#point-set-topology

1 messages Ā· Page 29 of 1

languid patrol
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Like if p is distance d from the boundary

odd flame
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it's the d that's important

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sorry too easy (i am a 7 year old trapped in a college student's body)

languid patrol
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Then just declare p \to q and points P of distance x from p move as P \to P + (q - p)*(1 - x/d) if q is further from the boundary than p.

silver umbra
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i think the intended method here wouldnt involve passing to a metric on the space

languid patrol
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I mean why not? You have to write down a function somehow.

silver umbra
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namely, we havent proved that all manifolds are metrizable yet

languid patrol
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You don't need a global metric

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We're doing this locally on a chart

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The fact that the euclidean n-ball is metrizable is much easier to prove.

silver umbra
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sure so we're working in the Euclidean n-ball

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and the function u give is a homeomorphism fixing the boundary and sends p to q?

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first of all how do we compute d

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the distance of a point to the boundary

languid patrol
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You don't need to compute it.

odd flame
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i'll be back w more questions when pdk is done catthumbsup but thanks again

silver umbra
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then d = 0

languid patrol
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x is not a point it is a number

silver umbra
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wait what

languid patrol
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P is a point in that formula and d(P, p) = x

silver umbra
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oh

languid patrol
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Anyway the idea is:

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Take a small disc around p which doesn't contain the boundary and such that the radius of the disc is less than the distance from q to the boundary

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(you don't care how big the disc is, the only important thing is that it exists)

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Call this disc D.

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D has radius r

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Actually here's a better way to do it

silver umbra
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mhm

languid patrol
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So take a homeomorphism from the interior of the disc to R^n

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then p, q map to two vectors in R^n

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So if this homeomorphism is \psi, we do P \to \psi^{-1}((\psi(q) - \psi(p)) + \psi(P))

odd flame
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ohhhhh i kinda see why my question before was true

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those regions in the equator are just being divided into four regions

languid patrol
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the result is that we push p to q, then the only thing left to do is to use a linear decay function to make sure the homeomorphism fixes the boundary.

odd flame
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did that post

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oh there it is

silver umbra
languid patrol
silver umbra
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so psi is some artbirary homeomorphism from D to R^2

languid patrol
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If your manifold is 2-dimensional, yes.

silver umbra
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sure, let's reduce the case to surfaces

languid patrol
languid patrol
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Then we use the vector space structure on the target to just translate from one point to another

odd flame
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yeah i see the general idea now i need to squeeze MV in there too

languid patrol
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So this gives a homeomorphism on the open disc D which takes point p_1 to point p_2

odd flame
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sorry i'll let you finish that other q tho

silver umbra
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gotcha, i see what's going on here

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the vector space structure on R^2

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makes it possible to do these translations easily

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and represent them by just adding vectors

languid patrol
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Yeah, really it's just a dumb hack so you don't have to write a bunch of coordinates.

silver umbra
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sure

languid patrol
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So anyway once we've done this and we get our homeomorphism f on some open disk U, we fix an \epsilon > 0, for points of distance 1 - \epsilon or less from the center of U, g(x) = f(x), however for points x of distance d >= (1 - \epsilon) we define g(x) = f(x)*(1-d)/\epsilon+ x(d - (1 - \epsilon))/\epsilon

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This looks like an annoying mess but all this is doing is dampening the effect of the homeomorphism as you get closer to the edge of the disc, that way the boundary is preserved

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We're picking a ring of width \epsilon around the outside of the disc and decreasing the effect of the homeomorphism as you go further out along that disc

silver umbra
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hmm ok

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i'm trying to think of how to prove that this is a homeomorphism

languid patrol
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Well let's just think about the same problem but in R^n since we're in that context

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We want to construct a map from R^n \to R^n which is a homeomorphism, takes p to q, and does nothing for points very far away from the origin.

silver umbra
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sure

languid patrol
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Ah wait here's an even better way, which is really obviously a homeomorphism with no work

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Take the midpoint of p and q and rotate around it, but rotate points less and less as the distance from the midpoint changes from |p - q|/2 to N, where N is sufficiently large.

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This actually switches p, q which is kind of neat.

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So wolog (p - q)/2 is the origin

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Then let R(\theta) be a family of rotations by angles \theta around the origin such that R(\pi/2) takes p to q and vice versa. Then we do f(P) = R( (2(N - |P|)/|p - q|) * \pi/2) when N>= |P| >= |p - q|/2, f(P) = R(\pi/2) if |P| < |p - q|/2, and f(P) = P if |P| >=N

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This one is clearly bijective since you can just rotate back. And it's very easy to check that it's continuous since it's clearly continuous on each region where it's piecewise defined and it matches on the boundary.

silver umbra
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ok so R(theta) is counterclockwise rotation by angle theta

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what is N here?

languid patrol
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Sure in 2-dimensions yes

silver umbra
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yeah lets just reduce all of this

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to two dimensions

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for simplicity

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what is N here?

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also why is it ok to take the midpoint of p and q to be the origin

languid patrol
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N is just some very large number

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Arbitrarily large

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Just a big distance from the origin, and outside the sphere of radius N we want the homeomorphism to be trivial

silver umbra
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um

languid patrol
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If you like just replace "the origin" in what I said with "the midpoint of p and q" if it makes you uncomfortable.

silver umbra
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wait so is this map defined on the closed disk? or R^2

languid patrol
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I'm defining it on R^2

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But the point is that because it is trivial outside the sphere of radius N, that means that when we translate back to the disc, it will be trivial outside of some open subset of the disk which doesn't touch the boundary.

silver umbra
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but how are we translating back to the closed disk

languid patrol
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We're defining a function on the interior of a disk, which is trivial near the boundary

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so that function can be glued with the identity on the boundary to make a function on the closed disk

silver umbra
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but how is triviality near the boundary defined for a function on R2

languid patrol
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(trivial meaning is the identity)

silver umbra
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like doesnt it depend on what homeomorphism we choose from the open disk to R2

languid patrol
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Not really, being trivial "outside a compact set" is well defined for any homeomorphism

silver umbra
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i think this description is going over my head a little bit; would it be hard to prove that the previous map u suggested is a homeomorphism

languid patrol
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Like it makes sense on both sides, on the R^2 side that means outside some disk of radius N, inside our open disk thats some wobbly looking compact subset.

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I dunno none of it is hard, but you might find it easier if you construct your own function inspired by this method.

silver umbra
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i mean its not hard viewing it from a purely visual high level perspective but getting down to it and trying to like

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actually find the inverse

languid patrol
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The method being: do whatever you want inside some open disk, then make it trivial outside of some compact subset by continuously reducing the effect of the homeomorphism.

silver umbra
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espcially when ur dealing with distances and stuff

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kinda hard

languid patrol
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The nice thing about the rotation one is that the inverse is explicit.

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Since it's just rotating back basically.

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I wouldn't calculate out the distances explicitly, that's a waste of time. Just write dist(blah, blah)

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The distance function is obviously continuous so any expression involving it and other continuous functions will also be continous.

