#point-set-topology
1 messages · Page 268 of 1
and then i want to think about the complement of V'
since it's an open set, the complement is a closed set
hmm
hm
i don't know of that helps
oh
you get neighborhoods of each
ok
so i have x, and i have cl V
and i get U'' around x, and V' around cl V
right?
this is easier to see if you draw it
yes
it's like we have a point and a blob, there are circles around both, and if you look at everything outside the circle around the blob, that includes everything inside the circle around the point.
(as well as everything outside both circles)
alright but V' complement is closed
right
and we have a subset of a closed set
so what can you say about the closure of that subset?
yep!
if you have A inside B, and B is closed, then closure(A) is also inside B.
so now we can boost this to saying closure(U'') is inside V' complement.
(if you want to think about this intuitively: we have 2 disjoint open sets, and if i take the closure of one of them, it can't contain points from the other. if it did, then whatever point we added couldn't have possibly been in the interior of its open set)
right, but this doesn't prove the result unless we can show cl U subset cl U''?
Are two arbitrary simply connected spaces not always homotopy equivalent?
Like am I just dumb
don't you just need to show that there are some open neighborhoods where this is true?
it doesn't matter if it's true for U
maybe im misreading the question

ok if thats the case then I solved this yesterday i think
"we can find a pair of open neighborhoods U and V"
you just need to find 2 neighborhoods
they don't have to be the ones you get from regularity or whatever
i mean
idk
like
i figured it was those sets
this could very easily not be true for certain pairs of open neighborhoods
(for example, (-1, 0) and (0, 1) in R)
well that's good
are they connected too?
okay well this still was helpful thx ryc
also like, it's not true anyway
S^2 and S^3 are not homotopy equivalent
but they are both simply connected
Simply connected yes
pretty sure simply connected does not preclude connected
i mean
maybe it does
i've never seen that as part of the definition, just "every path contracts to a point"
Topologists name thing well challenge
I mean path connected implies connected right
sure, but just because every path contracts to a point doesn't mean any two points are connected to a path
Oh right yeah
also what i mean to say is every loop contracts to a point
No I see
anyway S^2 and S^3 are a counterexample to what you say (why are these homotopy inequivalent? i don't think there's an easy way to see it besides computing homology)
So any two simply connected spaces with the same number of path components should he homotply equivalent
no
Or wait I'm dumb
it's just not true
Actually just stupid
i mean it's easy to think this
once you realize it's not true though
it starts to make the whole higher homotopy thing sound a lot less silly
S^n is just the obvious counterexample
it's definitely not obvious that S^n and S^m are not homotopy equivalent unless you've done some work
you can't visualize S^3? 
it's just R^3 but every direction takes you to the same point at infinity...
anyway this doesn't tell me why they're homotopy inequivalent
i can only see it by thinking about how spheres contract to a point on S^3
but not always on S^2
sorry i mean S^2s
like
you can kind of convince yourself that pi_2(S^3) = 0
wat
the point is that S^2s dont contract on S^2
so pi_2(S^2) != pi_2(S^3)
this is something you can see sort of
if you have the right picture of S^3 in mind
yeah
ok for S^3
pick a point not on the S^2
that you've embedded
and then stereographically project to R^3 about that point
and now contract the S^2 to the origin
and undo the projection
that's how you see pi_2(S^3) = 0
it's still a 2-sphere

how is a loop contractible?
i don't mean contractible as a topological space
i mean homotopic to 0

clearly because no one is reading this shit
it's fine
this is not true

unless regular means regular hausdorf
Yes
ok then its true
xd
but fuck ur definition of regular
Regular usually includes T_1
If you don't include T_1 then you don't get T_(n+1) stronger than T_n
definitions are not supposed to make sense
Did they say call a point and a set disjoint 
also imagine having closed points
Sounds like a cope ngl
u get what he means Moldi 
nooooooooo my primes are points and must be closed 

just finished the assignment tho 😎
My book is defining totally disconnected groups to be groups who have a neighborhood basis of open subgroups around the identity. I cannot figure out how this is equivalent to the usual definition (no nontrivial connected sets). any hints?
Any feedback on this proof?
Open subgroups are closed too, so you have a neighbourhood basis of clopens. By taking all translates you get a basis of clopens. This along with Hausdorff gives the standard definition (without hausdorff the above definition allows the indiscrete topology to be totally disconnected I think?)
Replace hausdorff with T_1
Right makes sense (yeah its assumed all groups are haussdorf, which is equivalent to T_1 for groups)
what about the converse? thats what i was stuck thinking about
@coral pivot so you want no nontrivial connected sets => basis of open subgroups around the identity?
yeah
confused on the definition of f. d is a function from X^2 to R, since it is a metric. how are you taking in a subset of X as an argument of d?
A is fixed
$f(x)=d(x,A)$ relates the distance of the point $x$ to the set $A$. So $d(x,A)=inf(d(x,a)|a\in A)$.
SelahW
And yes, A is fixed
yea no i got that. is there really no problem with just writing d(x, A) and d(x,y)?? i feel like it should be d’(x,A) or something
since this is measuring distance from a point to a set
should be notated differently imo, but ig that’s just me
It doesn't matter because the arguments disambiguate it anyway
ehhhh gross
like, if i were a computer, and i had two local variables named d, i would be confused.
You should probably say that the inverse triangle inequality is happening in R rather than in X
Good thing you aren't 
And not really, overloading is a thing programming languages have too
So replace $x,y$ with $a,b\in\mathbb{R}$?
SelahW
For thm. 1
The variable names are fine, but just add the in R part
Ah okay
If
\begin{tikzcd}
X
\arrow[r, shift left=1, "f"] \arrow[r, swap, shift right=1, "g"]
& Y
\arrow[r, "h"] & Q
\end{tikzcd}
is a coequalizer and $f, g$ are open surjections, why must $h$ also be an open surjection?
It's somehow supposed to be obvious, but it's really not 🙈
please anyone? 😦
expectTheUnexpected
Coequalisers in Top are surjective, so you only need to prove that it is open. Given an open set U in Y, you can saturate it with respect to the equivalence relation f(x) ~ g(x) by taking
U ∪ g(f⁻¹(U)) ∪ f(g⁻¹(U))
And this saturation is open
An open set with an open saturation wrt ~ maps to an open set under the quotient map defined by ~
Saturated wrt ~ means union of equivalence classes of ~
The saturation should be that because the saturation of a singleton is that and both image and pre image operations on subsets commute with unions
Is there some categorical characterisation of open maps in Top?
there's this, but I don't understand it haha
https://ncatlab.org/nlab/show/open+morphism
dang, never had proper topology, so I don't know what saturated means. brb learning
Another definition of U being saturated wrt ~ is U being an inverse image of the (set) quotient map by ~
So the quotient topology can be interpreted as "the open sets are exactly the images of saturated open sets"
A set and its saturation will have the same image under the quotient map because you're just adding all the things that map to the same image as something already there
So saturated wrt a function (ie wrt to equivalence relation defined by mapping to the same image under it) is a set such that adding anything enlarges the image
This is the language munkres uses to define quotient topology and I quite like it
So just that I get this right. You take the open set U in Y. Because h coequalizes f, g, we have that h(U) = (h o f)(g^-1(U)) = (h o g)(f^-1(U)).
I don't see why this means U' = U \cup f( g^-1(U)) \cup g( f^-1(U)) is a saturation w.r.t. h,
Then because h is quotient, it maps saturated sets to open sets, hence h(U) = h(U') is open, and h is open.
Oh you're right, that may not be the saturation
Saturation will be an even larger union
Any sequence of going back to X then coming back to Y will be there
They will all be in the saturation because the equivalence relation is f(x) ~ g(x) so for any x the image of any of its preimages of it must be there
And the saturation will be in this because this is saturated
Being saturated is easy enough to check because the equivalence relation is the equivalence closure of f(x) ~ g(x) and we are just taking the equivalence closure in this process pretty much
Saturated open to open
Oops
What are some conditions such that we can find an open saturation of a given open set? I suspect that these are exactly satisfied in this scenario
(they have to be lel)
The equivalence relation can be very different so idk if there's a general thing
But if you are coequalising stuff then maybe
Like we can say from f and g being open continuous that the saturation of U is open
But it may be open in other cases
It's an infinite union
right, but then the existence is not so clear yet?
Existence of what?

