#point-set-topology
1 messages · Page 236 of 1
jesus christ
pain
geometry good
but do carmo's abuses of notation and consistent sweeping under the rug of technical details like this is irritating
unless i'm just being stupid
Wait isn't this just a thing you can generally do, extending a vector field defined along a curve to the manifold
Unless I'm misunderstanding and there's some relevant context here
if the curve is an embedding you can
Oh ok so the problem is that it isn't regular
yeah
But assuming you can construct such a curve making it normal shouldn't be an issue with Gram-Schmidt right
Since that process doesn't change the definition of A(s) along the curve that you already have
$\int_{\mathbb{C}^n} \log|x_1x_3x5 \ldots x{2n - 1} - 1| \neq 0$ for $n \neq 1$
Learner
I am trying to prove this result
Could someone explain to me what's going on here?
p is some random polynomial (with its first coefficient being 1) that doesn't have any roots
what about that dont you understand
It’s a complex polynomial but doesn’t have any roots?
Well, Hatcher says the whole thing defines a loop in the unit circle based at 1.
He's trying to prove that only constants can do that
ah i see
intuitively x/|x| gives you xs "direction"
as a vector of length 1
this is a concept from linear algebra (normalization)
Yeah, but what's the "x" in this case doing?
Does p(re^(2piis))/p(r) just end up being some random function, is there nothing special about it?
i dont know hatchers argument
I mean, formally it is a loop, but I can’t understand what it is doing intuitively
IIRC the intuition was wrapping up the polynomial p around the unit circle
I'm not sure I remember how that f_r accomplishes that, but it might also be too early for me
Okay so if I understand it correctly, the domain is [0,1] because the e^blabla “captures” every complex number so it’s sufficient to have a domain of [0,1]. Now f(0)=f(1)=1 and the function is continuous and therefore a loop??
And if it had a complex root then it would be a division of 0 so it wouldn’t be a loop?
Yeah, it's assumed that this doesn't have any roots.
But what about the "r" though?
After that he says that f_r is a homotopy of loops based at 1.
and I don't know what that means

Usually we say that we have a homotopy between 2 paths
So the function is a loop and a homotopy between all other loops based at 1? 0.0
veryfrustratedperson ✓✓
May I ask why are you reading this proof without learning the definitions of paths and homotopy first?
I’m just curious about this question so that’s why I’m here lol
I did learn the definitions of paths and homotopy first
well you dont need that
the idea is that you take any of the loop f_r, and you can see it is homotopic to f_0
(the homotopy arguement would be you are doing the loops f_{rt} with t\in [0,1])
oh, okay, thanks.
What do you understand by a homotopy?
A continuous transformation of one function onto another
(Hatcher always keeps the endpoints fixed)
Correct. Then f_r is a homotopy here between f_0 and f_1
And each f_r for r in [0,1] is a loop in the circle
Which is parametrised using the variable s
Yeah, but what worried me is that Hatcher didn't limit the r in his proof
If there a homotopy between f and a constant fn, f is said to be null homotopic. It might be useful to prove the equivalence of the following facts given h is a function: S_1 -> a space X
1.h is nullhomotopic
2.h is extendable to a function k:B_2 (disc) -> X
Couple it with the fact that z^n 'dominates' the value of f(x) polynomial with degree n you can show that under certain condition, which you can enforce every time, f(x) when restricted to S_1 is homotopic to the loop going n times around the circle where n is the degree of f.
But you have a contradiction! (Assuming you are proving ftoa)
Yeah, you don't need the interval [0,1] strictly. A homotopy is just a transformation, it can be done over any interval. So, in Hatcher's argument, f_0 is homotopic to f_r for any r bigger than 0.
Since the loop going n times around cant be nullhomotopic, assuming you know about covering spaces/fundamental group of circle
So Hatcher goes f_0 ~ f_r ~ w_n and hence by transitivity, w_n is trivial in pi_1(S^1) which is Hatcher's contradiction
Guys, r isn't a real number here, it's a complex number
The way you get a homotopy between $f_{r_1}$ and $f_{r_2}$, for complex numbers $r_1$ and $r_2$, is by composing any path from $r_1$ to $r_2$ in the function $f_r$
Tormeson
So if you define this path by $\alpha$, say, then the homotopy is given by $H(s,t) = f_{\alpha(t)}(s)$
Tormeson
modulo how you order the variables in a homotopy
@fading vale https://youtu.be/8EI_jKhHhdA
Based
PTYamin, more like PYTamin
get it? YT? Like YouTube?
oh you have videos on Galois theory! I will watch them and like them and then I will subscribe to the channel
Since when did nlab contain these articles
(from lee ISM) isn't it sufficient to show that the maps aren't topological embeddings or am i missing something
I think in principle you can have an image that is a submanifold even if the map itself is not a homeomorphism onto the image
loop around the circle twice xd
even better, the standard parametrization of the circle on [0, 2pi) is an injective immersion, but not a homeomorphism onto its image. the image is still an embedded submanifold
ah lol
lemme unstone myswelf
ohhhhh
righttt
cuz it says the image here
not the map
LOLL
ye thanks


i just realized the author's name is kkk

yikes
well, yeah
it's just repeated differentiation
no different than an elementary calculus course









why would you ever need anything past like the second order term 
what cursed shit requires you to expand the metric to the sixth fucking order term
you can already get some cool stuff with just the second order term
ikr
wtf is higher????????
thanks physics
apparently there is stuff in the opposite direction
idk why would one ever use those

Do physicists have an index fetish
I could mean anything
I see, it's like Schrodinger's cat. That's a physicist's favourite.metaphor 
This isn't only true for the unit sphere, right?
what do you mean?
"For every continuous map f:S^2 \to R^2",
Is this only true for S^2 (the unit sphere) or could this be any sphere?
you have to be careful about what you mean by antipodal but a similar result should be true of any space homeo to the unit sphere
Okay, thanks.
in particular any such choice of homeo to the unit sphere gives a sufficient analogue of antipodal

