$$
But i am not exactly sure what the problem is asking me. Is it asking me to show the first part in the above pde transforms tensorically?
Zero0
Might be a silly question but what would be the symmetry group of a parallelapiped in R3 with L=/=W=/=H
in R2 i know you can rotate by 180
and by 0 of course, so im guessing in R2 itd be order2
ooooo right right Ty @chrome dew
yup you're welcome
Any examples of topological spaces that naturally arise in some fields of math but are not Hausdorff?
Or being even more strict, any examples of important topological spaces that do not attend any separabiliy axioms nor countability axioms?
The zariski topology on an affine scheme is usually not even T1
It only satisfies the incredibly weak T0 axiom, in fact schemes exist where the closure of a single point is the entire scheme
That's some crazy stuff, man, I really need to study some algebraic geometry.
There's some interesting stuff going on.
I wonder why this is so.
Anyway, any easy examples of algebraic or projective varieties with these properties?
I've never studied about schemes yet
But I think that it is somehow a generalization of the usual algebraic sets and projective varieties.
There are schemes without closed points too
What is an example of non-path conected space?
your favorite non-connected space
geometrically, What means the fundamental group is trival?
Hi folks - I'm trying currently to construct an orientable 3-manifold (probably with torus boundary components) with the same fundamental group as the Klein bottle.
i.e. the Klein bottle cross the interval is no good
Is there a way using the orientable double cover maybe?
if you're interested here's a bunch of connected spaces that are not path connected https://topology.jdabbs.com/theorems/T000040
thanks
<@&286206848099549185> sorry for the ping but could use a hand with this one
@wicked trout
nvm this is wrong in general
this seems to prove its still not possible tho
@marsh forge thats a v interesting result u have there
basically im looking at (generalized) Heegaard diagrams for 3-manifolds with Baumslag-Solitar fundamental groups
so if you take a genus 2 surface and draw a curve representing the element bab^{-1}a that defines a manifold w the fundamental group of the Klein bottle
but i want to identify what it is so im going backwards
trying to take the Klein bottle and do something to it to make it an orientable 3-manifold
im thinking maybe a twisted line bundle??? who knows
How about this: The klien bottle is a fiber bundle of a circle over a circle, given as the mapping torus of the orientation reversing diffeomorphism of a circle. Instead, realize it as a bundle over a mobius strip
so, itd be the mapping tours of the diffeo S1xR reversing both the S1 factor and the R factor. Since it reverses both, it should preserve the volume form on S1xR, and thus be orientable
more concretely, it'd be $[0,1] \times \mathbb{C}^*, (0,z) \sim (1,z^{-1})$
eeliot
I think that should work?
@tacit stratus that sounds like what i was going for!! ill look over it tomorrow:) thanks!!
Hey guys, can someone help me with this exercise?
I was able to prove the first implication, but I donโt know how to use the compact and ENR hypothesis
Here ENR spaces are the ones such that there exists $r:V\to Y$ where V is a neighborhood of Y
pmorelli
The book which Iโm studying assume V and Y as subsets of R^n on the def of ENR. I donโt know if this would help on the solution
I am a little confused as to why a closed subspace of a complete metric space must be complete.
My understanding is the counter-example below is wrong based on the above, but I am having a hard time understanding why.
Lets say we have a metric space A {x in R: 0 <= x <= 5}
and a subspace B {x in Q: 0 <= x <= 5}
In my mind, B is closed, but it has a Cauchy sequence that converges to pi, which is in A but not in B.
Our book's definition of complete space is: every Cauchy sequence in a metric space X converges.
I don't see how the A/B example would break that. A sequence in B (subspace of A) might not converge to a value in B, but it does to one in A. B would not be complete as it doesn't have Pi.
ahh tyvm
np
@crimson imp i would think this has something to do with the compact-open topology?
This site is all about giving examples of topological spaces satisfying certain properties?
I've never even heard of that book before.
Is there something similar to other fields of math?
Like
for analysis, as well
A site which gives lots of counterxamples to stuff concerning manifolds?
if you find one, let me know 
Well
In fact
A while ago I've found this site here
The manifold atlas project
Take a look at it, idk how much of a use it would have to me at the moment.