since I'm new to saturation: a subset U \subset B is saturated w.r.t. h iff U = h^-1(h(U)), right?
Yep
So this is the idea, right? If that's correct, then at least I know what things to check now.
Yep, though I don't see why the first equation about U is needed

Just thought of that, now I feel accomplished 🙏
But then I don't see where we use surjectivity of f and g 
Oh
the line is maybe not unnecessary, since it's basically saying: this holds for all open sets, since f,g are onto
just that it's not saying it explicitly
Yeah but that fact doesn't seem to be used later
I mean, we need to show that all opens get mapped to opens, but w/e. Those are just notes for me anyway
Right, but doesn't the argument work even without the image of inverse image under f being itself
Well, one might use it here: h(U) = (hf)(f^-1(U)) = (hg)(f^-1(U) ?
Hmm right, though it feels to me like this is true without surjectivity if you look at the element level (and view h as the quotient map)
And anyway you don't need equality
You need the left side to contain the right side
And image of preimage of U under f is contained in U
so, is the statement then that the coequalizer of two open maps is an open surjection?
Seems like it to me 
oh man, almost same formula as me, I'm trimbling
very good, thanks 🙂
Actually, I dont understand why this formula holds. I mean, I can believe that the right hand side is contained in the LHS by some induction argument, but I don't really understand why that's everything there is in h^-1 h (U).
Intuitively it seems right, but my intuition is a heaping pile of dung, so...
Suppose y is in the left set. then there is some x in U such that x ~ y. This means that there is a sequence of elements a_1,...,a_n of X such that f(a_1) = x and g(a_n) = y and f(a_i+1) = g(a_i) (or exchange f and g in this)
That is how you construct the transitive closure of a relation
or equivalence closure in this case I guess
reflexive symmetric closures are trivial anyway
F
brb enrolling in bachelors again
right, so if x~y, then there must be some "chain" of f's and g's connecting them, i.e. they must be in the image of f or g - because elements not in the image of f or g have equivalence class with just 1 element? wut
the statements are both true on their own
elements outside are not equivalent to anything else
and the chain thing
I don't get what you mean by the because

derivations are functions from the stalk to R, so composition doesn't make sense. Is this some other operation?
right, makes sense
thank
what’s the difference between level set,fibre of a point of a real valued fn and the preimage of that point?
3 notions but they seem equivalent to me
level set is apparently a special case of a fibre
fiber is a shorter name for preimage of a point
level set is a fiber of a function R^n → R in particular, according to wikipedia
james_ash_.
What is G_alpha?
"[0,1/2] can't be covered by finite subcovers." For this I would first say "there is an open cover of [0,1/2] such that..."
You say intersection of the U_n is {x} for some real number x, are you using Cantor intersection theorem here? That requires compactness. But here you could just say that the intersection is {0} by inspection
@wispy veldt
"are you using cantor intersection theorem." I think its common to have this result for closed-bounded intervals in R without mentioning compactness
doesnt seem like compactness is required only closed bdd intervals and diameter coverging to 0 (which i forgot to mention)
You'd be using sequential compactness to prove it though? At least that's the proof i know
yea

but i mean, the idea is this is heine borel in R.
u start with a notion like "closed and bounded intervals" and get the topological def of compactness.
yea james, ur not supposed to let Un = [0, 1/n], but instead you should continue the process of splitting up non-compact subintervals into more non-compact subintervals
Also
You can just explicitly compute that the intersection of the Un is {0}
So you didn’t have to pull out the nested interval theorem to make an argument anyway
I already said that

What's the point, in the end chmonkey wins anyway 
so what i did i was always taking the bottom part of the interval and made a sequence instead and i guess since they intersect at 0 we can use that as an open cover? cause i was both of the intervals wont be covered but then i realized we can cover 1 half by finite subcovers but the other can still be impossible to do so
so i made this adjustment with that in mind
james_ash_.
does that maybe makes more sense or am i still missing the point?
I think you want to rewrite this to be more clear, it’s a bit hard to tell exactly what you’re doing and the assumptions blah blah but
My understanding is [un,vn] is always not compact
Or specifically there’s no finite sub cover of O which covers it
Which you get because if all of them had a finite subcover you can just union the finite ones for each one
Hoohee finite subcover of O
Then you used the nested interval thm to grab a point x in each [un,vn]
Then grab an open set U in O with x in U
This contains some open ball B_e(x)
But now because the diameter of [un,vn] goes to 0
There’s some n so that [un,vn] < B_e(x) < U in O
So wait [un,vn] is covered by a finite subcover of O (in fact it’s a single open)
Is that correct?
yeah that sums it up well
ile try to write it more clearly i kinda rushed this your right