Is there a name for a multi-set M of points in some space S such that there is a function from real numbers to M? Or maybe something that is similar? I would like to consider such "paths".
can you explain a bit more?
It is not a homework question. I was thinking about the paths drawn by rotations of points around axis. Then I was thinking about the images of addition and multiplication by a constant (as functions). I thought that it could be a useful concept for describing generating functions, comparing them etc. Intersections of paths are ordered (as are real numbers). This concept can be generalized to surfaces and manifolds.
As opposed to sets of points, paths can wrap around themselves (as the case with rotations).
Paths don't need to be connected (so we can consider special cases of paths (such as piercing several layers of paper with a needle)
I can also consider paths in natural numbers (primality, residues modulo different powers, etc)
I know that the word path in topology is already reserved, so I wonder if such concept already exists and if it does what its name is
Did you find dF?
To investigate exactness of omega, you may want to consider integrating it around the unit circle starting and ending at (1, 0). If it were exact, what should this integral be?
idk i missed the lecture
:yikes:
this is for my homework lol.
6th lecture
also do u have any idea about a? @hollow harbor
like rly what i mean isi have to do e xterior derivative right
Yeah
i tried doing that
So for a you want to show the exterior derivative of omega is 0
and this is the eqt for it
?
yes?
or am i dumb
cause i missed that so wikipedia it is.
LolLol
can u give me ur notation for it @hollow harbor
if that's oki c:
cuz i really just dont get wtf is going on here lol
There should definitely be some minus signs in that definition wikipedia gave, funny.
You can look at the general formula for the exterior derivative and it's super confusing, but when you have a 1-form like f(x_1, ..., x_n) dx_k it just ends up being df wedge dx_k. So the derivative just falls on f (only if it's a 1-form!)
So in this case, you want to compute d(-y/(x^2+y^2)) (the x partial derivative dx, plus the y partial derivative dy) and then you wedge both pieces with dx.
Since dx wedge dx = 0, the dx part will go away.
So you really just need the y partial derivative times dy wedge dx.
so that is just derivative with respect to x multiplied by dx right

That's all that will matter (because the other part, the derivative w.r.t. y, will cancel once we get dy wedge dy).
Now be careful of the signs. One of these terms will give you dy wedge dx. The other will give you dx wedge dy.
When you flip dy and dx, you need to add a minus sign to the front.
They're "antisymmetric."
And you'll see that the two things cancel out once you flip one of the 2-forms.
So that wikipedia thing you saw has some implicit minus signs in it, that's what makes it confusing haha
d(x/(x^2 + y^2)) wedge dy?
That's the second term
I see...
Since we're summing the terms at the start
And since d(w + v) = dw + dv where w and v are any forms at all.
alright tysm
i think i understand

again thank you
I gotta go cause its fathers day but
luv u ll
lol*
is there any difference between this and simply considering functions R -> S x Z?
@hollow harbor i returned on my phone,sorry for pongg but idm if general formula is confusing i still wanna see it 😄
pls
I beg
LolLol
well for a 1-form with 1 var and 1 differential
Yeah
yey
Is it that for f * higher order form too?
but how do u get df for multivariable
I dont remember
Well for df you are kind of doing a chain rule. It's "df = (df/dx) dx + (df/dy) dy + ....". It's helpful to think of things as cancelling
Even though they don't
thanks a lot for you help ❤️
pretty much caught me up on the whole lecture
😛
so exactness means: The k-form is the exterior product of a (k-1)-form
teah derivative
Basically "exact" means "in the range of d"
And "closed" means "in the kernel of d"
my brain is infinitely differentiable everywhere mb
and closed means: The k-form's exterior derivative is 0
so like
Yeah
xdx is closed
Yep, we get dx wedge dx and that's 0
It's also exact, it's the derivative of x^2 / 2 (which is a zero form)
instead of wasting 2 hours on a lecture I come here and talk to u for like 2 minutes
ez
oh ye
its like the omega
Every exact form will be closed, because d^2 = 0 (try to prove that d^2(function) = 0, it's harder to check for higher forms though!)
hmm
d^2f = f''dx^2
and dx^2 is dx wedge dx
:perhaps:
idk if that last part is true
doe
so its
f'' * 0
which is 0
or im oversimplifying lol
True if f is single variable, if f is multivariable it gets more complicated.
Yeah lemme have a go for dat
wait a minute

