#point-set-topology
1 messages · Page 225 of 1
You only have to worry about the cohomology of any one ball here
because the balls are open, right
so their union is a finite union of open sets that covers itself obviously
and their intersection is trivial
by exactness we get isomorphisms from the direct sum of the cohomologies of the balls onto the cohomology of the union
so as long as you can compute H^k(B) you're good
sorry I have to leave now
cya 
oh ok. Well thank you so much for your help! Let's see if @fading vale and I can work on part b. If you don't mind
Np 🙂
yes. Here's part b: Let A = ${(x,y) \in \mathbb{R}^2: 1 < x^2 + y^2 < 4}$ Compute $H^k(A)$ for $k = 0,1,2,\dots$
hype_db
ah i see
mhm before we work on part (b) id like to say that theres a much simpler solution to part (a) using mayer-vietoris
its basically what i described before, the balls are open so their union is a union of open sets covering itself and we can apply mayer vietoris because its finite
Moth In Shambles
meaning the image of each map is contained in the kernel of the next
yeah that's going above my head. I'm sorry. That circle with lines through the middle i don't know, and we haven't even mentioned kernals in here. I appreciate the effort there, but I think I'm just going to go with the longer way lol
maybe once I take a topology course I'll get it better
Let U and V be open sets in $R^n$ with U and V homologically trivial in all dimensions. Let $X = U \cup V$; suppose $A = U \cap V $ is non-empty. Then $H^0(X)$ is trivial and for $k \geq 0$ the space $H^{k + 1}$ is linearly isomorphic to the space $H^k(A)$.
hype_db
so yeah it's ok. I'll just stick with what I have lol
let's do part b so I can be done with this problem. lol
thats real wacky 
I agree at least it's only one problem he asked about this stuff
okay i havent really done much de rham stuff so i dont think i can help very much with the computation itself but as a hint: the cohomology should look like the cohomology of the circle
even cohomology wasn't defined in my book. I learned that word today

so I really don't know how to do part b. It's ok though, I can wait for either Moldilocks to come back or someone else to jump in. I'll repost the question in case if anyone else wants to jump in
part b Let A = ${(x,y) \in \mathbb{R}^2: 1 < x^2 + y^2 < 4}$ Compute $H^k(A)$ for $k = 0,1,2,\dots$
hype_db
Do you have a visual understanding of what this space looks like?
(also, is this integral or real cohomology? sorry if this was in the backlog)
I'd think it's a circle with radii between 1 and 4.
cohomology was a new word for me today, so I am not sure
What tools do you have? Meyer-vietoris (i.e. Covering it with simple sets)? homotopy invariance (i.e. homotopy equivalences induce isomorphisms in cohomology)?
their class hasn't even defined homotopy 
nope
That's why I'm asking 😉
we were given a version of meyer-vietoris, but someone else earlier said it was a very bad version. We did part a of this problem from other principles that I understand even though it was longer
Well, you can try applying whatever version of mayer-vietoris you have, if that's everything you have (C:
Do you have an idea of how one could cover this „circle“ (let's call it annulus instead) with „simpler“ sets?
I do not. I have no background in topology, and my instructor covered this on the last day of class without doing an example as he got stuck in the proof. It was really an unfortunate situation
Mayer vietoris essentially tells you that H(U\cup V) is determined by H(U), H(V) and H(U\cap V).
So if U, V, and the intersection are „simple“ in such a way that you already know the cohomology for these sets, you should be able to calculate the cohomology of the whole space.
You can first answer out of „gut feeling“ how you can find such a cover (i.e. with sets that „feel conceptually simpler“ than the annulus)
Then you can try looking through your resources to find what spaces are „nice enough“ that the cohomology is already known.
I don't have a gut feeling. I don't even know what cohomology is. Like I said I have no background in Topology. I don't know what spaces have known cohomologies
so I still have no idea how to go about the problem
Ignore the words „cohomology“ and „topology“, and try to think about it just visually – how can you cover this annulus with two simpler sets?
with circles? I don't know
Ah, good idea, haven't thought about that
In this case we require open sets tho.
The answer would be that we take a set U that covers the left half plus a bit more, plus a set V that covers the right half and a bit more
ok so U would basically start at 1 and go to about halfway and V starts at that halfway point and then goes to 4
it's ok. I can see it fine
the point is that the sets U, V themselves have known cohomology because they're „essentially ℝ²“, and the intersection as well, just „essentially two portions that look like ℝ²“
But what the precise properties are that you need here depends on what your material covered.
Has the notion of „contractible“ been introduced?
it has not
What book / lecture is this
Multivariable Analysis we're using Analysis on Manifolds by Munkres
So it's de rham cohomology, right? I.e. closed differential forms up to difference of exact differential forms?
Perhaps the intent of the assignment was to explicitly calculate it, lol.
yeah he called it the DeRham group. H^k(A) = C^k(A)/E^k(A) where C^k(A) is the set of closed k forms and E^k(A) is the set of exact k forms
doesn't munkres have an entire chapter on de rham cohomology
and yes it is asking to calculate H^k(A) for k = 0,1,2,....
section 40 talks about it. It's a short section though, and my professor got stuck in one of the proofs so he didn't do an example or cover anything cause he got stuck. He also did not mention cohomology at all
I assume it has been shown that H^*(ℝ^n) = (ℝ, 0, 0, …), right?
I can see if it's in the book. It wasn't covered in class
I should've been clearer. with „explicitly calculate“ I mean „don't use any tools like mayer-vietoris and try to find the explicit classes one-forms/two-forms contributing to the cohomology“, which would be… perhaps possible, but way less systematic, and I don't see an obvious way how.
with MV it's clear how to arrive at that goal at least :>
well, let's just do it with MV. This is my last part of a problem for the entire semester, and I just want it to be done lol. I am hopeful I'll understand all of this better when I take an actual topology course, it's just tough right now with how my professor did it
sure
So first of all we don't need to worry about H^k for k>2 since every such k-form must be zero.
Also, H^0 must be ℝ, since we only have one connected component (H^0 is the class of locally constant function up to difference of a constant function)
so that means it would be 1 since that is the dimension of R. And why is it 0 for everything larger than 2? If it's possible to explain with my limited background
Because e.g. H3(X) = (closed 3-forms) / (exact 3 forms), but both things in this quotient are a 0-dimensional vector space
got it
i.e. when there's no 3-form, there cannot be any „nontrivial“ one
that makes sense
We also need that $H^k(A \sqcup B) = H^k(A) \oplus H^k(B)$, where $\sqcup$ denotes disjoint union
lux
Because recall that the intersection of our left half and right half is essentially two disjoint portions of ℝ^²
and that tells us that we can look at them separately
So this A and B correspond to the U and V you were talking about earlier?
No, but to both halves of $U \cap V$, i.e. the top and bottom portion of the intersection
lux
they are also „nice“ as sets 🙂
oh ok. So U and V need to be defined in order to define A and B got it
and this is for the k = 1 case, correct?