I think the proof works then
It’s just a little unclear how you’re taking the un,vn
And then the explanation of why it’s contained in your N_r(x) is kind of lacking
But the idea is good I think
Just need to polish it up
ye fair enough i can see the issues in my proof
thanks for the help 

hoohee
Why does that suffice? (I know that $SO(n)$ is connected)
gustavn64
Perhaps it has something to do with the fact that $\lambda$ is a Lie group homomorphism, and is therefore an open map.
gustavn64
You could also try lifting a path from the quotient Spin(n) / ker lambda
Using the fact that a quotient map of Lie groups is a covering map, cover the path (compact) with finitely many evenly covered neighborhoods. Lift the path in each one, by picking one of the two sheets arbitrarily. Now for two consecutive neighborhoods, pick a point x in the intersection, and connect the sheets with the path x --> -x you found.
Not specifically topology and geometry related but I think you lot will give the best answer
When you are late king the Mayer vitreous sequence
Or such similar things
Do you use tikzcd
Or just a standard display math with \rightarrows
The arrows seem too long when using tikzcd
You mean that it's a covering map on each connected component of Spin(n), right? So since ker lambda has two elements, this means that either we have two coverings with one sheet each, or one covering with two sheets. If it were two coverings with one sheet each, every loop based at the identity in SO(n) would lift to a loop. But since we found a non-loop in Spin(n) which maps onto a loop in SO(n), it has to be the case that we have one covering with two sheets.
Does that sound about correct?
A wedge of vectors is intuitively the oriented area/volume formed by their convex hull
At face value, just dual (multi)vectors at each point, but they vary smoothly as you move around the manifold, so they have an extra structure. Intuitively a k-form is precisely the kind of thing you can integrate over a k-dimensional manifold.
It's a covering map of the quotient space. Locally, each point [x] is evenly covered by 2 sheets, one containing x and the other -x
If a wedge of vectors represents an oriented convex hull, it becomes natural to express "how does a linear map distort volumes." You apply it to each vector in a wedge, and you get a new wedge. If the new wedge is a positive multiple of the old one, then the linear map acts on volumes by scaling.
A smooth map f is locally approximated by a linear transformation df : T_pX --> T_qY. So you can ask, how does it (locally) distort volumes? Form wedge products of tangent vectors (so the exterior algebra of T_pX), and look at how df acts on wedges.
Assume f : R^n -> R^m for now. Then df is a linear map at each point, that varies smoothly. The induced map on the exterior algebra should also be smooth. Fix a basis for T_pR^n and T_qR^m, say dx_1, ... dx_n and dy_1, ... dy_m, and you get a basis for the exterior algebra, given by wedges of these things. We can characterize df's action on wedges by writing down what it does to this basis. The induced map sends a basic oriented volume (a wedge of dx_i's) to a sum of wedges of dy_i's, weighted by coefficients which vary smoothly. This kind of thing, we call a differential form. (Technically we really want to do this on the cotangent space instead of the tangent space.)
So, in the same way wedges let us measure how linear maps distort space, differential forms let us measure how smooth maps locally distort space
where k-forms measure the distortion of various (oriented) k-dimensional spans
Now you play with this idea and see that you can make sense of integration on manifolds
And you get the slightly more mature intuition of "the things you can integrate over k-submanifolds"
Thanks I’ll check this out
excision gives that H(X,A)=H(X-A,\emptyset)=H(X-A)
but there are details you have to be careful about
when does thsi go wrong?
Honestly H(X, A) = H(X-A) sounds convincing to me on a intuitive level. Is that wrong?
Something something A not closed?
I’m a chmonkey so just ignore me. Chmonkeys don’t know AT, only sheaf cohomology
yeah like excision does only work when like the closure of B is inside the interior of A or something like that
wait how do you think of it intuitivly
oh yeah I see
wait isn't that exctly excision tho
or is there something else to it
because this is how I think of intuitibly lmao
like you just ignore A
ye that's what I said
but I used B instead 
B gang
chmonkey
thank you
both for having a name that is nice to say
and for your answer
chmonkey
question about algebraic topology: is it pronounced "chuh-monkey" or more like "shmonkey"
i’ve been saying it like ch-maunky
chmunky
sorry
choe
as in
type choe into google translate and use the english pronunciation
but honestly
joe monkey
what if everyone just said
joe monkey
i don't know if you got a good answer to this question because fuck reading the backlog lmao
The suspension is a functor, meaning that for two spaces $X, Y$, if $f : X\to Y$ is continuous, then there is an induced map $S(f)$ between the suspensions, $S(X)\to S(Y)$. It's not hard to work out what $S(f)$ should be, and how it should be defined.
You can prove that if $f,g$ are homotopic maps, then so are $S(f),S(g)$ homotopic as maps $S(X)\to S(Y)$.
A famous theorem of Freudenthal - the Freudenthal Suspension Theorem - is as follows
diligentClerk
diligentClerk
hmm ye okay I see
but like when talking about suspensions and stuff, do you talk about reduced suspesion or just "regular" suspeinsion?
because I've mostly seen the reduced suspension in play
The answer to that is: figure out what base category you're working in, the category of all spaces and the category of pointed spaces and basepoint preserving maps
Now, if $Y$ is $k$-connected for some $k$, then the suspension should be $k+1$ connected unless i'm badly screwing up here, and if $X$ is $k$-dimensional then $S(X)$ should be $k+1$ dimensional. So if we keep taking iterated suspensions, over and over again, then $Y$ becomes $n$ connected, $n+1$ connected, $n+2$ connected... and so on, and so the $2n$ in the question becomes $2n+2, 2n+4,\dots$
diligentClerk
So the right hand side of the inequality $dim X \leq 2n$ grows by $2$ every time we take the suspension of $Y$, and $\dim X$ grows by $1$ every time we take the suspension of $X$.
diligentClerk
It follows that if $X$ is finite dimensional and $Y$ is $0$ connected, then eventually, for some $k$, $S^k(X)$ and $S^k(Y)$ should satisfy the hypotheses of the theorem.
diligentClerk
Thus, for large enough $k$, for all $n\geq k$, $[S^n(X), S^n(Y)]\cong [S^{n+1}(X), S^{n+1}(Y)]$.
diligentClerk
Does this make sense?
okay wait let me read everything
This is what is meant by "stability." The maps between these spaces eventually settle down and become regularized after we take iterated suspensions enough times. One way to think about this is that there is a "stable homotopy category", where the objects are spaces $X,Y$, .... and the maps between them are homotopy classes of maps $S^nX\to S^nY$ for very very large $n$, large enough that the set $[S^n(X),S^n(Y)]$ is constant as a function of $n$.
diligentClerk
i don't think this definition is totally sufficient but it's close enough. The point is that like, because this set $[S^nX,S^nY]$ is eventually constant, perhaps it's better for us to study that constant set in some situations rather than $[X,Y]$. The theorem suggests that maybe this is a category worth studying.
diligentClerk
Stable homotopy theory is the study of spaces and maps between them after the suspension functor has been applied to them enough times that the hom sets stop changing.
Roughly speaking.
So, knowing that an operation on spaces plays nicely with suspension is important, because if something is unchanged by the suspension operation then you can study it as part of stable homotopy theory. This whole idea of "take the suspension however many times and then look at the maps between spaces" only works when you're talking about operations which are eventually constant under the behavior of this operation
For example, the homotopy groups $\pi_{k+n}(S^\ell+n)$ should eventually stop changing for large enough $n$. Asking that a cohomology operation is stable is basically asking that we are able to study it from the POV of stable homotopy theory.
diligentClerk
yeee okay I see
man daim
thank you so much for all the answer I got, including this
well the way hatcher says is it is that when A is a nice subset of X, H(X,A) = H(X/A). so this is a better way to look at it, i think.
but it is useful to think of it this way in some cases of relative homology, like for example if A is a subspace of X and you want to study 'the homology of A as embedded in X' then a natural thing to look at is like, the homology of X but we forget everything that happens outside A, i.e. H(X,X-A). which is what you said
i guess if it's reduced homology it's basically the same thing, because the base point is "nothing"
yeeee okay I start to see this
I will read this whole convo tomorrow tho because I'm super tiered to today
like I barely know what I'm typing in now
yeah goodnight diligentClerk!
💤
Can someone explain to me how the exterior algebra definition for determinant gives Cauchy Binet formula
Are open balls necessarily connected in a metric space?
discrete metric broski
Hello
I am learning about the quotient topology
but then they dive into this concept of partition(ing) and I reckon I am quite confused, even after trying to look it up online.
What are they trying to say here
@rancid umbra can I call you?
like in a voice chat?
sure
X = {a, b, c, d, e, f, g, h, i}
X* = {{a,b} , {c,h,i}, {e}, {f,g,d}}
A = {a,b}, B = {c,h,i} , C = {e}, D = {f,g,d}
X** = {{a}, {b}, {c} ,..., {f}}
Y* = {{a,b}, {c,h,i}} is a subset of X*
When we want to show that two spaces are homeomorphic, we need to come up with a suitable homeomorphism, my question is, what do you do to come up with one? Is it:
i) By geometry reasoning such as the polar representations or stereographic projection? i.e trying to find meaningful equation and then define a map based on that equation
ii) By trial and error
iii) By other means that I do not know? Sometimes in textbooks authors come up with the weirdest kinds of maps that I am so desperate to know how do they even come up with one
theres really no set of rules or algorithm to do this
I know, but I am struggling with defining maps on my own, I'm not looking for rules, but rather hints
Visual intuition lol assuming you don't have access to universal properties
The maps in intro top can usually be explained with some visualisation, do you have specific examples of ones that feel random?
To find the connection between geometrical objects in intro topology is not that hard, but I have to be careful with the map I choose based on intuition, because it requires bijectivity, continuity and continuous inverse, so I have to use the map in such a way to satisfy all of this
In other words, I have to choose my open sets well, and I have to be aware that my map that I extracted from a geometric equation, is going to be bijective
I just want to ask, when mathematicians encounter these problems, does it come natural to them and define the map in a matter of minutes or could it take more than an hour to define a simple intuitive map
So you are using a definition of covering which allows a covering space to be disconnected?
why would you require a covering space to be connected?
I don't know, this is what I have learned in the books I have read about it. But I suppose most theorems hold anyway.
are you sure?
weird
Anyway, suppose that we drop that requirement, then sure, I agree that Spin(n) -> SO(n) is a covering map. Given the fact that its kernel is {1,-1}, and the fact that there exists a path from 1 to -1 in Spin(n), how exactly does the argument go?
i said how it goes earlier
You just say to try to lift a path, if I understood correctly? I'm not sure how that implies that Spin(n) is connected
i said more right after
"It's a covering map of the quotient space. Locally, each point [x] is evenly covered by 2 sheets, one containing x and the other -x"? I don't see anything else you wrote related to this
I mean, this path from 1 to -1 in Spin(n) shows that there is a loop which lifts to such a path, i.e. the fundamental group of SO(n) acts transitively on each fiber
But why does this imply that Spin(n) is connected?
Using the fact that a quotient map of Lie groups is a covering map, cover the path (compact) with finitely many evenly covered neighborhoods. Lift the path in each one, by picking one of the two sheets arbitrarily. Now for two consecutive neighborhoods, pick a point x in the intersection, and connect the sheets with the path x --> -x you found.
Lifting the path? It is already in the cover, not in the base space. Not sure I understand that argument. However, I think I understand how one can do it. Given any points x,y of Spin(n), we can take a path between their images in SO(n) and lift this path to Spin(n), to a path starting at x. This produces a path in Spin(n) which starts at x and ends at y or -y. If it ends at -y, we can use the path from 1 to -1 to produce a path from -y to y. Thus x and y lie in the same path-component.
I'm saying to lift a path in the base space
the quotient should automatically be connected
So your argument seems like the same argument as mine, except that you use the path x --> -x while lifting the path, but I first lift to a connected path and then use the path x --> -x at the end if needed, if I understand correctly.
you're assuming my entire argument
"lift this to a path in Spin(n)"
how do you know this is possible?
Because Spin(n) is a covering space of SO(n)?
Let's assume that we already know that paths in the base space can be lifted to paths in the covering space.
So what we could do in your argument is that instead of picking one of the sheets arbitrarily, we pick the sheet where the last lifted subpath ended. Then at the end, we use the path x --> -x if needed
Sure
It depends, something it's easy and sometimes it's very hard
Hi! In the paper https://link.springer.com/article/10.1007/BF01078120 (which you can read on sci-hub by c/p the url above), there is the following which I don't quite understand:
F(x0,x1,x2) is homogeneous of degree 2k with real coefficients. We choose the sign of F so that the points corresponding the the non-orientable component of the complement of {F=0} in RP² is negative.
We now consider the equation z²=F(x0,x1,x2), where x0,x1,x2 are complex variables not all simultaneously zero. This equation gives a compact complex algebraic surface Y embedded in 3-dim complex space E of the 1-dim vector fibration over the complex projective plane P':E→CP²={[x0:x1:x2]} whose sections are homogeneous functions of degree k in the variables x0,x1,x2. From the real point of view, surface Y is a 4-dim compact smooth orientable connected manifold w/o boundary.
I don't quite understand the construction of Y... What is the meaning behind that equation z²=F(x0,x1,x2)? What is that vector bundle P':E→CP²? Does he define the vector bundle by means of all sections on open subsets of CP²? (which I don't understand because we have global sections here...)
(who buys legal copies of 1971 springer articles anyways? 😈)
Actually, reading through the rest of §2, is E defined as this?
$$E={(z,[x_0:x_1:x_2])\in{\bf C}\times{\bf CP}^2\mid z^2=F(x_0,x_1,x_2)}$$
Matplotlib
(which doesnt make sense because F(x0,x1,x2) is only defined up to a scalar)
it takes place in the line bundle O(k)
F(x0,x1,x2) becomes a section in that line bundle
well rather
F is a section of O(2k)
Yeah okay this I agree
and we look at the square roots in sections of O(k)
Okay, but how is this formally defined then?
well I guess you can cover P²(C) with 3 affine subsets
say U0 is the one where x0 doesn't vanish