what would d^2f be :yikes:
wait
i think i figure out
df' * dx?
First compute df
Then compute d of that
(it's a bunch of terms, each term is a 1-form which we know how to handle)
df = df/Dx dx + df/Dy dy
i use D to represent partial there
so d of that would be like
ahhh
df = df/Dx dx + df/Dy dy, first term: d^2f/Dx^2 dx^2 + d^2f/DxDy dxdy, second term is: d^2f/Dy^2 dy^2 + d^2f/DxDy dydx
so I think I figure out
it simplifies down too
d^2f/DxDy dxdy + d^2f/DxDy dydx
which is equal too
d^2f/DxDy dxdy - d^2f/DxDy dxdy
so it becomes 0
I think that is it :p
I wont ping u cause
I dont wanna keep hastling
but perhaps u will check this chat 😄
I will be driving soon lol
For most of the day
So someone else will have to answer
But yeah, that looks right to me!
The key thing here is that d/Dx and d/Dy commute (that means df/DxDy = df/DyDx)
yup thats what i did
since they're not actuaally differential forms i think
cause they're partial
cause u notice i did DxDy rather than DyDx
which was a detail I made sure to account for 😛
this can also be proven with logic not reallyp roven but conjectured
cause here take this for example,
x + y
we do x then y
it willgo to 0
both ways
x^2 + y, 2x then y, derviative goes to 0
xy^2, y^2, 2y, 2xy, 2y
it shows no signs of changing
"But sets of the second and third types are not open in the larger space..." - I understand this, but what is the relevance of this comment?
I think they're just trying to emphasize you get open sets that aren't open in the original space
but that's weird because the two topologies are the same - that's what they conclude
Well, that's not part of the reason
The reason is because those sets form a basis for the order topology
Yeah, both topologies have the same basis and hence are the same
So both topologies have the same open sets
Contradicting this
How does it contradict that?
Y under the order topology and Y under the subspace topology have the same open sets. But it also includes sets not open in R
Okay
can someone help me sanity check my sol to ISM prob 6.1:
(lee ISM 6.1: prove that for a smooth map F:M->N where dim M<dim N, F(M) has measure 0 using the fact that images of measure 0 sets under smooth maps remains as measure 0)
isn't M measure 0 in MxR^k and define F':MxR^k->N by F'(m,x)=F(m)
then doesn't it follow immediately that F'(M,0) has measure 0 in N since we can just piece together a covering of N, seems super overkill for lee to use sards if this works 🤔
What is the equation to work out the hodge star operator?
yes
liek, what is it
$\star \omega$
LolLol
what would dis mean?
or is that incorrect way
of using it
for a k-form omega
me gusta where you go 
you can probably find this on wikipedia or in any analysis on manifolds text
In mathematics, the Hodge star operator or Hodge star is a linear map defined on the exterior algebra of a finite-dimensional oriented vector space endowed with a nondegenerate symmetric bilinear form. Applying the operator to an element of the algebra produces the Hodge dual of the element. This map was introduced by W. V. D. Hodge.
For examp...
@past barn
@gritty widget ive looked at that page but I still dont really understand how to compute it
:/
the first problem I have is, where does n come from, and what would it's value be
the second problem I have is, what does the $\beta_{1}^{\star}$
LolLol
Okay I learned about these planes that you glue together to get a cool thing while reading about quotient maps. You can formalise the construction of a donut from a sheet of paper with quotient maps. (You take a "sheet of paper", fold it to get a cylinder and then you fold the endpoints togehter) But can't you do it with homeomorphisms too? What "visual" differences are there between quotient maps and homeomorphisms when they act on things?
quotients are about changing the spaces (and after doing that you get a map from the initial space to the new space, the quotient map), homeomorphisms are maps between spaces that are "topologically the same"
the point of homeomorphisms is that they don't change anything about the topology, so they're not exactly suited to glue stuff, because usually that will change the topological structure 
also a homeomorphism, as a function between sets, is a bijection, so you can't glue things because that would require identification
okay and what is a identification?
oh I mean just a function being non-injective
like
for f: X->Y, if f(a)=f(b), then you might say that f identifies a and b
like for example, if you wanted to make a cylinder out of [0,1]^2
you would want to maybe glue the top and bottom sides of [0,1]^2
"gluing" in this context is just making them be the same thing. you replace each points (x,0) and (x,1) with a single equivalence class
and the projection map is the map pi: [0,1]^2 -> [0,1]^2/~ that glues (aka identifies) the top and bottom
I think shika was making a good point about homeomorphisms too
homeomorphisms=isomorphisms in the category of topological spaces
from the topologist's perspective, if two spaces are homeomorphic they are really just relabelings. You might call a point blue, I might call a point purple, it's just names
Right okay, I get it now! In this case, gluing the [0, 1]^2 to a cylinder with the equivalence classes would require a non bijective function so it can't be a homeomorphism. But why is the definition of a quotient map like it is? So p^-1(U) is open iff U is open. How does that help with the "gluing" process?
Its backwards
the way its presented is
what you want to do is like
take some space
glue it in some way to get a new "space"
but whats the actual topology on this new space?
the topology you give it is exactly the condition in a quotient map
idk why people insist on presenting it in that way
basically the "definition" of a quotient map there is telling you how the topological data of the unglued space descends to give topological data for the glued one
ahhh okay. So a quotient map is a way to transcribe/give data about the topological structure of the unglued space and the glued space?
So maybe it's a way to "deliver" data about the glued space?
thats a good way of thinking about it yeah
Hmm but it almost feels more natural to define a quotient map to be p(U) is open iff U is open. But with this, we can't really say what the open sets in the glued space are and therefore it's "better" to define it using p^-1(U) is open iff U is open because then we have the information about the open sets in the glued space. Is this a good way to think about this?
For me, the thing that motivates the quotient topology is that it is the finest (most open sets) topology that makes the projection map continuous
from the point of view of semi-lattices quotients are what we usually call subobjects and subobjects are downwards closed sets
it's just a smaller collection of closed sets that's closed under intersections
oh boy, here we go again
I mean you seem to be having trouble understanding quotients in topology
Sorry but I don't really know what a semilattice is. I really appreciate the effort, but I don't really get it yet
just think about what happens to P(X) when you take a set-quotient
the former construction might not be closed under intersections. let $p(U)$ and $p(V)$ be open sets. then $p(U \cap V) \subset p(U) \cap p(V)$, but the other inclusion may not hold.
oh no my tex
yeah I actually thought about that but then you deleted your post and then I started to worry that I was wrong lol
TTerra
yeah i deleted it since i wanted to get on my computer and type a better answer lol
Half of Rosen's "oh no my queen" moments 
the thing is, $p^{-1}(U \cap V) = p^{-1}(U) \cap p^{-1}(V)$, so this isn't a problem in defining a topology
TTerra
yeah now I get it lol
okay I get it now. Thank you all so much, it really helped me to understand the intuition behind this!