The formula with the A and B holds in general tho, not only in our specific example, and for every k
ok got it
If you care for the reason: I think it's possible to show it directly when plugging in the definitions and noting that a form over A \cup B is exact iff the restriction over A is exact as a form over A and the restriction to B is exact as a form over B. Note that the „hard part“ is the converse, i.e. showing that an exact form over A and an exact form over B „together“ make an exact form over A and B together. But this works in this context since A and B don't intersect anywhere.
(with closedness we have the same, but it's easier since it's a local property)
Soooo
We have $H^\ast(U) = H^\ast(V) = (\mathbb R, 0, 0, \ldots)$ and $H^\ast(U\cap V) = (\mathbb R\oplus \mathbb R, 0\oplus 0, \ldots)$
lux
And this is enough data to be „plugged in“ to mayer-vietoris
I will write down the reason to look at in the future. I don't like accepting things without knowing the reasons, but for right now I'm ok just going with it. So then, what is this H^*? It's not the same as H^k is it?
And that ending result, is that R^2, or is that expression meaning something different
Yeah I feel ya, I don't like accepting such statements as well.
The * is just a placeholder, right. I could've also wrapped parentheses around it and write stuff like (H^k)_k = (…)
(Because H^k refers to a single cohomology group, whereas I wanted to write the values down simultaneously, so it's just syntactical shenannigans)
got it
The end result should be H¹(X)=ℝ, H²(X)=0, if I'm not being really, really stupid
well, if you don't mind, could we go through to check that? I'm so sorry, just without seeing an example actually plugged into MV I think seeing it in action would help
so in my statement of MV, H^0(A) is trivial (we have it as R) and H^{k + 1}(A) is linearly isomorphic H^k(A). But what exactly becomes H^k(A)? And if they are linearly isomorphic, does that imply they would have the same result?
Yes
I'm just verifying that I didn't do any stupid mistakes, I'm doubting my statement about H^0 a bit
let me think
ok no worries.
this makes me want to take a topology class really badly lol. Part of regrets not taking it this term
This is the poincare lemma I mentioned earlier
I mean it was either Topology or Computational ODE and I research dynamical systems so I guess it made sense
oh hey welcome back @empty grove
Hello
and yes, you mentioning Poincare really helped. I read the section so once he said that I was ok with it.
Ah cool
Ah, yes, I was stupid
It's not locally constant functions up to constant shift
It's all locally constant functions
I'll catch up on some of the chat
so I remembered correctly. But note that in that case H^0(A) is never 0 unless A is empty
H^0(A) is always ℝ^{number of connected components of A}
Which is what confuses me about the formulation of MV that you wrote, where it said that H^0 would become trivial.
here let me write out the entire thing again just to be safe. This is word for word from Munkres
that would be a good idea
Let $U$ and $V$ be open sets in $\mathbb{R}^n$ with $U$ and $V$ homologically trivial in all dimensions. Let $X = U \cup V$; suppose $A = U \cap V$ is non-empty. Then, $H^0(X)$ is trivial, and for $k \geq 0$, the space $H^{k + 1}(X)$ is linearly isomorphic to $H^k(A)$
hype_db
if you're curious, because it is easy to get the PDF online, it is on page 337 of the book
What does homologically trivial in all dimensions mean? All cohomologies are zero dim?
This is just wrong, unless Munkres has a very nonstandard way of calling the vector space H⁰ „trivial“
let me check the book. My professor didn't talk about it
Yeah any non empty space would have non trivial 0th Cohomology
I don't know if this helps, an open set A of R^n is homologically trivia in all dimensions if it is star-convex.
Yep, so the poincare lemma justifies this naming
Cohomologies being R, 0, 0, ...
Still think it's very misleading to call the specific vector space H^0 trivial, but „cohomologically trivial“ is a totally valid term.
do you think they mean cohomologically trivial when they say trivial in this book?
no, because the property „cohomologicall trivial“ applies to a topological space. H^0(A) is not a topological space.
got it
okay, let's use this
We've established that H(U) = H(V) = (ℝ,0,0…), i.e. U and V are „cohomologically trivial“
Where U was the left and V the right portion
The theorem now says that $H^{k+1}(X) = H^k(U\cap V)$
(avoiding „A“ because that's what I called one of my intersection pieces)
lux
Oh that's true. So I'm thinking of X as the one in the statement of the problem got it
yop.
So for X it's the entries for U\cap V shifted one to the right
And on the 0th entry we have the „clearly trivial vector space“ ℝ 😄
yes lol
0th Cohomology of intersection would be R² right?
yep
I see, cool
and that comes from the $H^*(U \cap V) = (R \oplus R \oplus 0 \oplus \dots \oplus 0)$ you had earlier right? At 2, that is $\mathbb{R}^2$?
hype_db
Every second oplus should be a comma, but yes
Although I'm not sure what you mean by „at 2“, since the second entry is 0 instead of ℝ²
Oh, no, the first entry is k=0
because that will give me H^1 ahhh
Yep, so
\begin{align*}
(H^k(U\cap V)){k\geq 0} &= (\mathbb R^2, 0, \ldots)\
\implies \quad (H^k(X)){k\geq 0} &= (\mathbb R, \mathbb R^2, 0, \ldots)
\end{align*}
lux
Wait that looks wrong tho
is it though? The theorm gave you H^{k + 1} not H^{k}
hence the values are shifted to the right, the first entry is just our H^0 we know anyway
i.e. H¹(X) = H⁰(U\cap V), H²(X) = H¹(U\cap V), etc
but that cannot be right, the first cohomology of the annulus must be ℝ as it retracts to a circle
and the theorem says it is trivial
here, do you think we should write out the whole proof? To see if it's all good? I can try to do it
You can try that, I'll try to recover this proof from full mayer-vietoris
Yeah you should get R, R, 0, 0, 0, ... 