so U0 = {[1 : x1 : x2] | x1,x2 in C} in an affine plane
the line bundle O(k) will be uuh U0 x C
and a homogeneous polynomial P of degree k corresponds to the section {([1 : x1 : x2], P(1,x1,x2)}
or rather
On U0, and then on U1 and U2 and you glue
I mean, okay I agree that F is a global section of O(2k)
or also {([x0 : x1 : x2], P(1,x1/x0,x2/x0))}
But my question was rather: how to make sense of this equation z²=F?
well then it becomes the set of points
of the form {([1:x1:x2], z) ; where z² = P(1,x1,x2)}
on U0
So E is defined on each three affine charts U0, U1 and U2 then?
yeah and they also glue together to make E = O(k)
Okay okay, I think I can work out the details now, thank you very much 🙂
That was helpful, I actually didn't think of O(2k) in the first place ^^”
and Y is compact because it is a branched 2-covering of P²(C)
basically the chart I picked for O(k) above U0 takes something called P that pretends to be a homogeneous polynomial of degree k and asks what is the value of P/x0^k
Actually, to put it formally, do you agree with: you have a natural map O(k)→O(2k) by squaring the sections
Then, Y is the surface of square roots of F in O(k), that is, you pre-image F under this map?
Is this true? I would think so, but don't see it immediately
So the first half is obviously just a question in Set
sh*t, also, A = X obviously
So, I'm doing things in Set now, and I only need to show one final thing. Namely, if a subset of $E \times_B X$ is $E \times_B f$ -saturated, then it is in particular of the form $U \times V$. I claim that it is actually given by $(E \times f^{-1}(f(V))) \cap E \times_B X$, but I can't see it.
expectTheUnexpected
element in free Z-module
I haven't learnt modules yet, should I do that first?
It's elements of the form a1[x1]+...+an[Xn]
with [xi] formal elements labelled the same as the xi's
And ai are integers
Basically, the same as a vector space whose basis is the set of xi, but coefficients are integers
What Matplotlib said. And at least for me, "formal" refers to the fact that you don't interpret the operation "+" in any meaningful way (yet)
Yup, [x1]+[x2] is nothing more than that, it's not related to [x1 * x2] for some operation *
but this is confusing
In mathematics, a free abelian group is an abelian group with a basis. Being an abelian group means that it is a set with an addition operation that is associative, commutative, and invertible. A basis, also called an integral basis, is a subset such that every element of the group can be uniquely expressed as an integer combination of finitely ...
Nothing, it's not a map
It's a formal element
Hausdorff
Oh so it's just there but has no meaning?
Yes and no, but it doesn't correspond to a map
Should I read all of this?
I was just giving the reference for the name, but you don't need it 🙂
Here, the notation is confusing, you should write elements as sums of [\sigma_i] and not \sigma_i
And so the \sigma_i are actual maps, and the [\sigma_i] make the basis of your group
What is [sigma_i]?
sigma_i is a map, obviously
See, I might be lacking algebraic background here
[sigma_i] is just a symbol
Well, that's the confusing part
It's something, it's an element of your free group
It just happens to be labelled the same as \sigma_i
Free group generated by?
Maybe think of it as a way of keeping track of data. Have you learned about "homologous cycles" in Complex Analysis?
Generated by the \sigma_i means that your group has a basis whose elements are symbols [\sigma_i] ine 1:1 correspondance with the actual maps \sigma_i
I haven't
Oh interesting
I think I'm getting it now
It just means "take a group with basis in 1:1 correspodance with elements of your given set"
You might as well label them the same because of that correspondance
Yep, okay
For instance the free abelian group over {a,b,c} is Z³, where each element is of the form (x,y,z), but also written as x[a]+y[b]+z[c] with [a]=(1,0,0), [b]=(0,1,0) [c]=(0,0,1)
By the way, what algebraic background would you suggest I know for sure at this point?
So that ([a],[b],[c]) is your preferred basis
My instructor has started talking about singular homology
For singular homology? Group theory, quotient groups etc
I'm familiar with that
What about modules? and free abelian groups?
I know free groups
Would make you a bit more comfty but that's not absolutely mandatory, it's almost the same as vector spaces so I'd say be fine with linear algebra and you'll work things out
It depends if you only talk about (co)homology over Z or any ring
If you do talk about homology over any ring, know what a tensor product is
Given a subset $S \subset X$ of a topological space and a map $f \colon X \to Y$, can we always find a smallest \emph{open} $f$-saturated set containing S? So, it's like a closure, but in general if would be an infinite intersection, so not necessarily open, right?
expectTheUnexpected
Yeah not necessarily. Consider f: [0,1] → {a,b} by 1/2 mapping to a, everything else mapping to b. Set S = {1/2}
really you can make any subset f-saturated by taking an appropriate f into {a,b} discrete
so your question turns into "does every subset have a smallest open set containing it?"
I guess we would call that operation open closure if it worked lmao
Alright, thanks!
Why is the stuff in blue true?
Am I missing something obvious?
that follows more or less immediately from the definition of free abelian group
note that it's about group morphisms from Sn(X) into other abelian groups
not into all groups
It's just saying that f:S_n(X)→G is uniquely determined by its image on all generators [\sigma_i]
Just the same as transpositions generate the symmetric group, the elements [\sigma_i] generate S_n(X) and so you only need to define f on such elements to have a well-define group morphism
Except in this case since it's free abelian you can also map the generators arbitrarily
Hausdorff I believe you have enough background to start thinking in terms of universal properties 
Now the true question: what is the universal property of Hausdorff spaces? 
Seems like nlab has got you covered, as usual: https://ncatlab.org/nlab/show/Hausdorff+space
What’s an easy way to show that identifying the boundary of a disk gives a sphere? I.e D^n/S^(n-1) = S^n
I have visual intuition how to construct an explicit homeomorphism but I was curious if there is a purely algebraic way to do it
This is a really dumb question but I don't understand why f can be extended over X^n union sigma iff fg_\sigma is null homotopic. Can't you just take an f such that fg_\sigma is not null homotpic and then extend f to X^n union \sigma by just sending \sigma to a single point?
\sigma grindset 😎
why exactly are maps with image in A homotopic to the identity in pi_n(X, A, x0)?
I guess a softer question related to this is that it feels odd to me that pi_n(X, A, x0) should be "smaller" than pi_n(X) so to speak. like i think the idea behind it is that we're treating A rather than x_0 like the basepoint by treating maps contained in A rather than x0 to be in the class of the identity
But unless im mistaken pi_n(X, A, x0) is homotopy classes of maps f: (D^n, S^n-1) -> (X, A) rel A
And an arbitrary map g(D^n, S^n-1) -> (X, A) with g(D^n) subseteq A shouldnt be necessarily homotopic to the constant map rel A?
since its not necessarily homotopic to the constant map in general?
I feel like i'm losing my mind, why is this a valid triangulation of a rectangle. I thought triangulations are supposed to be homeomorphisms, so how isn't the line through the middle getting in the way. Some points which were interior points aren't anymore
Moving this to a thread
The exact sequence of the pair is this long exact sequence
and it is long
can we instead just have a short exact sequence of rings
$H^(X,A)\rightarrow H^(X)\rightarrow H^(A)\rightarrow H^(X,A)$
lime_soup
Perhaps dumb question:
is it true that discrete spaces can never be compact, since the open cover {{x} | x in X} has no finite subcover?
Oh yeah that makes sense
Any finite space is compact right? Since its power set is finite so every cover is finite
Law of excluded middle?
Isn’t that always given in these contexts
Can topology even like, work, without that
Ah
I mean that’s pretty interesting, I thought lem was like everywhere in math
Like how sets are everywhere yknow
That’s cool, thanks
Is a pullback $X \times_Z Y$ automatically an open subset of $X \times Y$?
expectTheUnexpected
No
I don’t think so at least, I’m pretty sure that this is sometimes closed
Like if X = Y then the pullback is basically the place that your two maps agree
Or even easier, take Z a point
Then X x_Z X = diagonal of X inside X x X
And this isn’t open, it’s closed iff X is Hausdorff
:(
If $fg$ and $g$ are quotient maps, then $f$ is also a quotient map. The proof is: $f^{-1}(U) open$ iff $g^{-1}( f^{-1}(U)) = (fg)^{-1}(U)$ open iff $u$ open, and surjectivity is the general categorical fact that if $fg$ is an epimorphism then $f$ is an epimorphism.
expectTheUnexpected
Since quotient maps are exactly the extremal epimorphisms in Top, I was wondering if the statement "fg , g extremal epis => f extremal epi" is true in general.
Wait, this might be better for #category-theory
Oh, so actually $f, g$ continuous and $fg$ a quotient map is enough to conclude that $f$ is quotient.
expectTheUnexpected
If I have for n>=1 shown S^{n-1} is a strong deformation retract of R^n \ {0},
how does this follow next: for n >= 3 that R^n \ {0} is simply connected?
Hm alright I'm sure that is true. I just don't see how it is a corollary
For context, it is from Lee (p 201, topological manifolds):
Nobody
I know a retract of a simply connected space is itself simply connected.
Hm, not yet. Thus far we use the fact that S^1 has a non-trivial fundamental group
Oh wait, they do. Alright then it is straightforward. Since for n >=3, S^{n-1} is simply connected, so is R^n \ {0}.
thanks for the help!
I’m still stuck on this 
So the red part is Y, the blue part is the image of f and the yellow/green part is g. Let’s say that the white thing is a hole. Then fg is not nullhomotopic but can’t I still just attach the n+1 cell over that hole with no problems?
What am I missing?
Okay Max helped me lessgoo
Correct me if I am wrong, but I am pretty sure the answer for (a) is jack squat.
Hold on, dont answer yet.
If you take an open cover in Tau, it is also an open cover in Tau'. Since Tau' is compact, there is a finite subcover, which is also in Tau
Tau' compact implies Tau is compact
if by "tau' compact" you mean "x compact wrt tau'", then yes
Yes, my bad.
But the other direction wont cut it because there may be an open cover in Tau' that is not in Tau, so we don't have any information for that
Ooo, Hausdorff is the opposite
(X,Tau) Hausdorff means (X,Tau') Hausdorff
Discrete vs Indiscrete topologies is always a good starting point
Shoot, I always get them mixed up
discrete means powerset
Shoot, I always get them mixed up
But the Discrete Topology is not compact if X has infinitely many elements
Because you can take the open cover to be {x} for all x in X
What do you mean by collect along the top/bottom?
and comparable topologies will be in the same "string"
So I think the contrapositive is a good way to try and prove (b)
Actually, I'm not sure with this one ...
Why can't Tau be strictly finer than Tau'?
Nobody
Nobody
Oh, duh
wtf is the infinite-dimensional sphere?
Nobody
oh no
not the colimit
okay so you basically take every S^n and all the inclusions and then draw a big diagram and add S^\infty and arrows between S^\infty so that everything commutes?
Nobody
yeah nvm I need to read up on the colimit
apparently it has a CW complex structure
yeah okay I see. Is there a way to maybe visualize all this?
I assume it will be hard
but like, is it always the case that the colimit of cw complexes is itself a cw complex?
or is this a special case?
yeah okay I see. Do you maybe know where I could quickly read up on this?
okay I will give it a try. Thank you so much!
So
I’m trying to prove that if X -f-> Y is an iso on homology and X, Y are simply connected then f is a weak equivalence
Using the hints from class I’m stuck at one particular point
Namely I need to show that H_q(F f) = 0 using the serre spectral sequence (F f being the homotopy fiber)
I’ve gotten that like the bottom row of the serre spectral sequence stabilizes on the second page by using edge map shenanigans
But idk where to go from there
Not sure if this fits here or in #groups-rings-fields, but I will post it here. What is the intuition behind the Lie algebra of a Lie group? I know that as a vector space it represents the tangent space at the identity. But what does the Lie bracket represent here, intuitively? I mean, if you take a basis {e_1, ..., e_n} for the Lie algebra, then you can view them as a finite set of infinitesimal generators, in the same sense as a finitely generated group has a finite set of generators. If we look at the case finitely presented instead, we have a finite set of relations between the generators. Can the Lie bracket be viewed as an analogue of this, giving "infinitesimal relations" between these infinitesimal generators?
If I'm not mistaken, the Lie algebra determined the Lie group if you assume the latter to be simply connected.
Do you know the exponential map (from the lie algebra of a lie group to the lie group)?
I hear the phrase" the lie algebra is a linearization of a nonlinear lie group" but idk what the heck that means lmao
but that's defined for all t?
i am getting tripped up with this question on the tautological one form
i dont get how they want me to define "α*θ=α"
because it seems that these are elements of two different cotangent spaces
(this is assessed work so im looking for general understanding instead of direct answers)
im confused since we have α being an element and a map at the same time
this is what i have come up with
we can sort of "promote" a tangent vector of M to a tangent vector of T*M such that its sort of seen as an equivalence?
but honestly i have no idea what im doing
<@&286206848099549185>
i'm having a hard time with proving chain rule on smooth maps (milnor)
i've got f : M -> N and g : N -> P
f g both smooth, x is in M and f(x) = y
i'd like to show then that d(g o f)_x = dg_y o df_x
i can't see anything useful i can get from a comm diagram because there's no guarantee that dg or df are injective (how would you even use such a diagram anyway?)
i thought about trying to exploit the continuity of f and g by moving to the limit definition of the derivative
but i can't seem to wrangle anything from that either. I'm now considering using a taylor series expansion of f and the remainder theorem to get something workable, which ought to do it, but i have a feeling there's another approach the author wants me to get
a $1$-form $\alpha$ is a section $\alpha\colon M \to T^M$, so it induces a pullback $\alpha^\colon\Omega^1(T^*M)\to\Omega^1(M)$. since $\theta\in\Omega^1(T^M)$, $\alpha^\theta\in\Omega^1(M)$.
TTerra
so \alpha^*\theta = \alpha makes sense
equality of 1-forms
your flow is correct and you have correctly deduced that X is complete
i have not seen "induced pullbacks on one-forms" so im still a little confused
let $F,G$ be extensions of $f,g$ in neighborhoods of $x,y$, respectively. then $d(g\circ f)_x = d(G \circ F)_x$ by the definition in milnor, since $G\circ F$ extends $g\circ f$. the ordinary multivariable calculus chain rule will give you that this equals $dG_y \circ dF_x$. again, by the definition in milnor, $dG_y = dg_y$ and $dF_x = df_x$, so you may conclude $d(g\circ f)_x = dg_y\circ df_x$
TTerra
if $f\colon M \to N$ is a smooth map between manifolds, and $\omega\in\Omega^1(N)$, then define $f^\omega \in \Omega^1(M)$ by $$(f^\omega)m(v) = \omega{f(m)}(df_m(v)), \qquad v \in T_mM$$
oh, F and G are extensions to open sets in the embedding space.
TTerra
vry insightful
i think however the taylor series thing works too albeit much more ugly
taylor series
functions on manifolds
yep