@drifting sundial What would Z represent in f:R->SxZ? Current multiplicity of point on the path? If so, it is a viable model.
You want to define the open sets of the image (post glue) based on the original (pre glue)
oh whoops nvm
yes tterra has a better answer
very sleepy shouldnt be mathing
Oh hey, it's the lattice guy
My hero
He's an expert in his field
Of making all of topology incomprehensible

I dream for the day we get Urysohn's lemma in terms of upper semi-lattices or whatever

I mean, I just actually know topology... SMH, you should really lose your sully privileges for sullying people who know what they're talking about. This is like stack exchange all over again.
Please formulate Urysohn's lemma in terms of semi-lattices
i don't think there was ever doubt that you know topology. you just present it from a different viewpoint that most people here don't share or find pedagogical to people learning it for the first time
Imagine where society would be if y'all just accepted his opinions 
We'd have so many more godly copy pastas
But seriously tho do you have any resources where one could study this?
Because that would be better than just bits and pieces from you over text without knowing prerequisites
Ye, I'm actually kinda interested in seeing if these kinda definitions would make some parts of topology easier
it's just meme-tier when you answer with this stuff to someone asking something about elementary topology 
but yeah same, I'm also interested 
+++++++++++++++
I can't even say whether this is good or bad because I don't know half the terminology.
yep
holy hell
I think you could even interpret this as an actual topological path. in the case of rotations, choose some basepoint like (0,1) and identify all of its copies to get a quotient.
alright!
it should come out to something familiar

just for simplicity do it for n = 3
you've already done part of the computation anyways
alr
lol the person in my server mad at me
this is
d*df
now star of that

wait
is that like
$\star d\star df= \frac{\partial^2f}{\partial x^2} + \frac{\partial^2 f}{\partial y^2} + \frac{\partial^2f}{\partial z^2}$
uhhhh
UHHHHHHHHHHHHHHH
LolLol

there we go
correct
yay!
this is the laplacian!
TTerra

delta!
alright
i use
that
now what would
$\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star d\star df$
be

LolLol
coool thing is i realized u can rewrite physics equations with this
cause maxwells equations use a lot of those operators
which can be written in termsof exterior algebra operations :p
Please avoid spamming in topic channels. 😅
Why is the part in blue true?
If Vn is not dense, its closure is not X, so the compliment of Vn closure is a nonempty open set. hence we have an x0 and that x0 has a neighborhood around it that is not in Vn closure
Hausdorff
Yes it is. If |x|<r then |x+x_0-x_0|<r so x+x_0 is not in Vn. If it is the equality that is bothering you, we could take the closed ball of radius r/2 instead.
Thanks!
Hausdorff
I think it's just a matter of applying $\Lambda$ to $x_i$, and since $\Lambda$ is continuous you get $\Lambda x_i \to y$.
The rest seems like a matter of bookkeeping
Apopheniac
Wait what do they mean by THE open unit balls
Are they assuming that they are centered at origin by default?
Okay assuming that the unit balls are centered at origin, I have a proof. Let me type it out
if you see an alg topologist using coordinates (which they rarely do) its probably based on the most obvious choice of imbedding
hi, I've been trying to understand weil divisors, and am wondering if someone could help or point me in the right direction to a source which doesn't require knowledge of schemes etc
(I don't know.)
Does this definitely need the Baire theorem?
It seems so much simpler somehow.
Hausdorff
Looks good? Let me know if you see any errors
I realized I wanted to post this in #advanced-analysis but here it is now, oops! Hope it's not too off topic
@verbal wraith
In the spirit of not just sullying but explaining the sully, no one is sullying you because you are wrong. they are sullying you because you keep trying to shoehorn a POV that people don't respond to. If you acted like this on stackexchange I have no doubt people would be annoyed as well.
Im writing something up currently but realistically I'm not close to done.
new copypasta?
lessons in why it's important to learn math before category theory
i mean you can actually phrase a lot of point set very elegantly in categorical ways
but thats not related to the semilattice business
in some ways the category theoretic stuff can even be expressed without a fore-knowledge of category theory
but I am hesitant to try it out on people who are already confused by the way their source or teacher presents stuff
@gritty widget hi, you is pro at exterior algebra thingies, cans you explain interior product owo
it's relatively simple
gud gud
if you have a k-form on a vector space and a vector v, you slot v into the first argument of your form and get a (k - 1)-form
LolLol
if $\omega$ is a one form and $X$ is a vector field, then the interior product of $\omega$ by $X$ would just be $\omega(X)$
TTerra
LolLol
let me be a little more precise for a moment
but that still have differential
i told you the linear algebra version
now let me tell you the differential forms version
linear algebra: if $\omega\colon V^k \to \bR$ is a $k$-form (so alternating and multilinear), and $v \in V$, then the interior product of $\omega$ by $v$ is the $(k-1)$-form defined by $$(\iota_v\omega)(w_1,\dots,e_{k-1}) = \omega(v,w_1,\dots,w_k)$$
TTerra

to get the version for differential forms on manifolds (e.g., open subsets of euclidean space), replace "form" by "differential form" and "vector" by "vector field"
roughly
can u do example
(if k = 0, we define the interior product to be 0)
lol
oh
i see
so like can U do with
vector field = (x,y) and differential form is xydx + xydy
if our vector field is $X$, and the form is $\omega$, then it's the $0$-form (a function) given by $xy,dx(X) + xy,dy(X).$ since $X(x, y) = (x, y)$, $dx(X) = x$ and $dy(X) = y$, so the interior product ends up being the function $\bR^2\to\bR$ given by $$(\iota_X\omega)(x, y) = xy(x + y)$$
TTerra
differential 1-forms eat vector fields and give functions
(one way of looking at them)
(also my favorite since it keeps the notation simple and computations cleaner)

sadge
my brain does not understand
applying dif form to vector field
stinky brain
:C
like how u compute
dx(x,y)
=
x
hows
😢
learning math is precisely learning ct, nothing else is real math
$dx:T_p M \to \mathbb{R}$ takes as input tangent vectors. This form in particular satisfies
$dx(\partial_x) = 1$
Apopheniac
Ty 