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No need to write any square roots

silver umbra
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sure but its not continuity thats the issue

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its trying to find the inverse

hallow moss
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my homework asks that I classify the alphabet into homeomorphism classes surely I do not have to find an explicit homeomorphism right?

silver umbra
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like the previous suggestion u gave, how would one even try to go about determining the inverse of that map explicitly

languid patrol
silver umbra
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the translation one

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the inverse in the interior is obviously easy

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but when u start like massaging it so that it becomes trivial toward the boundary

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what even is the inverse

languid patrol
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Yeah I think you have to be more careful about the way you massage it than what I described, the nice thing about the rotation one is that the massaging can be expressed cleanly in terms of distance from the midpoint.

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Like I suspect what I described takes even more mess to turn into a real solution, whereas this rotation one just works.

rapid lagoon
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Excuse me for barging in, but I have a question regarding this problem, specifically 4b. Specifically, I am really not sure how I would construct a "smallest unique topology that contains all of T_alpha"

silver umbra
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also what exactly do u mean by N sufficiently large

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like N sufficiently large for what

languid patrol
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Just N larger than say 2|p - q| suffices, it doesn't really matter beyond that

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You just don't want to make the cutoff so small that it gets in the way of what you want to happen with p and q.

silver umbra
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im also very confused

silver umbra
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R is rotations such that rotating by pi/2 sends p to q?

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im not understanding what that even means

languid patrol
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Yep, so it's rotating around the midpoint of the line between them

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If you rotate by pi/2 you switch them, if you rotate by 0 degrees, you leave them alond

silver umbra
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would maybe reducing to the case that, say q = 0

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and the disk is the unit disk

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make any of this easier

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im just having a very hard time visualizing rotations about lines between points and stuff

rapid lagoon
gentle ospreyBOT
languid patrol
silver umbra
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but i cant just take fixed p and q

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then the whole problem is moot

languid patrol
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Yes

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Which is why I didn't make any particular assumptions about p, q.

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I thought you were asking for intuition, but to write it up you have to describe an arbitrary pair of points. Taking p to be the origin or something doesn't make anything simpler imo.

languid patrol
rapid lagoon
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Ah!

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Thats really neat! Thanks!

languid patrol
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No worries.

hallow moss
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bruh I just drew pictures for some of those alphabet things

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if i get points off for no explicit homeomorphism im gonna die

languid patrol
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I think that's fine

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I dunno it depends on your TA, but it would be ridiculous to expect you to write down coordinates for all the letters

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Just like some would say it would be ridiculous to stress too much about writing an explicit homeomorphism on the disk in enough detail šŸ˜‰

willow viper
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hello how can I start proving the first direction?? I know that f closed means that for all U āŠ† X closed there exists an f(U) āŠ† Y closed?

abstract saffron
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If my memory is of any use, f is closed if it maps closed sets to closed sets.

willow viper
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Is my definition different?

abstract saffron
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It follows from two things, $f(\overline{A})$ is closed, and $f(A) \subseteq f(\overline{A})$.

gentle ospreyBOT
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Megumi_Tadokoro

abstract saffron
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Then $f(\overline{A})$ also contains the closure of $f(A)$. QED

gentle ospreyBOT
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Megumi_Tadokoro

abstract saffron
willow viper
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maybe.. I tried to write it out to make things easier maybe

rapid lagoon
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sidenote, but topology is genuinely kinda nice

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beats real analysis

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XD

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real analysis, more like applied liminf and limsups amirite

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real analysis, more like applied topology XD

willow viper
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Oh Im dumb

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because cl(f(cl(A))) = f(cl(A))

willow viper
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Is the reverse direction then:
cl(f(A)) āŠ† f(cl(A)). So cl(f(A)) āŠ† cl(f(cl(A))) => A āŠ† cl(A), so A is closed.
Since A āŠ† cl(A) <=> f(A) āŠ† f(cl(A)). So f(A) is closed??

odd flame
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going back to this question

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for that last part about the homeomorphism is it enough to say that (1,0,0) has 1 line going to it in X and 2 in Y so it cannot be homeomorphic

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or maybe better that removing a nbhd of (1,0,0) will make X and Y deformation retract to different spaces

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X to like a disk with a cross up the middle

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but disk deformation retracts to a point so just the cross?

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and im p sure Y deformation retracts to a circle when such a nbhd is removed

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walter button :(

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,av walter

gentle ospreyBOT
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walter#1555's Avatar

Click here to view the image.

odd flame
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this needs to be an emote

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different question - how is this obvious

fading vale
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f induces a homeomorphism on the pairs of spaces

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alternatively take the maps induced on the long exact sequences of the pair and apply the five lemma

odd flame
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is that what you meant?

odd flame
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still curious

coarse night
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you know what five lemma is?

odd flame
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i looked ahead in hatcher

coarse night
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it's actually one lemma but called 5 lemma bleakkekw

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misnomer

odd flame
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classic

coarse night
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anyway given you have a homeo, X → Y you also have homeo X-x to Y-y which gives the maps
Hn(X-x) → Hn(X) → Hn(X, X-x) → Hn'(X-x)→Hn'(X)
|| || |? || ||
Hn(Y-y) → Hn(Y) → Hn(Y, Y-y) → Hn'(Y-y)→Hn'(Y)

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? now becomes an iso by S5L

odd flame
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so it's just

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automagical

odd flame
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f being the homeomorphism between X-> Y

coarse night
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yes

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that was implied

odd flame
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silly question but

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n' is n-1?

coarse night
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also yes

shadow charm
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Really don’t need 5-lemma here though šŸ¤”

coarse night
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wasn't enough space

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at least that's what I thought

shadow charm
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Homotopy equivalence of paire gives isomorphic relative homology, and in this case you have a homeomorphism of pairs (X\x maps homeomorphically through f to Y\f(x))

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Okay I should’ve read through your full answer didn’t realize you were justifying why it induced an iso on relative hom

odd flame
coarse night
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yes

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if you have seen excision

odd flame
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reading back rn

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what's the point of considering pairs of spaces like this

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actually is excision "part of the point"

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that's probably a really vague question bleakkekw

odd flame
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now i have this fun lil guy tho

odd flame
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wait wroong thing

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i'll just repost in case anyone is around

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intuitively i can see why C and Y have the same sequence but ive been unable to do it properly

languid patrol
odd flame
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this is what i came up with after messing around w it w a friend

languid patrol
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Something you wrote there is impossible

odd flame
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i did write this at like 3am so i could be wrong

languid patrol
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This long exact sequence where you compute H_0(U) you have written H_0(U - {x})

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is Z/2

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but I think that is untrue since youve written that you have an exact sequence 0 \to X \to Z \to 0 so X must be Z

unreal stratus
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Inch resting

odd flame
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hmmm

languid patrol
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In general H_0 can never have torsion.

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Or no what am I saying.

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It is.