multivariable taylor series
i see, its just a standard pullback applied to a one form, that makes sense
the problem here is that we havent assumed yet that $\theta\in \Omega^1(T^*M)$
aritmos
that would be part b)
ok, well, the pullback is still defined even if your form isn't smooth
and therefore i assume that there is some way to do it without coordinates
TTerra
so use this definition to prove part (a), and then go prove in part (b) that the thing is actually smooth
im trying to see if we have seen that in the class, but as far as im aware we have not and therefore would assume that is not the case
again, i am just given
ok, sure. and then you have to prove that α^*θ = α for one forms α. here, α^*θ is defined by the formula i just wrote
don't worry about whether or not α^*θ makes sense if you haven't shown θ is smooth yet. there's literally only one thing α^*θ could mean
my main problem is justifying the formula you wrote since we havent touched it
it's the definition of the pullback of a form
how have you not seen it if you're doing an exercise involving it?
or maybe you've seen a different definition of pullback. if so, what was it?
oh wait
found it
the difference in notation is tripping me up a bit but it should be the same thing
:,)
this is what you're looking for
it's the same thing i wrote, just without the argument v
but wait dont i have the opposite? this is the pull back of a one form via F, we have the pull back of θ (whatever it is for now) via a one form
a (smooth) one form $\alpha$ on $M$ is a (smooth) map $\alpha\colon M \to T^*M$, so the pullback of a form on $T^*M$ still makes sense
TTerra
it's a little confusing
you're pulling back the tautological 1-form (a 1-form on T^*M) by a 1-form considered as a map M -> T^*M
yeah my bad my point was that we still havent shown that θ is a one form
i just have that weird equation.
sorry if what im saying makes no sense
im not following the class very well
(i main phys and thought this math fit in well esp later with relativity but man does the class go fast and its so algebraic that it gets hard to follow)
i think i get what you're saying now
you could prove it's a 1-form before doing part (a) if that helps
$\theta$ still makes sense as a map $\theta\colon T^M \to T^(T^*M)$ so the formula for the pullback still makes sense, but i can understand why you'd be uncomfortable doing that if you've only defined the pullback for smooth forms, and haven't shown $\theta$ is smooth yet
TTerra
showing it's actually a 1-form should have been the first part of the problem tbh
DG is just hard
i was barely following my first class in it
now i've taken like 3 of them and it's my favorite subject
it just seems like all the math majors get it
and so ive kinda shut off
because i dont wanna ask stupid questions in lectures
while everyone else is asking about how to extend what we just learnt and stuff
just leading to a negative feedback loop
put them in their place by asking the prof questions about how it relates to physics
i can guarantee you you'll make some of the pmath majors confused