Perhaps "orbit"? Or "the orbit of a point (or points) under the action of a 1-parameter subgroup of a Lie group"
"Orbit" means the points you get after applying the action of the group. "1-parameter subgroup" meaning you'd like to move the points according to a curve, not a surface etc.
can you recommend me a few sources on graded algebra @gritty widget
i looked up in gallian and dummits book
didnt find it
did you check atiyah macdonald?
matsumura chapter 13
atiyah--macdonald chapter 10
Eisenbud does a lot of graded stuff throughout
would anyone like to do a reading group on hatchers spectral sequences over the summer?
These are three persistence diagrams produced by different datasets that represent the same underlying phenomenon. The points themselves are in a 512-dimensional space, but my computer doesn’t let me go that high. I know that these points lie roughly on a sphere in 512D, and the main question I’m interested in is how they are distributed on that sphere.
The 0D part of the diagram tells me that there are multiple connected components (usually 2, but potentially up to 4 in one of the plots) and no higher level structures (which is expected if they are distributed around a 512D sphere). I'm not sure what (if any) meaning the large gap in the 1D and 2D PH along the line x = y means.
Has anyone seen things like this before / have advice about interpreting these diagrams?
I have a topology question: In the moore plane (https://en.wikipedia.org/wiki/Moore_plane), do there exist disjoint open sets U and V such that U contains all (x, 0) points where x is rational, while V contains all (x, 0) points where x is irrational? I suspect the answer is no, but I don't know how to prove that.
(I'm self-studying, and this was an exercise, and I don't know how to even start this.)
Okay so this is the theorem that I'm reading now: Let X be a space. Then X is locally compact Hausdorff if and only if there exists a space Y satisfying the following conditions:
(1) X is a subspace of Y.
(2) The set Y-X consists of a single point
(3) Y is a compact Hausdorff space.
After the proof, the author writes "if X is not compact, then the point of Y-X is a limit point of X, so that the closure of X is Y". I don't understand how that follows. Why is the point of Y-X a limit point of X when X is specifically not compact?
okay so if that point were not a limit point, then X would be closed in Y since it would contains all its limit point. But then it is a closed subspace of a compact space so it must be compact, a contradiction I guess
Seems correct, though I'd hope there's a nicer way
I think it's a little more clear by contrapositive. If the closure of X is not Y, it must be X. So X is a closed subset if a compact Hausdorff space, and thus compact.
yeah that's true. Thank you!

petition to go back in time and tell old geometry authors that \langle and \rangle are a thing and to not use < and >
If $Y={P_1,P_2}\subset \mathbb{A}^2$ how do i find $I(Y)$. Am I right in thinking its $\langle (x-p_{1,x})(x-p_{2,x}), (y-p_{1,y})(y-p_{2,y}),(x-p_{1,x})(y-p_{1,y}),(y-p_{1,y})(x-p_{1,x})\rangle$
lime_soup
This channel is super cool
Visual Topology & Geometry is a project aimed at creating math animations of various spatial objects and their transformations. Visual representation is especially helpful while studying geometry and topology.
If you have any suggestions, corrections or ideas, feel free to send an e-mail using the address provided below.
I just wanted to share it
It animates some cool homotopies and covering spaces
Does anyone know of a good way of book keeping this
say I have r points in affine n-space
all distinct
I want to write down generators for the ideal
call the kth point P_k=(p_{k,1},p_{k,2},...,p_{k,n})
By the ideal do you mean the ideal corresponding to the n points? In that case the ideal is generated by elements of the form: (x_i-p{k,i})(x_j-p{l,j}) where i,j,k,l range over all possibilities
yes
is this enough?
i would have thought we needed all the coordinates
for example if we have 3 points in A^3
by this (x1-p11)(x2-p22) is a generator
but this does need not vanish on P3
Oh wait it should be intersection of ideals not products, damn. Well in that case i can’t see a nice way to get the generators.
Sorry I got a bit mixed up.
Ah wait nevermind, since all the maximal ideals are coprime the intersection is the product. So instead of a product of 2 generators, take a product of all r generators. Concretely: a_1a_2…a_r where each a_i is of the form x_l-p{i,l} for some l should be a generating set (when you take all possibilities for l)
okay thanks
No answers? TT_TT
Hint: if such a V existed, writing V as a union of B_i = {i} union B((i,r_i),r_i) for each irrational i (any other basis elements in V can be removed WLOG), then any rational q will be a limit point of {(i,r_i)} in the standard topology of R^2.
Actually I'm not sure if that will prove anything, nvm
Yeah. I can construct disjoint open sets U and V such that U contains (0, 0) and V contains all other points on the X axis. If your method of proof worked, it would also probably contradict this counterexample.
right
I feel like you could do something by induction. Take the basic set in U containing (0,0). That would have some finite radius which will allow you to choose an irrational close enough to 0 that its basic set in V has its radius bounded by 1/2. Then take a rational close enough so that its basic set in U is bounded by r/4 and so on. This should be a convergent sequence in R, and its limit should have its basic set bounded by every r/2^n
This kind of construction doesn't work, I think.
For any distjoint sets A and B that are subsets of the X axis, if A and B are countable, then a construction similar to that results in open sets U and V such that U contains A and V contains B.
Mine uses density of both the sets
Basically, order the points in A and B somehow, and for each of the point, choose a circle that's small enough that it doesn't overlap the previous points in the order.
oh
This only works for countable sets, and breaks down on the irrationals.
So I suspect that there isn't similar construction for the rationals and irrationals
@reef shore I'm actually not sure I understand your construction.
Are you trying to prove by contradiction that the two open sets can't exist?
yeah thats what I was trying
I am taking alternating between taking rationals and irrationals. Lets say the basic set containing (0,0) has radius r. Then pick any irrational x with |x-0| < r, so the basic set containing this must have radius < r/2, then pick a rational at distance < r/2 from this, and that must have radius < r/4 and so on
Oh. Wait. Lemme think.
That might work because that produces a series of numbers that must converge to something either rational or irrational.
Probably.
yeah that's what I am thinking but I am failing to see why this doesnt prove that the construction doesnt work for countable dense sets
And this convergence thing is what's missing from the countable sets thing.
oh I think I see it
right
yeah that limit point will be close enough to everything in the sequence to put a bound of 0 on it
Lemme try to formulate this properly...