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\pi_0 is not.

odd flame
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hows that related

languid patrol
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It's not I was responding to something that was deleted

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From potato

unreal stratus
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Yeah my half awake brain said smth very stupid

odd flame
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im gonna switch to another MV question for the practice then

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i already did a and b

languid patrol
odd flame
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wait quoi

languid patrol
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I'm just saying in the previous problem

odd flame
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oh is that about the one with the two spheres?

languid patrol
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Yes isn't that what you were asking about?

odd flame
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oh i just realized i posted the picture bleak

odd flame
languid patrol
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I see.

languid patrol
# odd flame

Anyway yeah for part (c) what are you struggling with?

odd flame
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is the right approach to break down E into the sphere parts and line parts and then use what we know about H_n(S^2)?

languid patrol
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You should follow the approach outlined in the problem

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so just calculate the H_2 for the interval [-n, n] with spheres attached at the integer points, then take the limit as n \to infinity

odd flame
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slightly unrelated but what is d) hinting at? isnt pi_1(S1 v S2) nontrivial, making that hint not helpful?

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iirc that has fundamental group Z

languid patrol
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No but E is simply connected

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because E is the universal cover of S1 V S2

odd flame
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ohhhhh

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and universal cover has trivial fundamental group

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so the first nontrivial htpy group is pi_2

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so this means that pi2(E) \cong H2(E)...?

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and we get that H2 from MV sequence

nocturne basalt
languid patrol
odd flame
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and how do you get the MV sequence

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this goes back to my first question

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when i asked if you started from H0 and built up

languid patrol
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It goes H_2 (A \cap B) \to H_2(A) \oplus H_2(B) \to H_2(X) \to H_1(A \cap B) \to ...

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And the first map is injective when everything is 2-dimensional or less.

odd flame
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oh it just always has that form?

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oh i guess that's how it works for SVT too

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and the groups themselves just vary per each space

languid patrol
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Yes in general all long exact sequences on Homology or covariantly functorial algebraic topological objects should decrease degree, cohomological or contravariantly functorial objects will have long exact sequences in the opposite direction.

odd flame
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so the nested subspace thing in the outline is just a hint about how to make it X = A U B

languid patrol
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This comes from some general difference between the degrees in homological vs cohomological spectral sequences. Which is something that you won't understand now but perhaps later.

odd flame
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we do cohomology soon yeah

languid patrol
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So in our case A_n = [-n - 1/2, n+1/2] with spheres attached at the integer points

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B_n is say (-\infty, -n - 1/4) \cup (n + 1/4, \infty) with spheres attached at integer points.

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The intersection is just two line segments, which have no H_2

odd flame
languid patrol
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This will show you that the maps from H_2(A_n) to H_2(X) are injective

languid patrol
odd flame
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including the respective spheres ofc

languid patrol
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Because our space is R with spheres glued in at integer points.

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So i'm using the coordinates on R

odd flame
languid patrol
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Anyway so this is a somewhat trivial Meyer-Vietoris

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But then you have to do another Meyer vietoris (which is similar) to compute H_2(A_n)

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Alternatively you could just note that A_n is homotopy equivalent to a Bouquet of 2n + 1 spheres, and presumably you've already computed the homology of that in class.

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If not you can also use Meyer Vietoris for that.

odd flame
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we never really defined a bouquet

languid patrol
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Just like 2n+1 spheres glued together at a single point.

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It's usually important for defining homology to compute the homology of that space.

odd flame
languid patrol
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Yes just to compute H_2 of the entire space.

odd flame
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oh so it's still trivial then

languid patrol
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What do you mean?

odd flame
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have no H2

languid patrol
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The space has lots of H_2

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But yeah the intersections will have no H_2?

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So because the map H_2(A_n) \to H_2(X) is injective this shows that H_2(A_n) \to H_2(A_{n+1}) is injective since A_n \to A_{n+1} \to X factors the map to X.

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Then as your professor states if X = \cup A_n where A_n \subset A_{n+1} and the map H_i(A_n) \to H_i(A_{n+1}) is injective, then H_i(X) \cong \lim_n H_i(A_n)

odd flame
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(i'll brb, relocating)

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ok i think i see the MV stuff

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how does it give us this

languid patrol
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Because we just computed H_2(E) by hand

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and showed that it was Z^{\oplus \infty}

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Since \pi_1(E) is obviously zero (E is homotopy equivalent to S^2 V S^2 V ...)

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By Hurewicz or whatever it's called this means that H_2(E) = \pi_2(E)

odd flame
coarse night
languid patrol
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Or are you asking a question?

novel acorn
novel acorn
gentle ospreyBOT
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Irony Incarnate

novel acorn
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which also holds in the basepoint preserving case

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and in that case we have $[(S^1,x), (S^2,x)]^0 = \pi_1(S^2, x) \cong 0$

gentle ospreyBOT
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Irony Incarnate

novel acorn
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which then implies that $[(S^1 \times S^1,x), (S^2,x)]^0 \cong [S^1 , 0]^0$

gentle ospreyBOT
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Irony Incarnate

novel acorn
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which is just the trivial map

coarse night
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But that’s not true

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You can always collapse the 1-skeleton and get a nontrivial one

novel acorn
coarse night
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It’s not basepoint preserving but I believe you can make it basepoint preserving

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Idea is using cellular approximation

novel acorn
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I still don't get what exactly were talking Abt here anymore???

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Like collapse the 1-skeleton of what
And why?

coarse night
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so CW structure of S¹xS¹ is we have S¹vS¹ and a 2 cell attached by aba'b'. Now collapsing S¹vS¹ gives us a S² which is not nullhomotopiv

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That is send S¹xS¹ →S¹xS¹/S¹vS¹=S²

novel acorn
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Ahh wait

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I know where I messed up yeah

novel acorn
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Mine is correct as well

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It depends on how you look at the space

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If you look at it as a product of pointed spaces

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Then you get a smash product

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But if you look at the torus as a space with a point as a base point

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Then i think what i said holds?
Tho I'm not sure

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Actually no it isn't lol

languid patrol
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Homotopy happens on the source not the target.

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All maps from S^1 \times S^1 \to S^2 are nullhomotopic by definition (based or not).

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For instance the real numbers R have a quotient S^1, just as your space S^1 \times S^1 has a quotient S^1 \wedge S^1, this doesn't imply that there are nontrivial maps from R \to S^1 up to homotopy though.

unreal stratus
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What do you mean by "by definition" here

coarse night
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I just gave a nontrivial map

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why is that nullhomotpoic?

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can you explain

languid patrol
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Why is it nontrivial?

coarse night
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I'm asking why is it trivial

languid patrol
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I had actually made a mistake but I think it's still nontrivial to show that it's nontrivial

languid patrol
unreal stratus
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Sure

languid patrol
# coarse night I'm asking why is it trivial

I just don't see any reasoning you gave to show that it is non-trivial, there is a more canonical looking finite cover of the Sphere by the torus which is obviously nontrivial.