its nonreduced cohomology i guess
We only need to worry about $k = 0,1$ as for $k \geq 2$, every $k$-form is $0$. This is because everything above this point will be in a $0$-dimensional vector space. Define $U$ as the left half of the region (plus a little more) and define $V$ as the right half of the region (plus a little more). Define $A$ and $B$ as the upper and lower portions, respectively, of $U \cap V$. We have that $H^k(A \cup B)$= H^k(A) \oplus H^k(B)$ because $A$ and $B$ are disjoint, and exact forms over $A$ and $B$ separately make an exact form over $A$ and $B$ together. So, we have that $H^(U) = H^(V) = (\mathbb{R},0,0,\dots)$ and $H^*(U \cap V) = (\mathbb{R} \oplus \mathbb{R},0 \oplus 0, \dots, 0 \oplus 0).$ Now, Mayer-Vietoris tells us that $H^{k + 1}(X) = H^k(U \cap V)$ and that $H^0(X)$ is homologically trivial, meaning $H^0(X) = \mathbb{R}$. Plugging in $k = 0$, one has $H^1(X) = \mathbb{R}^2$. Any other $k$'s give us a value greater than 2, meaning they are $0$. Therefore, $H^0(X) = \mathbb{R}$, $H^1(X) = \mathbb{R}^2$, $H^k(X) = 0$ if $k \geq 2$
hype_db
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From the long exact sequence we get an iso $H^k(U\cap V) \simeq H^{k+1}(X)$ only for $k\geq 1$
lux
Lux apparently this isn't the form of mayer-vietoris they were given
the version he has is just for the specific case of contractible spaces pretty much
Ah, so this is probably missing „is linearly isomorphic to Hk(A) for k≥1“
which is why we can't calculate $H^{0+1}(X)$ with that
lux
In my book it says k >= 0 not 1
for k = 1 it will be $\frac{H^0(U\cap V)}{\mathbb{R}}$
Moldilocks
That matches what I got from the sequence
yeah I plugged it into the sequence too
ALL HAIL THE SEQUENCE
so wait, is it right then? The way I typed it out earlier?
So H^0(X) = R, what does the quotient come out to for H^1(X)?
H^0(U cap V) is R^2 as 2 path connected components
and we quotient it by a 1 dim subspace so we get R
everything upto isomorphisms
odd. SO the book's theorem is wrong. So other than the division by R, is the rest of how I wrote the proof ok? It almost looks like A and B play no roll
it just looks like I mentioned them but then they didn't come up again later.
everything switched back to U and V
We got $H^*(X) = (\mathbb{R}, \frac{H^0(U\cap V)}{\mathbb R}, H^1(U\cap V), H^2(U\cap V),...)$
Yeah the A and B were for notational convenience here
you use them to figure out the cohomologies of the intersection
oh ok. SO just stating them in the way I did would be ok?
Moldilocks
in which way?
in the long proof I wrote out above. I tried to write out the entire thing
yeah you were able to write $H^k(U \cap V) = H^k(A) \oplus H^k(B)$
Moldilocks
thats why you were able to figure out the LHS
other than that yeah they didnt have a use
ah I see
alright. And then all I need to do is add the division by R in the last step, and I'm ok?
Well, thank you guy so much! That was a very long time to solve it. I hope it goes well. Thanks again!
Welcome 🙂
Hi I was wondering how to start this question?
part a) was this
these are results from part a)
althoug i cannot say i am 100% confident about my results
here is our cup product from class
im having trouble with b
my teacher said it might be easier to define the vector field by describing it on each chart, and then checking that these local definitions agree in the intersection of the domains of two charts
if it helps you can think of the vector field on R^2 and restrict it to S^1
there's a standard tangent vector field you can then use
whats the standard one
doesn't (x, y) -> (y, -x) work
you just need a vector field which gives a non-zero vector at each point of S^1
yea except im trying to do it formally using the definition for the tangent bundle
where the tangent space at each point is like
^yeah I was referring to this
equivalence classes of $A_p$x$R^m$ where $A_p$ are the charts in your atlas containing the point and m is the dimension of the manifold
『Urahairywizard』
sounds painful
wait what
yea its a super abstract definition its hard to work with
i've never seen that defn before
just use part a!
yea in Lee they use derivations which apparently only works for smooth manifolds
so our teacher gave us one that works for C^k manifolds as well
and they're equivalent in the case of smooth manifolds which we proved on our last p set
if you wanna look up the definition i think its in uh
y∂_x - x∂_y should work then because S^1 is C^\infty
"Tangent spaces as equivalence classes of n tuples"
just define cotangent space as a certain quotient in C^\infty(M) and take the dual, works for manifolds of any regularity
ah that's in lee
he gives a list of alternate definitions; that's one of them
ya i think im gonna use the derivation definition and use this one
i don't 'really understand the other definition too well
wait how do you show this forms a basis for the tangent space at a point
the tangent spaces are 1-dimensional so any non-zero element gives a basis
ah of course
Consider a smooth and free $S^1$-action on $S^2\times S^1$. Is this action equivalent to the action where one just acts on the second factor?
gustavn64
Or alternatively, is the orbit space always diffeomorphic to $S^2$?
gustavn64
Hey I'm trying to compute the addition of points on a cubic curve using group law.
The curve is given by $$zy^2 = yz^2 +x^3 -x^2 z$$
Let $A=(0:1:1), B=(1:1:1)$, I want to compute $A+B$ using $O = (0:1:0)$ as the identity. To do this I found the equation of the line between them to be $y=z$. Then plugging this into the cubic I get the only points of intersections are $A$ and $B$. From here I'm not sure how to proceed.
snypehype
a line intersects a cubic curve in three points if you count them with multiplicity
So one of them must have multiplicity two?
probably
hmm in that case I'm a bit unsure on how to compute A+B
Oh I just noted that $(0:1:1)$ is an inflection point, but not sure how that would help
snypehype
have you tried factoring zy²-yz²-x³+x²z after replacing y with z ?
Yes, I get $-x^3 + x^2y = 0$
snypehype
As I wrote in the question the only solns are A and B
{x = 0, y = y}, {x = y, y = y}
.......
have you tried
factorizing
-x³+x²y
into
three
linear
factors
-x³+x²y = ? * ? * ?
you need to factor it completely if you want to know the multiplicities of the roots
Ok, I see. So you get $x^2(x-y)=0$. But I don't understand how knowing the multiplicity helps with computing the sum.
snypehype
well know that you knows x appears twice as a factor and (x-y) appears once
it tells you that the line intersects the cubic in A with multiplicity 2 and B with multiplicity 1
and so, A+A+B = 0
Ah ok, I see. That works because O is an inflection point right?
are they not saying that O is the identity of the group ?
A is an inflection point if and only if A+A+A = 0
if and only if the tangent line at A intersects the elliptic curve at A with multiplicity 3
for any line, if it intersects the curve in three points A,B,C (not necessarily distinct) then A+B+C = 0
only this however doesn't completely determine a group law and that's why you have to arbitrarily choose an identity element to make a group
@wanton marsh ok thanks a lot for the explanation
the books on AG are so terse
I find it hard to make sense of these theorems sometimes
and I said something wrong somewhere and I'm not sure where xd
but hmm yeah most of the time we pick O = an inflection point
it's not A+B+C = 0, but A+B+C is independent of the line chosen, I guess
so you were right about needing O to be an inflection point, sorry
bdobba
how can a chart map into R*?
If I take the definition of the tangent bundle charst and star everything I do get this result
but I can't interpret this as being a chart
It's a bundle chart, right? And the codomain of such a map should be something like (open set in R^n) times some vector space
And (R^n)* is just some vector space -- not even that different from R^n, since they are canonically-ish isomorphic
I guess if you're just asking "how is this a manifold chart" -- in principle, the only thing you still need to do is identify (R^n)* with R^n via some diffeomorphism, then you can use this map to construct a map with codomain U' x R^n, and that's an open set in R^{2n}
@cursive flume
(If you don't know what a bundle chart is, ignore my first two lines)
how to prove r* is diffeomorphic to r @uncut surge ?