(loading icon here)
So... start with (0, 0) is in the circle with radius r. Now we look at an irrational number between 0 and r/2.
Actually, let's just use an irrational number between 0 and r/4. So (x, 0). The radius of the circle there must be no more than r/2.
I think choosing one between 0 and r also gives a bound of r/2 
sure lol,
Let's say the new radius is s. (s < r/2).
Pick a rational number between x and x-s/4. The circle there has radius no more than s/2.
Repeating this results in a series of ever-shrinking circles. And since we switch between going left and right, and the steps keeps getting shorter, the tangent point of the circles must converge to something.
Something something contradiction. Good enough for me lol
There are a few more annoying details that I'm not gonna bother dealing with.
Oh right, doesn't even need to alternate since it's bounded by a geometric sum.
yep

Can anyone point me towards resources to help me tile a sphere with polygons?
Basically I want to do something similar to spatial partitioning but in a spherical domain. I am looking for the simplest way to achieve this but the internet indicates me(a math noob) I should give up. The only divisions I think I can do right now is dividing sphere surface into n wedge surfaces but its not the best division for my purposes.
Any suggestions?
They're not, B is shaped like a cross and D is a single curve
proof by picture
oh wait
B is not cross
yeah I was reading A for some reason
Projection should be a homeomorphism
45 degree projection
of D onto B
(1,1)
(0,c) should go to wherever the line x+c=y intersects xy=1
(c,0) wherever x-c=y does the same
I still not get the projection function ....
Or I think easier way would be to translate D so that (1,1) is on (0,0)
Then D looks like some stuff in the second quadrant and some stuff in the fourth
project the stuff in the second quadrant onto the y axis and the stuff in the fourth quadrant onto the x axis
How there any stuff in 2nd and 4th quadrant ? D is a curve in first quadrant...
Yeah break it apart into the 2 pieces, projection on each thing is a homeomorphism, then use pasting lemma to say that the pasted function is continuous 
ok even easier solution lol
B is homeomorphic to R because just bend the positive y axis onto the negative x axis
so (x,0) -> (x,0) and (0,y) -> (-y,0)
and D is homeomorphic to the positive x axis by projection
positive x axis is homeomorphic to R
just appeal to classification of connected topological 1-manifolds smh
the solution i had in mind was basically the same thing 
one's the graph of a continuous function on (0, \infty) so it's homeomorphic to that, and one's homeomorphic to R by fixing one half and rotating the other. and R and (0, \infty) are homeomorphic
your idea is geometric and nice though


I was new......
What is pasting lemma...
it pastes
i used it the other day 
What is "classification of connected topological 1-manifolds"
it's exactly what it sounds like
list out all connected topological manifolds of dimension 1 up to homeomorphism
If you have 2 continuous functions defined on 2 closed sets U and V respectively and they agree on the intersection, you can paste them to get a continuous function on the union
(i.e., give a list of connected topological manifolds of dimension 1 such that no two are homeomorphic, and all (previous adjectives) 1-manifolds are homeomorphic to one on the list)
for connected 1-manifolds the distinct four are [0, 1], [0, 1), (0, 1), and S^1
I like how you wrote (previous adjectives) instead of "connected"
repeating myself gets annoying
true,true
what is there except n circle glued together , R, the long line and other longer stuff in the same spirit of the long line (except if you enforce countable basis, in which case the long line and longer stuff doesn't count as manifolds ?) ?
you can do it for the empty boundary ones using some simple riemannian geometry
edges of a cube dont give a 1-manifold 
yeah the circles glued together don't either
3 edges meet at a point
oh and then this point can't have a neibrd homeo to R ?
yeah right okay
ok so what is there except R and a closed segment
tteppa already said the 4 
.
oh right
then I had all of them except [0,1)

and other stuff
that aren't manifolds
:pepega:
3/4th a geometer, and a little bit of something else
pick a riemannian metric g on M. consider a point of M and a maximal unit speed geodesic emanating from the point. you can prove that this has to be onto using a connectedness argument. it's also not hard to see that the geodesic is a local isometry. if it's injective, then M is isometric to the open interval on which the geodesic is defined. if it's not injective, then it's periodic and hence isometric to a circle
roughly

I agree with ultra here.
I agree with Moldilocks here
I agree with myself here.
i wonder if you can modify this argument for the manifolds with nonempty boundary
probably
I have a question about the standard proof of Brouwer's Fixed point theorem using homology, with the statement of the theorem as follows:
Suppose $f:D^n \rightarrow D^n$ is continuous, then it has a fixed point.
The proof i'm talking about is the one where you suppose by contradiction, then construct a retract onto $S^{n-1}$ by considering the intersection of the line spanned by $x,f(x)$ with $S^{n-1}$. My question is, it seems that $f$ must be continuous for this retract to be continuous, but I don't see exactly why this function must be continuous.
ShiN

Uh do you mean why the retract is continuous?
yes
more, how do you show that it is continuous
well if it wasn't continuous you couldn't call it a retraction
Try writing it out explicitly ig
it's in the name, retract, ct means continuous here
lol
Haven't proven that it's a retract yet