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I guess probably the way to do this is to calculate the map on \pi_2 by expressing the torus S^1 \times S^1 as a quotient of a square by identifying opposite edges, and the sphere as a quotient of the square by identifying the entire boundary.

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Then it's clear that the induced map on H_2 is nontrivial, so the map is not nullhomotopic.

coarse night
languid patrol
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As I mentioned above, I was confused.

coarse night
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okay

languid patrol
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And thought you were saying something incorrect.

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I still don't understand why it's related to the post that you posted this in response to.

coarse night
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It's not, just gave as an exercise

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I do that sometimes

languid patrol
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lol

coarse night
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in fact I believe the homotopy class of maps should be ℤ

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given by the degree of the map S² → S²

languid patrol
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Yeah, you can see this from the fact that the map on H_2 is just Z \to Z by the identity.

coarse night
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But I don't have a proof

languid patrol
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So, if I can redeem myself:

languid patrol
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Yes that is what induces the map

coarse night
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the whole idea was using cellular approx you get the 1-skelli of S¹xS¹ goes to a point in S² anyway as there's no 1-cell so you might as well look at maps from the quotient S¹xS¹/S¹vS¹ = S² anyway which gives the homotopy class to be Z

languid patrol
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Yes I think that's a good argument, perhaps worded another way: up to homotopoy, S^1 V S^1 has no maps to S^2, so any map from S^1 \times S^1 to S^2 is homotopic to one factoring through this quotient, and there are Z of those as you say.

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*homotopy.

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But the main point is that the canonical quotient map IS nontrivial, because this argument only makes sense if you actually produce one non-trivial map.

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For instance you could say the same thing about R mapping to S^1: certainly any map from Z \subset R to S^1 is homotopic to 0, but if the canonical quotient map isn't nontrivial the rest of the argument doesn't work.

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^This was the mistake that I thought you had made.

languid patrol
noble osprey
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Hi can someone give me a hint as to how to find the 4 boundary points. Thank you

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2a

compact stump
#

Suppose I have a closed hemisphere H āŠ‚ R³, then it's boundary āˆ‚H is the hemispherical shell. But intuitively, the upper hemispherical shell also has a boundary, which is the circle. How do I denote the circle in terms of H, even though technically the boundary of the hemispherical shell is itself?

coarse night
#

the are sometimes distinguished as the topological boundary vs manifold boundary

#

your "circle" here is manifold boundary

noble osprey
#

Yea, i got the shape but i dont get where the boundary points come from, in the picture.

nocturne basalt
noble osprey
#

yea sorry, I mean that I dont get where the coord (3,0) came from. Would it not be (0,2) since the radius is 2? I thought to use the circle equation, is that something I can do?

nocturne basalt
noble osprey
#

ah yes! i missed that point, thank you.

next crystal
#

what does it mean for a class of loops to generate a fundamental group?

plain raven
#

that every element in the fundamental group has a representative which can be expressed as the composition of elements in the class of loops, together with their inverses

quick bough
#

any hints?

#

i tried constructing such a J, but i came across a problem

#

so for every U_i, i can write it as a union of base elements, namely B_j with j \in N (since there is a countable basis), I choose the elements J to be the j such that U_{i_j} contains B_j. The problem now is that such a thing doesn't necessarily exist

novel acorn
#

A property of bases is that for any x in U where U is an open set, there exists a basis element B such that x in B subseteq U

#

So you can always choose such a U

opaque cloud
#

What more do you need for a topological space to be metrizable apart from hausdorff-ness? catThin4K

#

or are every hausdorff spaces metrizable?

languid patrol
#

The one point compactification of R (or any uncountable set) with the discrete topology is not metrizable.

#

(Because every compact metric space is separable)

#

(i.e. has a countable dense subset)

languid patrol
languid patrol
#

Yes, that's why I mentioned it

languid patrol
#

The one point compactification of a locally compact Hausdorff space is Hausdorff

paper wedge
#

hi

#

idk much topology

#

how do you attach a chain complex to a topological space X

unreal stratus
#

Uh you may wanna google singular chain complex

paper wedge
#

so u approximate it by simplicies?

#

and the map would be the boundary

#

cool

unreal stratus
#

Uhh approximate it by simplices is not really what you are doing

#

And "the map" lol

paper wedge
#

ig better is that ur forming a free group by just taking the vertices of ur simplex as the spanning set

unreal stratus
#

I would recommend just reading what this is lol

paper wedge
#

over X

unreal stratus
#

You aren't taking the vertices of a simplex

cedar pebble
#

well so if you have a triangulation of your space by simplices then you can build a chain complex from this triangulation and compute the simplicial homology from this

unreal stratus
#

Oky that too

#

Like there are a few different things here lol

cedar pebble
#

this is easier to think about than singular homology

unreal stratus
#

Yes sure

cedar pebble
#

where you are sort of looking at all possible ways of mapping in simplices at once which is a total mess

unreal stratus
#

I end up forgetting simplicial even exists

cedar pebble
#

yeah oops

unreal stratus
#

When do you even care about simplicial homology tbh like I have never used it to compute anything lol

#

Other than intro examples in Hatcher

cedar pebble
#

I mean this should basically just be cellular homology

#

you're just being picky about the sorts of combinatorial descriptions you're allowing for your space

unreal stratus
#

I imagine it's like usable for computers and stuff though

cedar pebble
#

but like morally these are seeing the same thing in the same sort of way

unreal stratus
#

Yeah

paper wedge
#

cool boys and girls

#

triangulation is easier for me yea

#

makes more sense

#

ty al

plain raven
#

One reason - computing the boundary map in cellular homology is harder than in the case of simplicial homology.

#

Even in homotopy theory it is very often useful to adopt a combinatorial perspective.
May wrote Simplicial objects in algebraic topology in 1960.
Goerss and Jardine wrote Simplicial homotopy theory in 1999.
Jacob Lurie wrote Higher Topos Theory in 2009.
Do you expect this to be the decade where we finally discard simplicial complexes?

#

I do not.

unreal stratus
#

Yeah Idk why I said that given I have used simplicial sets and stuff lol

plain raven
#

He probably meant connected.
But if the manifold is not connected, then each connected component will have a countable fundamental group.

golden gust
#

is there a name for the procedure (or final result) of gluing two copies of a manifold along its boundary?

umbral panther
#

Doubling / double

golden gust
#

thanks

solemn oar
#

If you are doing abstract homotopy theory you are far more likely to encounter simplicial sets and their associated simplicial abelian groups (which compute simplicial homology) than you are to encounter arbitrary CW-complexes.
The latter might be more common in manifold theory.

noble osprey
#

Hi, can someone explain to me in simple terms of open sets with different metrics. I cant seem to understand the sentence highlighted in terms of how the different metrics determine whether U is open or not? Thank you

paper wedge
#

open sets with different metrics

#

@noble osprey

#

an open set is a set where if you choose any point inside this set there is a ball around it that is contained inside the set

#

a ball of radius r centered at x is defined to be the set {y | d(x,y)<r}

#

if u change the metric the ball "sorta" changes

#

so u can have an set that is open wrt a metric abut is not wrt another metric

#

as the definition of the ball is different cuz the metric is different

#

do u get it

#

(this is all in the setting of metric spaces )

paper wedge
noble osprey
#

I get it thanks, so if the open ball had a radius r about (1,0) w.r.t the railway metric then the distance is 1 but from that point how do we go about determining if the open ball is open or not?