Do the expressions "dx_1, ... , dx_n" mean something to you? These are the standard basis of the dual space (R^n)*, so for a diffeomorphism between R^n and its dual, you could just take the mapping which maps e_1,...,e_n to dx_1,...,dx_n
why would this map be smooth and bijective?
I am familiar with dx^1,...dx^1n, they are the basis for the dual space
it's bijective because we map e_1 to dx^1 and so on so it's 1 to 1
but why smooth?
for it to be continuous would make senes because the dual basis is defined with the help of an inner product,which induces a toplogy on R* and it's the same as on R
but i can't see how the smooth structure would be the same aswell
Hi, dumb question ! A handlebody decomposition with k1 1-handles, k2 2-handles etc gives a CW decomposition with k1 1-cells etc, right ?
By deformation retracting all the handles ?
Is there an inverse operation for the exterior derivative, basically a translation of Biot-Savart law and its relatives into the language of differential forms? So, if I have a, let’s say, 1-form $\omega=udx+vdy+wdz$, satisfying $d\omega=0$, how to find at least one solution to $d\varphi=\omega$?
BIGfoot496
https://en.wikipedia.org/wiki/Closed_and_exact_differential_forms#Poincaré_lemma The poincaré lemma gives a very explicit way to find such an "antiderivative" if you're on a starshaped domain
In mathematics, especially vector calculus and differential topology, a closed form is a differential form α whose exterior derivative is zero (dα = 0), and an exact form is a differential form, α, that is the exterior derivative of another differential form β. Thus, an exact form is in the image of d, and a closed form is in the kernel of d.
F...
Thanks a lot! I’ll go and try to translate that Wiki text from Mathematical to English then😋
hi was wondering if anyone could help me with this question
having trouble with the reverse direction for a and also the example for part b
oh i just looked at lee for part b i can just take any submanifold that isn't properly embedded
Hi guys, I really need help with this question :/
(my sketch:https://www.geogebra.org/classic/hgyxdyxu )
Let ABC be an acute, non-isosceles triangle with D is any point on segment BC.
Take E on the side AB and take F on the side AC such that ∠DEB = ∠DFC.
The lines DF, DE cut AB, AC at M, N, respectively.
Denote (I1), (I2) as the circumcircle of DEM, DFN.
Let (J1) be the circle that internal tangent to (I1) at D and also tangent to AB at K,
let (J2) be the circle that internal tangent to (I2) at D and also tangent to AC at H.
Denote P as the intersection of (I1) and (I2) that differs from D and also denote Q as the intersection of (J1) and (J2) that differs from D.
(a) Prove that these points D, P, Q are collinear.
(b) The circumcircle of triangle AEF cuts the circumcircle of triangle AHK and
cuts the line AQ at G and L (G, L differ from A).
Prove that the tangent line at D of the circumcircle of triangle DQG cuts the
line EF at some point that lies on the circumcircle of triangle DLG.
Better suited to #geometry-and-trigonometry @dense mica
alright
I think this rather belongs in #geometry-and-trigonometry.
Also, please don't add so much unneccessary whitespace, your message covers over half of my screen 😉
Oh how weird my discord didn't load the last two messages, only after I pressed enter o.O
you must have a big monitor, this covers so much more than half of mine 
divisors are the easiest sub-things of a scheme that one can study
higher codim sub things are hard
(see: Hodge theory)
Let $P=T^*G$ be the cotangent bundle of a smooth manifold G. Let $\pi_1: P \to G, \pi_2: TP \to TG, \pi_3:TP \to P$ be the canonical projections defined on the bundles. Let $\alpha_q \in P, \omega_{\alpha_q} \in TP$ along the fiber $\alpha_q$. Define the maps $\theta_{\alpha_q}:T_{\alpha_q}P \to R, \theta_{\alpha_q}(\omega_{\alpha q})=\alpha_q(\pi_2 \omega_{\alpha_q}), \theta_{0}: \alpha_{q} \to \theta_{\alpha_q}$. Then $\theta_0$ is a smooth covector field and $\Omega_{0}:=-d \omega_{0}$ is a symplectic form on P.$
ProphetX
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trying to prove this theorem but struggling really hard 
this is how my prof started the proof(this is still ok)
can someone help me understand the last line here please?
i can't really see how it follows 
View $S^1$ as a subset of $\mathbb{R}^2\cong\mathbb{C}$, and view $S^3$ as a subset of $\mathbb{R}^4\cong\mathbb{C}^2$, and define an action of $S^1$ on $S^3$ by $z\cdot(w_1,w_2):=(zw_1,zw_2)$. Does there exist an orientation-reversing smooth involution $S^3\to S^3$ which commutes with this action?
gustavn64
My guess is that the $S^1$-action is somehow connected with the orientation on $S^3$, forcing a smooth involution $S^3\to S^3$ to preserve orientation. But I am not sure how to justify this.
gustavn64
If you have a metric space (X, d) and a subspace (E, d), and if a set is open in (X, d) then is it open in (E, d) also?
In general, no. Open sets in $E$ will be of the form $G \cap E$ where $G$ is open in $X$. So, for example, if you take an open subset of $X$ that does not intersect $E$, it cannot be open in $E$.
whysee
the empty set is open
So the big problem is that an arbitrary subset of X will of course not be a subset of E. The most reasonable thing you can ask for is "If a set A is open in X, then A intersected with E is an open set in E", and this is true
Correct
No, but your point about empty set is correct. I should've said non-empty in my statement.
I have almost a silly question, but if X and Y are two topological spaces and I have a continuous bijection f: X --> Y and a continuous map g: Y --> X such that gf=id, that implies X and Y are homeomorphic, right?
yes
Nice, it means I solved that problem. Yay!
Yes, I can. I was just making sure.
gf=id and f surjective together implies f is invertible. So, g=f^{-1}, and hence g is a bijection too.
How do you get fg = id?
that's direct from gf = id and f being a bijection
Right I see
Hey y'all I'm having a bit of trouble here. I need to show that A int. B is compact with the definition of compactness. But I'm really not sure where to start.
A U B was pretty easy, the intersection is the one I find difficult.
have you seen that a closed subspace of a compact space is compact?
and that compact subspaces of a hausdorff space are closed?