well the course then turns into semi-physics
sem1 we do differentiable manifolds
sem2 we do geometry of general relativity
(technically two separate courses but for the prof its one smooth yearlong class)
sounds fun
in my experience math majors like to ask complicated sounding questions of no actual substance just to flex what they know. don't worry about it too much
anyways let me have a go at showing that theta is a one-form, we have them defined as (smooth) sections
i took an intro course to diff geometry last year and so i still have the normie definition in my head (as just things that kill tangent vectors to R^n)
ok i see how by its definition, theta is a one form on T^*M (albeit we skipped smoothness)
now ill try plugging it into the lemma
idk if the q subscripts (your (p) evaluation) are in the right places but at least now all the stuff makes sense
the very first thing should be $(\alpha^\theta)(q)$ instead of $\alpha_q^\theta$, but other than that, it looks good
TTerra
youre right the q should be on the outside
but other than that it's perfect
alright two more parts to go
next is just local coords, which ill have to look at the notes to figure out (doesnt seem like it should be too hard)
and the last part is that for a diffeomorphism F:M->M, (T*F)*θ=θ
thanks for the help
oh wait
i used the formula without showing that θ was smooth, you said that it worked regardless right?
alright i guess ill just say that and hope theyre cool with it
they should be
they're the ones that put the pullback question before the showing it's smooth question