#

i mean if its less than r, but like how do we know?

paper wedge
#

how do we go about determining if the open ball is open or not? the open ball is always open under its respective metric

#

the point here is that under the railway metric this set IS the open ball

#

so its open by default ( u can try to prove it )

#

in general to determine if a set is open or not wrt a certain metric

#

it would be enough to show that all balls centered at some point of the set cannot be contained inside the set

#

for example consider [0,1] inside R with the metric defined to be d(x,y) = |x-y|

#

can u pick an element inside this interval and show no matter how small we choose our radius it still cannot be contianed in [0,1]?

unreal stratus
#

never heard of the railway metric lol

paper wedge
#

me neither

#

lmfao

#

i just trusted the text

unreal stratus
#

Oh wait no I did a question on it

#

But we didn't call it that lol

paper wedge
noble osprey
#

ahh so its not open since it would be outside [0,1]

paper wedge
#

what do you mean by "it" here

#

i know this shit is confusing

#

but u must understand it as its very important later on

noble osprey
#

like if we choose r such that 0-r, 1+r is outside [0,1] ?

paper wedge
#

whats 1+r?

#

lets recap

#

choose an element in [0,1]

noble osprey
#

yea, this open stuff is confusing

paper wedge
#

such that an open ball around this element can never be fully contained in [0,1]

paper wedge
paper wedge
#

all u need to make sure u know fully are the definitions

#

once u have the definitions it just takes time untill u get it

#

but u will never get it if ur definitions are fuzzy

#

u will always be confused

noble osprey
#

so i know the def of open ball

#

and i know that an open set contains an open ball

paper wedge
#

okay lets be more accurate

#

an open ball has a center and an eleement

noble osprey
#

but i dont get the metric part

paper wedge
noble osprey
#

yep

paper wedge
#

okay so

#

i want you to tell me

#

as accurately as yo ucan

#

the definition of an open set in some metric space X with a metric , call it d.

#

can u do that

noble osprey
#

a subset of X is open if there exists an open ball within that subset such that d(x,y) < r

paper wedge
#

hmmm

#

"within that subset"

#

its not quite

#

the word "open ball" is ambigious

#

what is its center

#

what is its radius

#

what are x and y?

#

a subset of X is open if for every element u can center a ball around it such that the ball is fully contained in that subset

#

so for example suppose u have some subset S

#

and this S is open

#

that means that for any random element

#

b for example

#

there must exist a ball centered around b such that the whole ball is contained

#

that is

#

there must exist some radius r; such that the set {a|d(b,a)<r} is a subset of S

#

better?

#

the set {a|d(b,a)<r} is called the ball centered at b with radius r.

noble osprey
#

oh wait, so an an open set is an open ball?

paper wedge
#

no, but for every element u can form an open ball around it

#

so more ilke

#

a union of open balls

#

something like that

#

best thing to do now is to do examples

#

lets take our set to be R , the real numbers and the metric to be defined as d(x,y) = |x-y|

noble osprey
#

ahh ok i get the definition

paper wedge
#

the usual distance

#

this is a metric space.

#

so now

#

answer this question:

#

how does the open ball centered at 2 with radius 4 look like

#

describe it as a set

noble osprey
#

a| d(2,a) < 4

paper wedge
#

yes

#

now

#

u missed something very small

#

or its just more pedantic really

#

but u should say {a is in R | d(2,a) <4}

#

cuz we are in R

#

at the end of the day right?

#

makes sense?

noble osprey
#

ahh yea, so if we are in R^2 then a belongs to R^2

#

makes sense

paper wedge
#

okay now

#

u can do go further now

#

this d(2,a) <4

#

can u unfold the definition?

#

u know what the metric is.

#

i defined it above

#

what does d(2,a) <4 mean

#

given the d i defined above

#

"expand" it

noble osprey
#

d(2,a) = |2-a| < 4

paper wedge
#

good

#

okay

#

so now lets look at extreme cases ig

#

from them we can understand a little bit better ig

#

u know what an open set is now correct?

noble osprey
#

yep

paper wedge
#

what isi t

#

what is an open set inside our metric space

#

define it for me

#

again

noble osprey
#

so an open set is when you take an element x , you have an open ball around that x which is the center of the open ball with a radius r such that d(x,y) < r

paper wedge
#

good

#

but

#

thing is that r could be anything

#

we cant choose it

#

the definition tells us that THERE EXISTS an open ball

#

idk how small or how large the ardius could be

#

but i know there must be atleast one

#

now lets look at this example

#

and i want u to prove or disprove that this set is open

#

for example

#

is the set {1,2} open in our metric space?

#

why or why not

noble osprey
#

Ok so this is what i dont get, if we are given a set we know that it has to contain an open ball in that set for it to be open. but with repect to the usual metric say, d(x,y) = | 1-2| < r i dont know how continue from here.

paper wedge
#

okay

#

so

#

we only have two elements right?

#

1 and 2

noble osprey
#

oh wait is it because d = -1 and its not in the set {1,2}

paper wedge
#

so can u form a ball around 1 such that the whole ball is contained in{1,2}

#

?

#

if u can do that for 1 and u can do that for 2 then that would mean this is open

#

if no matter what radius u choose , a ball centered around 1 would always contain an element other than {1,2} then this is not open

#

do u get it?

noble osprey
#

yea i think i get it, as long as its centred around 1 then if we pick a radius around r that still contains in {1,2} then it would be open? i guess

#

around 1 sorry

paper wedge
#

well try it

#

try to pick a ball

#

choose any radius u like

#

and see if its still contained inside this set

noble osprey
#

so if i choose u=2 then {1-2, 2+2} = {-1,4} is not contained in {1,2} ?

paper wedge
#

whats u

noble osprey
#

r sorry

#

radius

paper wedge
#

okaay so u want to look at the ball centered at 1 with raidus 2

#

so {y | |y-1| < 2} right?

#

this is your ball?

noble osprey
#

yes

paper wedge
#

now is this balll contained in {1,2}?

#

by contained i mean is every element of this ball an element of {1,2}?

#

if no then show me one

#

pick an element in this ball that is not an element of {1,2}

noble osprey
#

oh so {1,2} is an open set

#

yes i think

paper wedge
#

i want u to justify it for me

#

for {1,2} to be an open set there must be an open ball around 1 such that the whole open ball is in {1,2}

#

and as well as for the element 2

#

but lets pick in general any open ball around 1 with any radius

noble osprey
#

cos if we pick y=1,2

#

it would be in the ball

#

i guess

paper wedge
#

okay

#

so ur saying that

#

both 1,2 are in your open ball

#

rihgt?

noble osprey
#

yep

paper wedge
#

now are those the only ones in ur open ball?