I'm so bad with analytical geometryt
but in essence parametrising it should be the same in any dimension right
I mean it’s AT you just picture it and say it’s obvious
clearly
x + t(f(x) - x)
yea that's what I thought
ok you know what, I think i'll skip proving that it's continuous
I mean it's easy to see
a true topologist

soo that's how we're supposed to do topology
anyways just find t that makes |x + t(f(x) - x)|^2 = 1 and you have th map
wow that makes everything so much easier
it should be straightforward
i think nothing in ag has ever been proven
people just assume someone before them made it rigorous
@swift fjord here's an actual idea. $|x + t(f(x) - x)|^2 = 1$ if and only if $$|f(x) - x|^2t^2 + 2\langle x, f(x) - x \rangle t + |x|^2 - 1 = 0.$$ the leading coefficient $|f(x) - x|^2$ is always non-zero by assumption. by the quadratic formula, to show that the root $t$ (and thus the point on $S^{n-1}$ obtained by the line from $x$ through $f(x)$) depends continuously on $x$, it suffices to show that $$ \langle x, f(x) - x \rangle^2 - |f(x) - x|^2(|x|^2 - 1) > 0 $$ when $|x| < 1$
TTerra
(or >= 0, whatever)
maybe it's geometrically obvious that this thing should have a root and that this is a silly thing to check
but if you actually wanted to be sure of continuity without writing down an explicit formula for the retract, this would probably work with minimal pain
tl;dr the quadratic formula ensures continuity
moldi pls one up me with a real argument
ok fine having a root is geometrically obvious, the quadratic formula ensures continuity, now apply homology qed
i mean that seem quick enough (the root part follows from cauchy swartz)
You could also say that given any epsilon neighborhood on S^(n-1) around the image of x under this function, contains the image of some delta neighborhood of x. For this, you can find a delta_1 small enough such that delta_1 balls around x and f(x) are such that any line going through both in the right order lands in that epsilon neighborhood (visually obvious, can probably prove) and then you can take a delta small enough so that the delta ball around x lands inside the delta_1 ball around f(x)
Then take min(delta, delta_1)
g&p has a proof of continuity iirc
or am i thinking of a different book
can't believe these geezers copied me
Maybe i'm dumb but I don't see where this argument uses the continuity of $f$
ShiN
Last line
Hyperbolic geometry
I was trying to show in $\mathbb{H}$ -Poincaré half-plane model- that hypercycles defined for a given line $l$ and a given $a$ in $\mathbb{R}$ as $$H(l)={z \in \mathbb{H} : d_{\mathbb{H}}(z,l)=a } $$
are not lines.
To prove something I tryed to argue that given that $Mob(\mathbb{H})$ acts transitvely on the lines of $\mathbb{H}$ I can find the hypercycles of the imaginary axis and via the $\gamma \in Mob(\mathbb{H})$ that maps my line in the imaginary axis i can state $$H(l)=\gamma^{-1}(H(\gamma(l))$$
Where I'm using the fact that a Möbius transformations preserves distances. At this point I defined [already here i have doubts] $d_{\mathbb{H}}(z,l)$ for a given $z \in \mathbb{H}$ and a line $l$ as the inf of the distances $d_{\mathbb{H}}(z,w)$ with $w \in l$.
Given this and the general assumption $z=a+bi$ and $w=ki$ i'm left with trying to calculate the inf of $$arccosh(1+\frac{|a+(b-k)i|^{2}}{2bk})$$.
Is any of this correct? There is any "distance from a given point to a given line" standard formula in hyperbolic geometry? Thanks for any help and hint.
Stephen
@gritty widget idk how much it helps, but hypercycles based on the imaginary axis in the half-plane model are rays of the form y = mx with m real and nonzero
But how do you know it? @west spindle
do you want the honest answer or an attempt at a mathematically sound answer?
The second one
alright
To you think deriving the expression that i found might lead to something?
so you have $\min_{k>0} \cosh^{-1}\paren{1 + \frac{|a + (b-k)i|^2}{2kb}}$
Yes imho this is the general distance
Ann
And i defined distance as the inf
that's the formula for the distance between two points in the upper halfplane model
we might want to focus on minimizing $\frac{|a + (b-k)i|^2}{2kb}$ instead since the function $x \mapsto \cosh^{-1}(1+x)$ is monotone
Ann
so we have $\frac{a^2 + (b-k)^2}{2kb} = \frac{a^2 + b^2}{2b} \cdot \frac{1}{k} - 1 + \frac{1}{2b} \cdot k$
Ann
this is just algebra. do i need to go into detail here?
Ok the monotone thing makes it clean
yes it does
I hope i would be able to end from here
you can take the derivative of this wrt k and find the minimum that way
Hoping it gives the wanted results
i believe you'll find that it is a function of (b/a)
b/a are fixed it's fine
yes i know
it'll just prove my point that equidistants based on the line x=0 are rays at non-right angles to the absolute
for that matter, equidistants centered around other lines are circular arcs which intersect the absolute at non-right angles.
I feel kind of weird about this
with some small conditions we can make a statement like
almost all smooth functions are morse functions
but its still a pain to check if a random function is actually a morse function
is there must be some nice trick like, if we have a family of smooth functions parameterized by some continuous thing then at there are only finitely many non morse functions in the family
this statement is obviously not true
but it just feels so weird that they are everywhere but hard to check
Im not sure about the definition of distance from a point to a line but it should agree with what im doing
As lines are geodesic
So this is the exercise that I'm working with: if f: X_1 -> X_2 is a homeomorphism of locally compact Hausdorff spaces, show f extends to a homeomorphism of their one-point compactifications. What does it mean for a homeomorphism to extend to a different homeomorphism?
MaxJ (Sockoist) ✓
Compile Error! Click the
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(You may edit your message to recompile.)
thats ugly
okay anyway
you want to show that there is a homeomorphism
form X_1* to X_2*
such that
when you restrict the map to the subspace X_1
you get the original homeo
does that make sense?
so like a homemorphism g
such that g(x)=f(x) whenever x is in X_1
so for all but one point in this specific instance
hmm but how can I get the original? So the restriction will be like f: X_1 -> X_2*, but this can't be a bijection since X_2(star) is "one point" bigger than X_2?
oh
you get the original when you restrict to the original space
yeah
so you want a homeo g between their one-pts
that restricts to a homeo f between the original spaces
so the property that this morphism "extends" is a certain factorization property for the canonical inclusion X->X*
(this isn't exactly a normal extension problem since the target changes)
okay so I am restricting both the domain and range?
ahh
it's not asking for the restriction to be a homeomorphism of X_1* to X_2
or X_1 to X_2*
sorry
yeah okay I see I think. So the image will be X_2?
yes
Okay great, thank you so much!
any good differential topologists here?
If I have a perfect morse function
you don't need to worry about the gradient flow lines to compute the homology
its just done from the indices of the critical poitns
ping dami for morse theory help