I wanted to be sure that this answer my partner and I have are right here. We just need to do c and d.
This is what he sent me for his answer. He fell asleep now but I just wanted to be sure it was all right.
Namely I'm confused why and how he made the vertices 2a - 2d.
wrong geometry channel lol
Oh. Which one would it be in?
This is pre university? But it's an advanced geometry class.
oh idk then 
Here's the full question if it makes it any better.
uhh, mp of AB is (1/2,0)
Where are you getting that?
We aren't trying to find the mp.
That first picture isn't the actual question, it's just one I found that also had it and a visual representation.
This is the actual question.
1a is the same as in the first image, just c and d.
ah wait, so you can do this just by scaling
like, a is just some vector pointing in the direction of the lower left vertex, so that when you scale it up by a factor of two, that vector lands on the lower left vertex. same for all the other points
then the vector pointing to the midpoint m is (2a + 2b)/2 = a + b
this was probably done for notational convenience
This is from a while back but I absolutely abhor telling people wrong things. The pullback X x_Z X where Z is the 1 point space is not the diagonal like I had claimed, it’s the entire product X x X lol. When Z = X and the maps X -> Z are identity, THEN X x_X X is the diagonal lmfao
For c, why can't I define the flow to be $\theta_{(x,y)}(t)=(x+ty,y=4xt)$?
Finitely Many Bananas
Why do I have to do the weird stuff with the differential equations?
The derivative vector field associated to your flow needs to equal your vector field at every point; I think yours only does so at t = 0?
Oh I thought it was only supposed to agree at t = 0
For example, starting at the point $(x,y)$ and $t = 1$, your flow ends up at the point $(x + y, y - 4x)$, where the vector field you are given has the shape $((y - 4x) \partial_x, 4(x + y) \partial_y)$, but the flow you define has tangent vector field $(y \partial_x, x \partial_y)$
Lartomato
Then you'd basically just define a linear approximation for your vector field at t = 0, but the flow is really supposed to give you the curve that you get when walking (or flowing wink wink nudge nudge) along your vector field
naisu
Hello everyone. Assuming T and S are linear maps what are some consequences that follow from ||Tv|| = ||Sv|| where v is a any element of a vector space V. Thank you for reading.
I meant norm of Tv = norm of Sv. Also let’s assume S and T are operators on V
||Tv|| = ||Sv|| for all v or some v?
For v = 0 