#

are 1 and 2 the only solutions to the inequality |y-1| < 2 ?

#

what about y = 0

#

ur confusing the set definitoins

#

the condition is that

#

EVERY element of this ball IS AN ELEMENT of the set

#

so if ur set is just {1,2}

#

then ur ball's elements must CONTAIN either 1 or 2 or both

#

its a SUBSET of the whole set

#

but u know now that y=0 is inside your ball

#

so the ball around around 1 with radius 2 IS NOT a subset of {1,2}

#

because 0 is inside that ball but its not inside {1,2}

#

hence it is not a subset

#

do u get it?

noble osprey
#

0 would fail since it’s not contained in the ball

paper wedge
#

no

#

0 is not contained in the set

#

{1,2}

#

it is in the ball ( satisifies the condition ) but its not in the set

#

hence the ball is not contianed inside the set

#

contained*

#

do u get it?

noble osprey
#

Ahh so {1,2} is an open set with open ball around 1 or 2

#

But 0 is not contained in {1,2} so we can’t form a ball around 0

paper wedge
#

no

#

an open ball around 1 with radius 2 is not contained in {1,2}

#

do u see why

noble osprey
#

Because it’s not contained in the set {1,2}

paper wedge
#

yes

#

it has an element that is not in {1,2}

#

so that would only SUGGEST that it is not open

#

it would not show that is not open cuz that is just one ball

#

who knows if maybe we chose too big of a radius

#

do u get it?

#

to show that this is not open we would want to argue that for any choice of radius

#

an open ball around 1 would always contain an element that is not 1 or 2

#

remember that we are over the real numbers

#

that is alot of numbers

#

haha

noble osprey
#

Ahh so we always look at the end points 1 or 2 and form a ball around it

#

I get it now [tears]

#

I’m so sorry for being stupid and thank you for your patience haha

paper wedge
#

no need

#

u werent stupid

#

anyways

#

is the interval [1,2] open?

noble osprey
#

No because we can find an element that is not contained in the set {1,2}

paper wedge
#

not {1,2}

#

[1,2] is the closed interval

#

this is another problem now

paper wedge
#

u must mean that u can find an element such that there is no ball around that element contained in the set

noble osprey
#

Oh ok so what exactly is [1,2] ? Is that a subset of R ( real line) ?

paper wedge
#

its the interval

#

All real numbers between 1 and 2 including 1 and 2

noble osprey
paper wedge
#

yes

#

the dotts are the ball

#

And the center is 1

#

U can see no matter how we shrink the radius

#

It will always be outside the interval

#

No matter the radius

#

So its not open as for all radii ucant center a ball around 1 such that the WHOLE ball is contained in the interval

#

Got it?

noble osprey
#

Yup get it, does that apply to open interval as well (1,2)

#

I mean in this case the centre can’t be 1 or 2

#

I’m I right in saying that?

paper wedge
#

So what does that mean

noble osprey
#

Then it would contain within (1,2) thus it’s open

paper wedge
#

u got it

#

now notice that this depends on the metric choice

#

now

#

As for the finisher

#

lets now look at the same set but different metric

#

let it be the same set (R)

#

But define d(x,y) = 1 if x=y

#

d(x,y) =0 if x !=y

#

i want u to try examples with this metric

#

How does the open ball around any point look like? What are the open sets?

#

Good luck

#

this should answer ur original question on how like different metrics induce diff open sets

#

different*

noble osprey
#

In this case would it be open

next crystal
plain raven
#

Of course this is not actually function composition. But the term "composition" is common in group theory to refer to the multiplication of a group.

tulip bridge
#

Does someone have a visual example of cell decomposition, For example, if I was starting out with a disc from which two discs were removed (sort of like a torus but with 2 holes instead) how could I decompose that?

#

Then from that how could I think find the euler characteristic?

languid patrol
#

Okay sorry that this looks like it was drawn by a child, I did it with a trackpad

#

Here is a decomposition of your space with 8 vertices, 10 edges, and 4 faces.

languid patrol
#

The orange arrows are orientations

#

The green arrows indicate the orientations of the edges.

tulip bridge
#

Thanks! And no worries about the drawing, it helps a ton regardless. Do you mind describing how you went about doing it like that?

languid patrol
tulip bridge
#

Oh ok, my initial attempt was just straight across the middle with 6 vertices instead of 8, but I was unsure if it was necessarily ā€œcorrectā€

languid patrol
#

I think that should work as well afaik.

#

It depends on what you mean by cell decomposition. Sometimes there are extra rules if you want to compute simplicial homology etc.

tulip bridge
#

I mean I guess ultimately all the matters is I get the same characteristic, then they’re just homeomorphs of each other

#

Nah nothing that fancy

#

You had the right idea

#

My professor went at a snails pace so we didn’t get that far lol

languid patrol
#

Yeah, and in the end even that doesn't matter. For a "reasonable" space (i.e. anything that you can draw) you can just make the cells basically random and everything will work out.

#

In terms of computing homology or just the euler char.

pseudo coral
#

hey

#

for higher homotopy groups

#

all

gentle ospreyBOT
#

MyMathYourMath

pseudo coral
#

all

#

$\gamma:[0,1]^n \to X$ such that

gentle ospreyBOT
#

MyMathYourMath

#

MyMathYourMath

languid patrol
#

Yes, it is those things up to homotopy which fixes the boundary

pseudo coral
#

yes so all boundaries are x_0

gentle ospreyBOT
#

MyMathYourMath

languid patrol
#

The boundary of the image of \gamma is x_0

pseudo coral
#

yes

#

what i meant to say

languid patrol
#

but a homotopy is a map $H: [0, 1]^{n+1} \to X$ and it fixing the boundary means that $H(\partial [0, 1]^n \times [0, 1]) = x_0$.

pseudo coral
#

ok im doing a project on higher homotopy theory so i may be in this chat room a lot these next few weeks

languid patrol
#

ok

gentle ospreyBOT
#

Topos_Theory_E-Girl

steel glen
#

im not entirely comfortable with the construction of cohomology groups yet \
is there a general result we can get from $H_n(X) \approx H_n(A) \oplus H_n(X / A)$, given that $A$ is a retract of $X$ about the cohomology groups $H^n(X)$

gentle ospreyBOT
#

maximo

steel glen
#

im trying to show $H^n(X) \approx H^n(A) \oplus H^n(X / A)$

gentle ospreyBOT
#

maximo

steel glen
#

actually can i just use mayer-vietoris?

#

those are meant to be (X,A) not X/A sorry

chrome ridge
#

I am trying to show the bijection of isomorphism classes of covering spaces with isomorphism classes of $\pi_1(X, x_0)-sets$. I know that for any given a covering space we can get a $\pi-$set by considering the action of $\pi_1$ on the fiber $p^{-1}(x_0)$. Now I am trying to show bijection. In particular I am struggling with surjectivity. Any ideas?

gentle ospreyBOT
#

ru0xffian

nocturne basalt
thorn citrus
# chrome ridge I am trying to show the bijection of isomorphism classes of covering spaces wit...