will they mind?
probably not. the only people i can think of who probably know morse theory past the first 3 sections of milnor are dami and brofibration
@honest narwhal i would like to summon you
What's up
Lol I don't actually know shit in Morse theory but I'm down to struggle with you guys a little bit
Im working through the calculation of the cohomology of the complex grassmannians
it actually ends up being pretty slick at the end
oo
free groups of size counting schumber sells
Don't interrupt
I'm deleting it lol
okay but what i am confused about is
Sorry, tought here you could ask
With more liberty
From now on if you see a conversation happening
Don't frickin blow it up lol
Wait your turn
Got it?
there is a section that goes through calculating the gradient flows of the morse function
but
we also show that it is a "perfect morse function"
What's perfect here?
and by this we mean all the critical points have even index
Ah
so then we you make the homology complex, the odd degree things will vanish
(this tells you why CPn does have cohomoloy in odd degrees)
Oh I guess that makes sense in hindsight
doesnt
but then i don't see why they calculate the gradient flows
maybe its just there for completion?
Maybe? What are you working out of?
Lectures on Morse Homology
(I might give a talk on this after I figure it out if anyone would be interested)
yes
i would
Very much down. But yeah lemme read that bit
i read the first few sections of milnor and loved it so i'd be down
guys for hyperbolic Geometry questions here is my best spot?
Yeah I got it, I'm waiting for the signal
fire away
I will paste as is a latex one okay?
I was trying to show in $\mathbb{H}$ -Poincaré half-plane model- that hypercycles defined for a given line $l$ and a given $a$ in $\mathbb{R}$ as $$H(l)={z \in \mathbb{H} : d_{\mathbb{H}}(z,l)=a } $$
are not lines.
To prove something I tried to argue that given that $Mob(\mathbb{H})$ acts transitvely on the lines of $\mathbb{H}$ I can find the hypercycles of the imaginary axis and via the $\gamma \in Mob(\mathbb{H})$ that maps my line in the imaginary axis i can state $$H(l)=\gamma^{-1}(H(\gamma(l))$$
Where I'm using the fact that a Möbius transformations preserves distances. At this point I defined [already here i have doubts] $d_{\mathbb{H}}(z,l)$ for a given $z \in \mathbb{H}$ and a line $l$ as the inf in k of the distances $d_{\mathbb{H}}(z,w)$ with $w \in l$.
Given this and the general assumption $z=a+bi$ and $w=ki$ i'm left with trying to calculate the inf of $$arccosh(1+\frac{|a+(b-k)i|^{2}}{2bk})$$
EDITED FROM HERE TO SHOW MORE WORK:
given that arccosh is a monotone function i need to find the inf of $$\frac{a^{2}+{b}^{2}}{2bk}+\frac{k}{2b}-1$$
taking the derivative I'm looking to the zeroes of:
$$\frac{-2a^{2}-2b^{2}+k^{2}b}{2bk^{2}}$$
solving and remembering that i need $k>0$ i get $k=(\frac{2(a^{2}+b^{2})}{b})^{\frac{1}{2}}$
looking now for the $a+bi$ such that for a given $p$ we have:
$$ d_{\mathbb{H}}(a+bi,(\frac{2(a^{2}+b^{2})}{b})^{\frac{1}{2}}i)=p $$
expanding this i got an expression of $z,z^{*}$ that is not a standard form for a line in the plane and it should end the exercise.
Is any of this correct? There is any "distance from a given point to a given line" standard formula in hyperbolic geometry? Thanks for any help and hint.
Stephen
If anyone knows any reference for this problem
In book or any hint i would very much enjoy. Can't seem to find any answer
did you ask this already?
Yes
did you try asking on stack exchange?
Yes
can you link to your post?
Thank you for helping
Hahaha
Which page ish?
Is it chapter 8? The bit in chapter 1 isn't giving much deets lol
Ah 8.6?
Yeah so in the next section he does just state that since the Morse function is perfect you just need to count cells in order to compute homology
I'm guessing the point of computing gradient flow was some mix of completeness and possibly to understand the unstable manifolds (which is a task that one can care about from a purely dynamical systems pov, not just in service of algebraic topology)
@gritty widget that's my guess
opps sorry was getting food
yeah i think you are right
this probably belongs in baby linear algebra but
permutation matrices are in U(n) because they are similar to the identity matrix
Uh
No matrices are similar to the identity matrix
Rows of an ONB are just the standard basis but in some different order
Which is still an ONB of C^n
@gritty widget
cf
identity matrix in shambles
what is the most appropriate laugh react
hey need help with a question