So that's why I asked you if you had any other references.
only the copy of lee on my desk
I don't know, the only thing I manage to prove, which is a consequence of triangle inequality is that d(f(x),g(x))โคn\epsilon
This n may depend on epsilon, I'm trying to use compacity argument to prove that it doesn't, but I don't know where this would take me
Does chirstofel's symbol transform tensorically under linear transformation? I got this does and just making sure
no, i don't think they do. here's an excerpt from lee's riemannian manifolds book
if i'm misunderstanding what you mean by "transform tensorically" lemme know
i just have a hunch this is what you're looking for 
if by linear transformation he means A has constant entries, then its derivative is 0 and so you don't have that second term, so it would transform as a tensor

ya that merosity
๐
haha
and what is that book TTerra
i dont think there is a word 'tensorically' i just made tht up ๐คฃ
well u get the idea
is there an intuitive reason for why this was defined like this? 
it seems reasonable that the result is a k+l form but I can't really picture this
maybe bad answer: because then dx^1 wedge ... wedge dx^n is the volume form (up to a scalar multiple)
although i wouldn't be surprised if that's not a bad answer, since a lot of things relating to DG seem to be defined just for the sake of getting a certain property lol
that's just something i pulled out my ass on the spot, btw 
good question
I hope there's more to it than that, but I do agree that thinking of it in the context of elementary forms is easier
there might be some stupid algebraic way to look at the wedge product that characterizes it as something that's completely natural to consider, idk
damn there's a stackexchange post for everything
this could be helpful or not, or useful or not, but I always go back to the idea that forms are merely alternating tensors of covariant rank, and in the same way we have the tensor products to make higher order tensors, we want an alternating (or antisymmetric) product to make higher order alternating covariant tensors. the wedge product should be the antisymmetrization of the tensor product.
god fucking fuck of course there's a goddamn algebraic natural isomorphism bs to it 
fking algebraists
i do like the "wedge product is the antisymmetrization of the tensor product" that craft suggested
since it's just Alt(phi tensor omega), ya?
maybe you can show that as an exercise, ~circle 
(maybe, up to a scalar multiple, though)
yeah so in warner they construct the exterior algebra as equivalence classes of covariant tensors modulo the ideal generated by stuff of the form (v tensor v), the stuff that definitely needs to be trivial in the exterior algebra. from here, you can just say that the wedge product of two forms, or two equivalence classes, is just the equivalence class of the tensor product of any pair of representative samples from each of the two original equiv classes
(not to imply that warner's construction is unique, just I like that reference in particular...)
That makes sense, ty!
warner 
Just to clarify about the argument that uses
$$\bigwedge^k V^* \equiv \qty(\bigwedge^k V)^*$$
it identifies the two vector spaces via the isomorphism $$\phi_1\wedge \phi_2\wedge...\wedge \phi_k \mapsto \qty(v_1\wedge v_2\wedge ... \wedge v_k \mapsto \det(\phi_i(v_j)))$$
So the wedge product of forms is equivalent to sortof just concatenating them into the matrix?
~S^1
So I remember doing this exercise in an algebraic topology book once but I can't find the reference
so I'm crowdsourcing it
As I recall there was some construction of a ring associated to a topological space that preserved all the information of the space. I think up to homeomorphism but maybe up to homotopy
the point of the exercise was that certain algebraic constructions for topological spaces are too fine-grained. If you recover all the information then these things are like impossible to compute and don't allow you to solve any problems easier
but I can't remember the book or the construction
Maybe the fundamental infinity groupoid?
i know what you are talking about
@obtuse meteor you are talking about this, right?
this is from page 13 of rotman's intro to AT
npnp
The same is true for smooth manifolds, btw
Taking the ring of smooth functions is a full and faithful functor
and actually if you think of the manifold as a locally ringed space, the (co?)unit M -> Spec C^infty(M) of the spec/global functions adjunction is a topological embedding
and when M is compact (iirc?) the image is exactly the maximal ideals
Isn't there also an equivalence with C^infty modules and bundles over the manifold or similar?
please remove your category theory from my calculus spaces 
Oh yeah it was Serre-Swan
that theorem is also the starting point of Top K-Theory -> Alg K-Theory
@sleek thicket yeah I'm familiar with this idea. It's very nice !!!
Cohomologay
oh hey my name thing actually works
i tried it earlier and it didn't lmao
and yeah I think it's sweet!
I hate your name thing tbh
I want to be able to mention you without texit going "brrrrrrrrrrrrrrrrrrrrrrrrrrrrrr LaTeX"
Hello everyone could someone spare 2 mins to help my dumb ass with a question thats probs very easy for you to spot the answer to
Do i send it here? Its not exactly related to topology, although i wish i knew more about thee subject to be able to oost questions here about that
My question was about this equality
And if it would hold true from -inf to 0
Instead of 0 to inf
hmm
IDK where the best place to ask this would be
problably #multivariable-calculus or #calculus
This equality seems to come from integration by parts + gaussian integral. It will definitely hold from -inf to 0 because the functions are even, aka f(x) = f(-x)
topology/geometry isn't closely related to this question :)
so let's move to #calculus
Sorry to ask this but would you mind helping me understand cause in my head it seems like in 0 to inf u sub in inf first and thrn 0 which woukd =0
But for -inf to 0 ud sub 0 first which =0 and then -inf
And since when u sub in its [sub a] - [sub b]
Wouldnt thr result be muktiolied by -1?
we try not to clog up these channels with this stuff :)
it's no problem!