I'm not sure there is a simple way to show the surjectivity.
Maybe the actual construction is needed.

For a given $\pi_0(X,x_0)$-set $A$, consider it as a discrete topology,
Let $Y$ be the set of all paths in $X$ starting from $x_0$, with a topology defined to satisfies
the map $\gamma \mapsto \gamma(1)$ from $Y$ to $X$ is locally homeomorphic.

Now my suggestion is:
take a quotient topology of $A\times X$ by the equivalence relation
$\gamma(1) ~ \gamma'(1)$, where $\gamma'$ is the path obtained by:

  1. first lift any element of $\pi_0(X, x_0)$, starting from the $(id, x_0) \in A\times X$,
  2. and then lift $\gamma$

I believe this construction might work, but please check it.

gentle ospreyBOT
fading vale
cedar pebble
#

moth use ur szamuely knowledge

fading vale
#

EVIL

#

demon

chrome ridge
cedar pebble
#

it may help to talk about the universal cover

fading vale
thorn citrus
#

Sorry for few mistakes in my writing.

Consider $(a, \gamma(1))$ and $(b, \gamma'(1))$ in $A \times Y$ whenever the following holds:

  1. There exists $g \in \pi_1(X, x_0)$ s.t. $ga = b$.

  2. Whenever you lift the a representative of $g$ to $A\times Y$ and then lift any element homotopic to $\gamma$ (with the same end point), the resulting path is homotopic to $\gamma'$.

gentle ospreyBOT
steel glen
thorn citrus
#

I think everyone are saying the similar strategy, but the actual construction might bother.
It's hard to me to remember the exact one.

fading vale
#

yes this is the quotient by the universal cover in question

#

you could also go via gluing which might be slightly more explicit

thorn citrus
#

Right

gentle ospreyBOT
fading vale
#

This has not been topologized yet, to be clear!

gentle ospreyBOT
fading vale
#

Ok tbh im realizing I dont know quite how to make this construction work without the fundamental groupoid instead of the fundamental group kekw Im sure i can but I will think about it for a bit instead of posting something wrong

long grail
#

An open set of a compact hausdorff space X can't be dense if it is missing isolated points, correct? For instance, in X=[1,2]U{3}, (1,2) cant be dense because the closure of (1,2) is [1,2], which doesn't include {3}. The reason I ask is because the boundary of a closed set is nowhere dense. But I read the complement of a closed nowhere dense set is open and dense. Where I'm having trouble is that the boundary of X is {1}U{2}U{3} the complement of which is (1,2) which is not dense from what I said above. Can someone tell me where I'm going wrong?

thorn citrus
gentle ospreyBOT
languid patrol
gentle ospreyBOT
#

Topos_Theory_E-Girl

gentle ospreyBOT
long grail
#

For a compact Hausdorff space, If C_1 > C_2 > ... is a nested sequence of closed sets, the intersection is non-empty, is that right?

bitter smelt
#

Yes. You don't need hausdorff. This is cantors intersection theorem

noble osprey
#

Hi for this prop 9.11 if X\V is open is that the same as X being open? ( but 1. says X is closed) Thanks

#

oh wait X\V a collection of open subsets yea?

long prairie
#

X\V is an open set, for some closed set V

#

if you put $V=\emptyset$, then you can see $X \backslash \emptyset=X$ is indeed a closed set.

gentle ospreyBOT
#

cflau_

long prairie
#

in fact, $X$ is both open and closed, and there's nothing wrong with that

gentle ospreyBOT
#

cflau_

noble osprey
#

Get it, thanks a lot

abstract wigeon
#

a grad student at my school told me that topology allows us to use open shapes to determine which points are near to each other without specifying distance, can someone help me think through why this is the case?

#

i would assume that two points are "near" if we can find an open set that contains both of them, but the whole space is open, and obviously the whole space contains any two points in it

#

so im not exactly sure the intuition behind this notion

fading vale
#

It's a heuristic notion of being near rather than a formal one

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If I take the points 0, 1, and 2 in the real line then any open ball about 0 containing 2 contains 1 but not the reverse so in this vague sense 1 is "closer" to 0 than to 2

abstract wigeon
#

hmm okay

fading vale
#

But there are uncountably many open balls about 0 containing both so it's not really a strict definition

#

A useful intuition might be to think about Hausdorff spaces vs non Hausdorff spaces

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In a non Hausdorff spaces you have points x, y such that any open ball about x contains y

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So in this sense the points x and y are "so close together you cannot distinguish them topologically"

abstract wigeon
#

oh okay that makes a bit more sense

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so in a general case, how can we determine whether two points are "near" or "far"?

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or is this not the correct way to think about it?

fading vale
#

It doesn't really mean anything in an absolute sense beyond this separated vs non separated thing

gaunt linden
#

It's not really "nearness" you get to model -- it's more accurate that you get enough of the properties of distance to be able to define limits.

fading vale
#

Yes this is a better way of thinking about it

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Honestly for most practical purposes whatever particular field you're working in will have it's own heuristic notions of what makes points close or near that you will practically use for intuition

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So I think worrying about this nearness closeness idea is not super important in the point set context

gaunt linden
#

So in a topology you can say no matter how close you insist it has to be, there's something with such-and-such properties. But you cannot say "this is closer than that".

abstract wigeon
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okay i think this makes more sense now

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thank you both for your time šŸ™‚

chrome ridge
languid patrol
#

Did you at least show that you can reduce to constructing a cover for each G = \pi_1 set with transitive action?

chrome ridge
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Isn't the idea if we show that for each orbit we get a path connected cover and then the cover for all of the set will be the space with all these path connected components ?

languid patrol
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Yes exakt

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*exactly

chrome ridge
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Now wlog we can assume that our pi-set is transitive and we want to construct a cover (it's gonna be autmoatically path-connected)

languid patrol
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So fix a base point for your G set

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How can you write it using this?

chrome ridge
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Not sure; but we want loops that lifts to loops in the covering space to have no effect on the base point. So do we consider the covering space whose fundamental group is the stabilizer of the point that we fix in the G-set?

languid patrol
#

Yes so this gives an equivalence between based coverings and based G-sets (which should’ve been part of your equivalence)

#

The other direction comes from looking at the monodromy action of pi_1 on the fiber, wrt the fixed base point in the fiber

chrome ridge
languid patrol
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That’s almost by definition of X^univ/H (note that X^univ also comes with a based point in this based category)

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The monodromy action on the fiber comes from the action of G on the fiber of X^univ above the base point of X

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But if you didn’t prove this in class you can show it with path lifting

chrome ridge
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I see. I like this approach better; we're utilizing the classifiaction that we have of path-connected covering spaces.

languid patrol
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Yes. It's a nice way

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Then the claim about isomorphism classes of unbased objects comes from forgetting the base points on both sides.