Doesn't matter if we did. We have to use the definition of compactness here
hmm
My thought is that we choose an open cover for A int B and then consider an open cover of B that contains the open cover of A int B
yea if you could extend the open cover of A cap B
well @quasi forum if you can show that A and B are closed (idk if you guys have heine borel) then A cap B is closed in A (or B, whichever you choose) and then you can extend it very easily by throwing in A - (A cap B)
this is a cover of A
and now use compactness 
But not an open cover of A
oh it is tho
because A - (A cap B) is open
and it covers A - (A cap B) obviously
and then we take our open cover of A cap B and throw them together
to get an open cover of A
Why is A/(A int B) open?
oh yeah you have to show that A cap B is closed
idk if you have heine borel
but you can show compact in metric space -> closed
Yes we do, that is one of the first things we learned
Yes
and then X - (A cap B) is open
so A cap (X - (A cap B)) = A - (A cap B) is open in A
alternatively A cap B is closed in X so A cap A cap B = A cap B is closed in A
But A is closed, how are you getting openness out of this
oh ur taking the complement of A cap B
which is open cause A cap B is closed, right?
Yes, but A is closed. How does takinh the intersection of an open and closed set imply it's open?
no i mean A - (A cap B) is open in the relative topology on A
because X - A cap B is open, and so its intersection is open in the relative topology
like it looks like this
this is A - (A cap B)
maybe i said this in a confusing way 
you only need your sets to be open in A
not necessarily open in X
I think it's worth pointing out our class mainly focuses on metric spaces. So topology/relative topology really doesn't mean jack to me yet
A is compact if for every open cover of A there exists a finite subcover
right
so like
you need open sets in A
lemme post an image showing what i mean by this
like U cap A isnt open in X right? thinking of X as R^2 or whatever
and A as R x {0}
open sets in A are open intervals
and those intervals arent open in X
but they are open in A
and furthermore if i take an open ball in X and intersect it with A i get an open interval in A
does this idea make sense? like a set can be open in our line without being open in the plane?
I appreciate the help, but I'm not sure I am getting much from this. I think I need a mental break
yeah thats fair
that happened a lot to me when learning topology id take a break and come back to something a few hours later and it went much much easier
Let $X$ be a connected topological space with nice enough properties to admit a universal cover. Assume that the fundamental group of $X$ is finite, so that the universal covering $\pi:\widetilde{X}\to X$ is finite-sheeted. If $f:X\to X$ is any (continuous) involution (i.e. $f^2$ is the identity on $X$), then the composition $f\circ\pi:\widetilde{X}\to X$ lifts to a continuous map $\widetilde{f}:\widetilde{X}\to\widetilde{X}$, satisfying $f\circ\pi=\pi\circ\widetilde{f}$. Does this map $\widetilde{f}$ have finite order, i.e. is there some $n\in\mathbb{Z}_{>0}$ such that $\widetilde{f}^n$ is the identity on $\widetilde{X}$?
gustavn64
Since $\pi\circ\widetilde{f}^2=f\circ\pi\circ\widetilde{f}=f^2\circ\pi=\pi$, we at least know that $\widetilde{f}^2$ preserves fibers. Can it be shown to be a permutation on each fiber?
gustavn64
Can anoyone help? Pick an arbitrary point D on the side BC of the triangle ABC, and consider the bisectors of the two angles at D and their intersections E,F with the sides AC and AB. Show that AD, BE, CF are concurrent (via Ceva's theorem).
@quasi forum You can do it similar to what Moth was doing, but using the compact subset defn(i.e. looking at open covers in X rather than showing it is compact as a subspace). Then you can just take the complement in X. Take an open cover $O$ of $A \cap B$. Note that since A and B are closed, $(A \cap B)^c$ is open. Add $(A \cap B)^c$ to $O$ then you get an open cover in X of both A and B. ||Since A is compact, you can find a finite subcover of A which is then also a cover of $(A \cap B)^c$. You can then remove $(A \cap B)^c$ from the cover to make it a subcover of $O$ again.||
Lunasong the Supergay
I guess spoilers don't work in latex.
So you basically just add (A int B)^c and then remove it again.
Where ^c is the complement wrt X
Nvm, I overcomplicated, editing
You can do it similar to what Moth was doing, but using the compact subset defn(i.e. looking at open covers in X rather than showing it is compact as a subspace). Then you can just take the complement in X. Take an open cover $O$ of $A \cap B$. Note that since A and B are closed, $(A \cap B)^c$ is open. Add $(A \cap B)^c$ to $O$ then you get an open cover in X of both A and B. Since A is compact, you can find a finite subcover of A which is then also a cover of $(A \cap B)$. You can then remove $(A \cap B)^c$ from the cover to make it a subcover of $O$ again.
Lunasong the Supergay
I think I get it now. A int B closed implies X/(A int B) is open. So the open cover of A int B and X/(A int B) is an open cover of A, or B. So that'll get the job done.
right: more specifically once you intersect the X - (A cap B) with A (or B) to get an open subset of A rather than of X you will get an open cover of A

also you should probably use backslash rather than / for set minus because it might be confused with quotient spaces
or -
I never know which slash is the right one :p
How's this @fading vale ?
,texsp ||spoilers works||
Shika-Blyat
yea this works
Sweet!
i think once u see the relative topology what im talking about will make more sense
but its the same concept

That'll be something I do in grad topology (fall semester)
Thanks!
I would rewrite {U, X\(A int B)} as U union {X\(A int B)}. And the finite subcover of A doesn't have to necessarily include X\(A int B), but as I write this, I realize you could just include it anyway.
The whole point of including X-(A int B) is to show that the rest of the open sets must cover (A int B)
surreal that they don't do relative topology in undergrad top???
wtf is relative topology
@fading vale so quick question. This argument did not really use the notion of metric/hausdorff spaces. Why exactly does it fail if it is not a hausdorff space?
if a space isnt hausdorff then a compact subspace isnt necessarily closed
for example, equip a space with the trivial topology
in general if you want to see why a Tn axiom is necessary just look at the trivial topology 
Tn axiom?
Also, when you say the trivial topology , do you just mean the space and the empty set?
yes but this is actually a bad example lol let me think of a good one
uh
two point space {x, y} and let the open sets be the empy set, {x}, and {x, y}
then {x} is compact but not closed in {x, y}
uh separation axioms, hausdorff is T2, T1 means singletons are closed, things like that
dwai if u havent seen them most dont matter very much 
T1 does not mean singletons are closed, it means given two distinct points x,y there exists an open set containing x not containing y, and an open set containing y but not x
...
which is equivalent to points closed

well said you gibbon
@tough imp isn't that T2?
nope
For T2 the open sets are disjoint
as in you have nbd U,V of x,y such that U\cap V is empty
oh ok
i thought there just had to be one open set per pair
like in the sierpenski two point space
yea
is there a T1.5?
there's something about it
isn't it just 2.5 and 3.5?
maybe
its 2.5 for urysohn spaces
I swear that varieties satisfied soemthing slightly stronger than T1 tho
and 3.5 for tychonoff
Like the version of varieties that are embedded in affine spaces and whatnot
maybe R something
If it's embedded in affine space won't it be at least t4
no, the topology is way fuck
you mean zarsiki topology right?
yeah
oooooooooooooooh
Whatever, I left varieties a long time ago
I deal with T0 spaces now
sober spaces gang
lol
nah continua are where its at
does T0 imply Sober?