I'm guessing that S and T would differ by composition with an isometry then (assuming for all v)
So question: what does a homeomorphism tell us here?
I'm not sure I am following how that helps
Because take a basis of the image of S, choose a preimage of it under S, take image of that under T and this should be an isometry from im S to im T and then you should be able to extend this to the whole space as long as dimension and codimension are equal?
If the identity set map is a homeomorphism then the open sets in both topologies are exactly the same
Why is that exactly?
Homeomorphism tells you that image and pre image of open set is open 
Oh duh!
Well, we proved a seemingly niche theorem a while ago: If a continuous bijection maps a compact space onto a hausdorff space, then the function is a homeomorphism
Turns out this niche theorem is gonna come in handy :p
It's an important theorem 
Well, "seemingly niche." It seemed like a very specific claim when we first did it
I'm not sure what maximally compact and minimally hausdorff means?
Oh wow! That's quite the powerful claim
The 2nd exercise is asking you to prove pretty much exactly that 
Yeah, Nobody was very helpful. I was just having a hard time processing everything yesterday.
How so? I am not sure I see why this is?
Oh yeah, I understood that bit. I guess I am having a hard time understanding why coarser topologies can't be hausdorff, and finer ones can't be compact
Thank you for the responses. In conclusion it seems that there needs to be more specifications to have more interesting consequences.
If you have compact hausdorff X, you make it finer, you get hausdorff space Y. Suppose this were compact as well, but then this will contradict problem 2 because you have comparable unequal compact hausdorff topologies on the same set
Similar reasoning works for coarser topologies not being hausdorff
Hmm, alright.
I got another question. I need to induce R with the cofinite topology and prove every subspace is compact.
What is so special about R here?
And we use the fact that topologies finer than hausdorff topologies are hausdorff, and topologies coarser than compact topologies are compact
Nothing
Phew, that's what I was thinking. I just had to make sure
Okay, so let me share my idea for this one.
If we take a cover of a set in R, then the complement of this union is the intersection of the complements. Since there is at least one set that has one of these elements as a complement, we can just choose a set that has an element in its complement: and we just do this for all of the elements in the complement.
That is a finite number of sets, producing a finite subcover
But I am actually not sure if this actually the job (Perhaps all the sets I chose are all missing an element in my subspace)
Oh wait, I know what to do!
If we just considered one set in the cover, then there are finitely many holes in the subspace (possibly zero), then for each missing element, we choose a set that contains that element. This is a finite number of sets, giving a finite subcover
Yep
Perfect. For part b) I am pretty sure the answer is no, but I can't figure out a nice counter example
@quasi forum
Nvm
Big crank moment 
||R - {1/n, 1/(n+1), ...}|| are the open sets you should consider
Loon star
🐐
Yep, already found it :)
The big crank moment? 
What is Topology exactly a study of?
And how does it relate to things like geometrical shapes or 'knots'?
im not sure how to show that the tautological one-form $\theta\in\Omega^1(T^*M)$ relative to local coordinates $(x^1,...,x^n,p_1,...,p_n)$ for $T^*M$ is of the form $p_i dx^i$
aritmos
in the past we've found the local coordinates for maps between manifolds F:M->N but im not sure how to adapt that reasoning to what we have here
<@&286206848099549185>
it's going to be of the form $a_i dx^i + b^j dp_j$ for some smooth functions $a_i, b^j$, and here, $$a_i(q) = \theta_q\left(\left.\frac{\partial}{\partial x^i}\right|_q\right)$$ and $$b^j(q) = \theta_q\left(\left.\frac{\partial}{\partial p_j}\right|_q\right)$$
TTerra
now use the definition of the tautological 1-form to compute these
oh, i guess the notation might be misleading. these are functions on (a chart of) T*M, so the q here should be a covector
hmm i still dont really know how to proceed
i just think im missing conceptual understanding for the tangent and cotangent bundle stuff
(your definition with the a_i and b^j did make sense)
its just the inserting the tautological nature that is confusing
Yep. I chose to look at the sets $U_k=\R - {\frac{1}{n}: n\neq k}$. Not only does $\bigcup_{k\in \N} U_k$ cover $[0,1]$, but removing any of them would mean it will no longer cover it.
dackid
Where's the crankery 
I think this is the big crank moment (whatever that is) because I found this before anyone suggested anything.
Crank moment is like the opposite 
It's the stuff you find in the pinned messages of this channel 
Indeed 
I had a wrong suggestion (big crank moment) which I deleted before my right suggestion 
Ohhh, I get it now
you should have pi(x, p) = x in your local coordinates, so it's just a matter of working through the definition of the tautological 1 form and seeing what pops out
it might help to recall what p_i does to a covector as well
does it just pop out the "i-th coordinate of the covector"?
pretty much
alpha -> alpha_i
alright ill take a look at it after i finish this lecture
we're covering vector bundles now
if you're still stuck, you can ping me and ill see if i can help
Ok let p: E -> I^n be a fibration
if you dont know a fibration just means that there exists some F such that every x in I^n has some neighborhood U with p^{-1}(U) = U x F
I fibration p: E -> B is trivial if E is homeomorphic to B x F itself
anyway I need to find a way to subdivide the cube I^n up into N^n subcubes of length 1/N small enough that the restriction to each subcube is trivial
My idea was to take every point x in I^n, pick an open U around it, and then use compactness to find some U_1, ..., U_k covering I^n
and then take some N smaller than the diameter of each
But im still not confident that this actually works because it doesnt imply that each subcube is in fact contained in some U_i

Its a bit rude to post your question when someone else already has
Oh, I'm deeply sorry. What is the correct protocol in this situation? I wait until your question is answered or no one answers it for too long?
Yeah pretty much
I'm not used to Discord netiquette
No problem
I'll delete it and repost later then

anyway moldi do you have any ideass
This seems like it shouldnt be too hard at least from how its presented in the book but i cant think of a nice way to do it
I didn't even bother reading because you usually ask advanced stuff 

I dont really have intuition for why this should even be correct, an arbitrary fibration might be trivial over subsets U_1, ..., U_k and its entirely possible that you cant fill them with cubes
Feels like lebsegue number lemma
Rather than choosing the size of the cube to be less than all diameters you'd want it to be a lebesgue number of the given covering

i should file that away
and remember it
@kind cedar my question is resolved now if you want to post yours 
thanks
I was asked to prove that the vector bundle $T\mathbb{S}$ is diffeomorph to $\mathbb{S}^1\times\mathbb{R}$. I managed to prove that in a chart $U_i$ I have a map from TS to SxR, but my professor said I could prove it "globally" instead of locally. I don't know how exactly I should do that. I managed to construct a chart transition map, but what do I do with it?
Necrowizard
to prove it globally you'll want to come up with a diffeomorphism
do you guys think it's okay if I start a thread here to ask a question?
that's what they're for
How is this a homotopy?
A bijective smooth map? I did it on a chart, isn't it enough?
can someone help me actually compute a geometric realization?
for some reason I can't seem to verify for myself that geometric realization of horns is like
geometrically what it should be
Nobody
@gritty widget finally finished my other work and can get back to manis
by the "definition of the tautological one-form" should i be focusing on what they gave me at the start or what i showed in the first part
i wish i had some other example of how to find local coordinates based on some criterion