Right
Schemes are Sober
right, I just mean that Schemes don't fit anywhere on this separation axiom scale
they're sober, but the most you can get from that is T0
Oh true
my book has the proof T₃ is hereditary then just adds "why does this proof not work for T₄ spaces" 
imagine learning the separation axioms lmao
this meme brought to you by "I dropped my general topology course cuz it sucked ass" gang
no wait, it was the product one
idk urysohn's lemma was fun in my topology class
Is that related to the partitions of unity or whatever
or like
open set inside a clsoed
exists a bump function blah blah
supported on
or whatever
i learned the stone-weierstrass proof from nlab but then the prof asked me to prove some function is not continuous
and i froze up

btw, are absolute extensors useful?
There is a simple procedure for calculating a knot group. Is there a reverse procedure? Can you take a group with a Wirtinger presentation and find some knot with this group?
abstractly knowing the fundamental group of any hyperbolic 3-manifold uniquely determines it up to isotopy so yes
as for explicitly drawing out the knot tho im not too sure :p
@empty grove 👀
hey what surface/manifold embedding is this emoji?

my guess was https://en.wikipedia.org/wiki/Boy's_surface , but I dont think it has the right genus
there should be more things like this
https://twitter.com/omnisucker/status/927521141463199744 found the original
guys I'm not sure f is continuous if it's graph looks like this :/
If i have two topologic spaces X,Y and two continue functions f,g X->Y how do i prove that C = {x in X : f(x) = g(x)} is closed in relation to X?
sorry if it's trivial
i thought that it's a subset from id(x) then objectively it's closed
considering f(g^(1)) = x as a subset from Id(x)
one of those two spaces needs to be T₂ i think
Yes
why?
Have you seen Y is Hausdorff iff diagonal in Y x Y is closed?
i missed that i think
thats a beautiful drawing
Trying to calculate pi_n(RPn,RPn-1): I have formed the LES of the pair and then since pi_n(RP_n) = Z and pi_n-1(RP^n) = 0 so I have LES: Z -> pi_n(RP^n, RP^n-1) -> Z -> 0 so the last map is surjective. What else do I need for the calculation?
Hey y'all, I'm really struggling with number 5. I'm not quite sure I understand where compactness comes in to play here
I know f is uniformly continuous, but how does that help? 🤔
Not in this class. We need to stay away from contradictions as much as possible
I'm interested
honestly, excercise 4 looks useful here. given x in X, x would never be in the image of f
there are no fixed points. f(x)\neq x for all x
ah nvm
thought excercise four was saying something diff.

analysis profs are deranged
one of my analysis profs was very pro contradiction
he liked to write contradiction even when it wasnt
he said something like "there might some sensitive souls who will claim that what I'm doing is not proof by contradiction, but I don't care"
Nah, my prof rocks!
Anyways, back to the problem
I was wondering if there was a way to make use of compactness in this problem

I see you read what I said earlier ultra
Nice try though
sadge
you have to reprove every theorem you use, but without using a proof by contradiction for them
Well it is in metric spaces
what is a minima in an arbitrary metric space?
Anyways slim, I'm confused on your hint. I'm straight lost
I mean sure, f(x)=x
Well, the function we actually care about is d(x, f(x))
Since X is compact, the function attains it's bounds by the extreme value theorem
And... since x is not equal to f(x), that infinum cannot be 0
So the epsilon is the mimimum of d(x, f(x))
Do I need to prove this claim? 🤔
Hmm, I feel like I've done this before. 🤔
But I'm struggling to do it for some reason
Yes
What?
So we are looking at the metric d(x, y) where y=f(x)
But I'm not sure if that helps 🤔
no consider the function g: X --> X x X, g(x) = (x, f(x))
Actually, I'm not sure how that's a composition. That's what confuses me
Ah, okay.
Then take the distance of that
right
And I think we've shown in the last that compositions of continuous maps are continuous
great. that finishes the proof
Yep, all I need to do is equip X x X with the max metric so it's really easy to see g(x) is continuous
So you told me earlier slim that the statement in the question may not be true if X is not compact. Why is that?
I'm not sure I understand why that's a counter example
got an interesting question thats been bugging me for the last couple of days, so I might as well ask it here to see if anybody has any input. Below is the initial question. The more general case is what I am interested in.
Let d: R^2 x R^2 --> R be the usual metric on R^2. Suppose X is a subset of the plane such that when d is restricted to X x X, it induces the discrete topology on X. what is the maximum number of elements X can have?
if by |R| you mean uncountably many, then no
it is countable, but its not infinite
its a really geometric statement
all points are not a distance one from each other
then its not the discrete metric
slimvesus
its saying that all the points x,y in X are a distance one from each other, or they are a distance 0, in which case x and y are the same point, when measured with the usual metric
slimvesus
im talking about the metric d(x,y) = 1 if x\neq y and d(x,y)=0 if x=y. is that not the discrete metric?
but yes this is also what i was thinking
but that's not the only one that induces the discrete topology
for instance replace 1 with any nonzero nonnegative constant and that still works
okay, then my fault for not being more precise
(yeah, I'm just talking about constants to be sure to preserve triangular inequality slim)
but, i have been struggling to come up with a proof that it actually is n+1 in R^n
i immediately thought of doing that, but this proof doesn't really lend it self to induction
ah strong induction
hmm. but don't you have to set it up like this: suppose X subset R^n+1 has more than n+2 points?
unless im not seeing something.
so, once you have two points x_1, x_2, you can essentially look at the points equidistant from both x_1 and x_2 an n-dimensional subspace of R^n+1
right typo
right. wlog, you can assume its not affine, right?
You can be a little more direct by taking the average of the n+1 points in R^n, then looking at the orthogonal line to R^n in R^{n+1} through the average point. The distance from the average point to the n+1 points will be less than one, so by continuity you can find two points on that line that are distance one from the n+1 points (all points on this line will be equidistant from all n+1 points)
That at least gives you the lower bound of n+1. For an upper bound, I would try to use the fact that the convex hull of n+1 points in general position is n dimensional, so n+2 points must have one point as not a vertex of their convex hull in R^n.
so, the orthogonal line is a function from R^n to R^{n+1}?
ok.
right
im going to have to read more about what a convex hull is, but thanks for the input guys. this was helpful
Having thought about it a little more, what I said about convex hulls is not correct
oof
I remembered a square has four vertices in R^2...
so the problem is still trying to get an upper bound...
Yeah, you might still want to try to argue that the convex hull of n points that are all equidistant from each other must be at least n-1 dimensional, but the argument is not obvious to me at the moment
Actually, in line with my lower bound argument, the line through the average of the n+1 points in R^{n+1} should be ALL of the equidistant points to the n+1. Only two points on the line will be distance 1 to the n+1 points, but they will be distance 2 from each other, so you can only include 1 of them.
this is what i was noticing with lower dimensional cases, but i dont know enough geometry? algebra? (not really sure what this subject is called) to formalize what i was noticing
The points equidistant from 2 chosen points is a hyperplane (it's the hyperplane perpendicular to the vector from one point to the other, based at the average of the two points)
Thus the points equidistant to more than two points are intersections of hyperplanes
You should be able to leverage that to show that it's one dimensional
I have other things I need to work on right now, but hopefully that gives you a direction to ponder
anyone?

one sec
if i take a neighbourhood filter at a point x generically, how i guarantee that for a element of this filter(Let's say A) x doesn't reside in the closure from this element A
i mean, how the elements from this filter really defines the general notion of neighbourhood and interior in topology??
sorry if i'm missing something important
@gritty widget any idea to explain this for me?
You are wondering how to recover the topology on a space X from the set of all neighborhood filters? I haven't thought about it carefully, but maybe you can do something somewhat indirect, like charqcterizing the continuous functions on X (into what space?) in terms of the neighborhood filters and recovering the topology from those continuous functions
But maybe not 🙂 I am just bullshitting thoughts
Trying to calculate for real proj spaces $\pi_n (R P^n, R P^{n-1} )$ I formed the LES and then noticed $\pi_n (RP^n)=Z$ and $\pi_{n-1}(RP^n) = 0$ so I have in the end $\to Z \to \pi_n (RP^n, RP^{n-1}) \to Z \to 0$. I don't think the LES gives me the answer directly, but maybe something with the homom. for orthogonal groups $O(n)/O(1) \times O(n-1) \cong RP^{n-1}$ or some fibration or covering for the $RP^n$ but I'm not seeing it.
PAHUS
Still thinking of this one if any one has ideas for this
guys, a open set in a topology can be both open and closed right?
yes
is it relevant?
Yes! Trivial example being the empty set since it's complement is the whole space which is open
if i construct a topology based on filters i get elements that are open and closed... i just noticed that
if you construct a topology at all you get sets that are both open and closed
since the empty set and whole set are both open and closed
*all elements
ah.
im pretty sure thinking of these as topologies is typically the wrong perspective
@ivory dragon how?
Nice, this is a neat topology that I hadn't thought about really before
@gritty widget have u seen the topology induced by filters?
it has the same propety
Mm not really, my level of experience with filters is about at the level of being aware of them
What do you mean by the topology induced by (a neighborhood) filter? You don't just mean the topology that created those neighborhoods in the first place?
since i was studying axiomatic set theory i was about to ask myself how partitions would work in a topology
we get something nice as showed
@gritty widget neighborhood filter actually
im kinda lazy to write LaTex but it's this
What's the squiggly with subscript at the end?
Vx is the centered filter
a filter that converges to x
A is a element from every convergent filter to x from A
that means that those points are adherent points from A (?)
we get that the closure from A is equal to A then A is closed... but also open since it's a element that satisfies the axioms
@gritty widget does it make sense? we can define adherent points with convergent filters
It has been a while since I have touched filters 🙂 and I am a bit occupied right now, so I am not able to follow atm
sorry
No no
What’s the open mapping? Without context we can’t tell you how ^^
well it is strictly monotone and continuous, i think you could use that
why not just use that f(x) is an elementary function
all elementary functions are continuous
what does it imply to say that the only element in the boundary from a set S is Ø? (besides the fact that any other elements different from Ø in S is in it's interior)
sorry if my question is bad written
@thorny flare so this problem for one depends a lot on your definitions of log and exp. However a standard definition of log is as the integral from 1 to x of 1/t dt.
with this definition
a standard argument can guarantee that log is cts
@obtuse meteor any light for me?
from metric space stuff. I.e. show that for all x in (0, infty) there is a e > 0 there's a de > 0 so that if |x - y| < de then |log(x) - log(y)| < e
as for showing that log is open
there's a standard result you should prove
which is that for a continuous strictly monotonic function f : I -> R, where I is an open interval, it's an open mapping and a bijection
The main property for this is that f(connected set (for example an open ball)) = connected set
and then connected sets in R are intervals
and you can argue that the connected set you get out has to be an open interval
bc it can't have a max/min (argument here)
I don't know what "an element different from empty set in S" means, since presumably S doesn't have empty set as an element
this will suffice to show open-ness, because reasons
yeah, I know that part
*is its boundary
🥳 🥳 🥳
is anyone familiar with the proof that smooth manifolds admit a symplectic form and has like 5-10 minutes?
I'd have some questions related to it,but i'd have to introduce some strange notations so if you don't have time/patience no worries
the proof that smooth manifolds admit a symplectic form
uh
what's your favorite odd-dimensional manifold?
no i mean 2n dimensional smooth manifolds sry
hm what ok i might get the statement wrong
(since its second derham cohomology is trivial + it's compact)
oh cotangent bundles
would you have 5-10mins to go over the proof?
but the notation is very yikes sry in advance
mathphys notation 
ok
here it's a bit strange he writes stars for the charts,but it's ok since r^n* is diffeo to r^n
this looks like a foreign language
he proves it in charts
then he just denotes
and here he lost me
but i'm open to any proof if there is other, I just don't get this at all 
like why does the cotangent bundle have a canonical symplectic two form
if you're open to another proof take a peek at prop 22.11
yeah this is just terrible to look at
i strongly recommend looking at another source.
yes
Let $M$ be a smooth manifold. Let $(q, \alpha) \in T^*M$. Define $\tau_{(q, \alpha)}\colon T_{(q, \alpha)}T^*M\to\bR$ by $$\tau_{(q, \alpha)}(V) := \alpha(d\pi(V)).$$ If $(x^1, \dots, x^n)$ are local coordinates for $M$, and $(x^1,\dots,x^n,y_1,\dots,y_n)$ are the associated coordinates for $TM$, then you can show that $$\tau = y_i,dx^i.$$ So $-d\tau = dx^i \wedge dy_i$, which is a symplectic form. (It's just the canonical symplectic form on $\bR^{2n}$ pulled back to $TM$, where $n = \dim M$.)
my prof is trying to prove that the liouville form is a form
TTerra
thats half of the profo
this is all for that
just to prove theta is smooth

or
to prove it's smooth
write it in coordinates like me
no hassle
this is also the proof in lee i think
he uses xi instead of y but whatever
how can you show the tau equality?
also in order to write d tau like that you need to be in darboux coordinates right?
my prof said we can't use that until we prove that darboux coordinates do always exist

the point of the canonical form on the cotangent bundle is that every coordinate chart for the cotangent bundle coming from M is a darboux coordinate chart
when i wrote d tau
i literally just used the definition of d
ww w wat
this is enlightening
my prof did a whole course on why darboux charts exist
i'll note this
ok the only point i don't see is the tau
you can prove this by just writing out tau as a linear combination of the dx^i's and dy_i's, and solving for the coefficients
discord took like 20 seconds to send that for some reason
how to use teh definition of tau you gave to compute what you wrote?
I mean to me it just looks like a chart expansion since tau is a linear map from the tangent bundle of the cotangent bundle of M to R
but im confused a bit
if it's in the a section on tangent bundle,it should be a vector field
i'm missing smth
i'm typing something
long
let's say $\tau = a_i,dx^i + b^i,dy_i$, where here the $a_i$'s and $b^i$'s are functions defined on (open subsets of $T^*M$), and the $dx^i$'s and $dy_i$'s are the $1$-forms on $T^*M$ coming from the local coordinates $(x^1,\dots,x^n,y_1,\dots,y_n)$. then, $$a_i = \tau\left(\frac{\partial}{\partial x^i}\right), \qquad b^i = \tau\left(\frac{\partial}{\partial y^i}\right).$$ these are functions defined on $T^M$, so to compute them, take $(q, \alpha) \in T^M$. then
\begin{align}
a_i(q,\alpha)&=\tau_{(q, \alpha)}\left(\left.\frac{\partial}{\partial x^i}\right|{(q,\alpha)}\right) \
&= \alpha\left(d\pi\left(\left.\frac{\partial}{\partial x^i}\right|{(q,\alpha)}\right)\right)\
&=\alpha\left(\left.\frac{\partial}{\partial x^i}\right|_{q}\right)\
&=y_i(q,\alpha).
\end{align}
so $a_i = y_i$. can you compute $b^i$?
i cant really see this cause tau: TT*M->R
ugh
this seems to be a vector field on T*M
let me reformat this crap
also there's a slight notation abuse that i would like to bring to light
TTerra
note
right
but one-forms can be written also as multilinear maps from TM->R
ok right
I can't see why do we have x^...n, y_...n as local coordinates for TM
if we have a manifold its tangent bundle contains 2n many coordinates
slimvesus
- being coordinates of points, 2) being coordinates of velocities
are the b_i-s coordinates of velocities?
sorry, i mean y_1,..y_n here
so TM has n many coordinates as base points, n many as coordinates from velocities
so n many for base points,n many ofr one forms
right?
de y_1,..,y_n are coordinates of one forms?
yes
y_i(one-form) = ith coefficient of one-form written with respect to dx^1, ..., dx^n
but x_1,...,x_n are coordinates of base points,why can we expand tau in terms of them?
the y part makes sense
the other parts of the computation are ok
i just don't see the first line
$x^i$ is defined on (an open subset of) $T^*M$ by defining $x^i(q, \alpha) := x^i(q)$. (so it would probably make more sense to write something like $\tilde{x}^i$ for the coordinate on $T^*M$)
TTerra
and neither why b^i should be zero 
\begin{align*}
b^i(q, \alpha) &= \tau_{(q, \alpha)}\left(\left.\frac{\partial}{\partial y_i}\right|{(q, \alpha)}\right) \
&= \alpha\left(d\pi\left(\left.\frac{\partial}{\partial y^i}\right|{(q,\alpha)}\right)\right) \
&= \alpha(0) \
&= 0.
\end{align*}
TTerra
in jargon, d/dy^i is "vertical"
it gets killed by dπ
and that shows that tau has the required form (heh)
does that make sense?
ok now everything's clear except the last statement here
with the pullback
yes
ah
if i think of my coordinate chart as a mapping $\varphi$ from an open set $U \subset TM$ to an open set $\bR^{2n}$ (where $n= \dim M$), then $\varphi^*\omega_{std}=-d\tau$ on $U$, where $\omega_{std}$ means the standard symplectic form on $\bR^{2n}$
which is exactly what it means for phi to be a darboux chart
lol wait
TTerra
this is very similar to something i've seen
is this similar to that? he defines the coordinates on TM by pulling back from TR^n

are you following Ana da Silva's book btw on your lecture? @gritty widget
my class ended lol
ahh
but we did not follow it (or any book)
a homeomorphism will take distinct open sets to distinct open sets and conversely, so the spaces ought to have the same number of distinct open sets
lime_soup
like, youre saying the image of your function is all isolated points?
if so, then... yes but not for the reason youre saying
singletons in the euclidean topology are not open
but that is NOT the same thing as being closed
(well, it is since R is connected in the euclidean topology, but "morally" not)
oh unless you mean
maybe im misinterpreting slightly
hold on
let me revise
yeah i was totally misunderstanding what you were asking
the answer is "no"
the sets you look at when checking continuity
can be ANY subset of the codomain
they dont have to be subsets of the image of the function
so for example
consider the function [f(x) = \begin{cases}1&x\in \bQ \ 0&x\not \in \bQ\end{cases}]
Namington
consider the function \[f(x) = \begin{cases}1&x\in \bQ \\ 0&x\not \in \bQ\end{cases}\]
this does map x to "isolated real numbers"
but its not continuous
because the preimage of (-0.5, 0.5) is not open
the preimage of (-0.5, 0.5), or equivalently the preimage of {0}, is R \ Q
which is not an open subset of R
in other words, it seems you were assuming the set in "preimages of open sets are open" was a subset of the image
but it can be a subset of the codomain
(-0.5, 0.5) is not a subset of the image {0, 1} of f
but it is a subset of ℝ
and so its preimage should be open if f is continuous
but it isnt.
does that make sense?
yeah I think so
so
if I have 1 if x in U and 0 if x not in U where U is clopen and (proper nonempty) subset of X and f maps X to R
then its cont?
cus then i'd just demonstrate all closed sets have closed preimages
i know the pushforward of a smooth form will be smooth
but if we have $\alpha=f^*\beta$ with $\alpha$ and $f$ smooth can we conclude that $\beta$ is smooth?
lime_soup
no
take f : {*} -> R
pick any form beta on R
f^* beta will be smooth
and f is smooth
damn
the situation i have is i have a pr:C^n-0 to CP^n-1
i know that alpha is smooth
and alpha=pr^* beta
i've been trying to use that pr is a submersion but haven't gotten it
submersions admit local sections
what book is this
thank you
lee ism
if s is a local section of pr, then s^*alpha = s^*pr^*beta = (pr \circ s)^*beta = beta, so beta is smooth
very useful result
big thank you
actually can you clairfy
one direction of the proof is just linear algebra, and the other is the submersion normal form theorem
ok
i can try
(pr \circ s)^*beta = beta,
is just because
pr \circ s is the identiy
right, on an open subset of the codomain of pr
but i was lazy and omitted the restriction
yes thank you
i was fine with the restriction being omitted
but i was a little sus
in whether we had an identity on the map of manifolds
or only after taking the tangent map
let us say, hypothetically, i wrote this sentence
"Nonzero classes in singular homology characterize closed surfaces which do not bound a volume."
would you debate me on this
or does it spark joy
maybe a weird question but i'm wondering if this captures the correct understanding of singular homology in a snappy, intuitive slogan
i think it basically captures the visual intuition for homology
if i was trying to explain it to people in a handwavy way this is how id describe it visually
vewwy gud uwu