solar grove
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İs every line in topology a set of infinite point with them and we technicaly can chance arrangement of point in set and set will technicaly be same.so same logic affect topology is it because why to diffrent lines with diffrent shape is counted as same

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I think i wrote very complicated

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But you got the point

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Okey

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İ will trying explain

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So we have sets of 1,2,3

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İf we mixed up like 3,2,1

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it would be same set

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So i am asking lines in topology is a sets of infinite coordinate of points

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is that why it is diffrent lines in topology counted as equal

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Not equals

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Lets say only rule is a point not crosing with other point

noble osprey
#

Hi, for the preimage of e^3x it is h^-1({a}) <= 1 why is it not 2? Thanks

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not <=2

noble osprey
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so like the function X - Y ( In this case f : R - R) a is an element we choose in Y

novel acorn
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OK but then how did you come up with the bound <=1?

bronze wind
#

Hey ! In topology we can define the notion of convergence in a very general setting (for a topological space (X,T)). But does all the type of convergence that we see during our studies always mean that there is an "underlying" topology within the space that we study ? For example we saw in class the convergence for distribution and our teacher said that indeed it corresponds to the notion of convergence that you would have if you put a (very exotic) topology on the space of distribution. In measure theory for example, is there a topology for almost everywhere convergence ?

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I hope my question is clear

novel acorn
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for other types of convergence (here specifically convergence in measure) you put topology of convergence in measure on your function space and that gives you said convergence
But I don't think there's a topology for almost everywhere convergence
This is because I think almost everywhere convergence has some issues if you try to put the topological form of convergence on it iirc

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(But I think you can put a different structure on your space in that case but I'm not 100% sure what the details are)

shadow charm
#

What are some homological tools to show two spaces aren’t homotopy equivalent when you know homology and fundamental groups agree? I don’t think something like local homology should be preserved under homotopy equivalences but can we do something similar that is?

languid patrol
languid patrol
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So show that the intersection pairing between cycles is different on one than the other.

shadow charm
languid patrol
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Are you sure you're not being asked about homeomorphism? That would be easier and then local homology is preserved.

shadow charm
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Yeah for sure, homeo would be easy in this case

languid patrol
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Hmm shame that

shadow charm
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Im looking at S^1xS^2 vs S^1 v S^2 v S^3

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Intuitively speaking a homotopy equivalence would have to contract S^3

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But idk how to phrase that

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I was thinking maybe there was a way to say that a homotopy equivalence could be viewed as a homotopy in R^4 and use Jordan curve or smth to get a contradiction but that sounds whack

languid patrol
shadow charm
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Ah right im not used to thinking about covers

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Isn’t the universal cover of S^1xS^2 RxS^2 though?

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Not that it makes a difference

languid patrol
#

Yes, I was speaking up to homotopy equivalence.

shadow charm
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Yeah okay

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Alright that’s smart I’ll keep covers in mind from now on

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We haven’t really looked at them yet so I’m not too comfortable with calling them up to my toolkit but by exam time we’ll have seen it so it’s aight

languid patrol
#

It is a stupid example though.

shadow charm
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Ew long line

languid patrol
shadow charm
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Good to know though

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Thanks

crisp helm
#

To be honest, no idea where this belongs as it comes from a practical problem.

My friend is making a golf computer game with a twist: the user enters an RGB hex code, and that is where your ball gets putted to. You can see the flag you are trying to get to.

Since we are putting our ball on a 2D plane we want a projection from the cube of R,G,B values into the plane.
An important property that our projection needs to have is that if two colours are close in RGB space, they should be close in the 2D projection. It doesn't matter if far away colours are even further away than what they really "should be".
Is his game possible to make?
What sort of considerations need to be made for the projection?

Ideally he wants to have every colour represented in his game.

abstract saffron
#

Hilbert's curve is your best friend

solemn oar
obtuse meteor
#

A general idea in this topic is: build an object homotopy-theoretically from your two spaces and then look at the pi1 / (co)homology of that instead

#

this is surprisingly powerful, because if the construction is complex enough, it might not be that the object's pi1/cohomology can be computed just from the pi1 / cohomology of the base space you started with

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The simplest example being the loop space (but unfortunately this is terrible to compute, as it's higher homotopy groups)

solemn oar
#

You also have more complicated cohomology operations like the Massey product. For example IIRC the Massey product distinguishes the complements of Borromean and the Brunnian links, which the cup product is too coarse to detect.

quick bough
#

can anyone elaborate the definition of this, this seems so weird to me (at least the last part with the open cells)

novel acorn
quick bough
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(open cells)

unreal stratus
#

It's a definition

novel acorn
#

something something this makes the pushout work

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tho like idk what exactly is weird abt it

plain raven
#

is it confusing because they're not literally open

abstract saffron
#

I guess one of the many reasons is the glueing lemma

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Similar to how you breakdown simplicial complexes into simplices. Here you break down the spaces into a bunch of balls. Why balls? Because they're simple and nice.

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But don't quote me. I've fought with this for days. Still haven't got it.

crisp helm
plain raven
quick bough
#

i’m a bit confused on what the quotient map should be in the first place

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in this case (not the definition)

nocturne basalt
#

you quotient by the attaching map on the n-1 skeleton

unreal stratus
#

Basically the point is like if you attach a cell D^n to a space X to form Y, then there's a canonical map D^n -> Y

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Since you attach it via the boundary, this map is a homeomorphism onto its image when you restrict to D^n \ boundary

quick bough
#

ohhh, okay, got it now

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thank you

civic verge
#

guys a question is it true that the

#

$\partial X=X'-X$

gentle ospreyBOT
#

Awuita Fria

civic verge
#

I was thinking that no

unreal stratus
#

You're correct. For example note that if X is closed, then X' is contained in X, so X' - X is empty

civic verge
#

Thanks, I will do the demonstration

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I'm just not sure about some things but I'm going to do it hehe.

civic verge
#

Let $A$ be contained in $R^{n}$, If $A$ is closed then we say that $a$ belongs to $R^{n}$, suppose that $a$ is an accumu
lation point of $A$ where for any given epsilon, there exists a y that belongs to $A$ such that y belongs to the Ball of center a and radius epsilon.

We know that A is closed, this implies that $A'$ is contained in closed $A$, so the boundary of A is equal to empty since $a$ is an accumulation point, therefore it is false

gentle ospreyBOT
#

Awuita Fria

civic verge
#

look

grim knot
#

Hey guys, can someone help me get an intuition of retracts, deformation retracts and strong deformation retracts? I somehow can't quite imagine how they could work

languid patrol
# grim knot Hey guys, can someone help me get an intuition of retracts, deformation retracts...

Have you never seen examples of them? An example which contains all 3 types of retract is the following, let $X = {(x, y) \in \mathbb{R}^2| 0 < x^2 + y^2 \leq 1 }$ then we can parameterize $X$ in polar coordinates by $f(r, \theta) = r(cos(\theta), sin(\theta))$ for $0 < r \leq 1, 0 \leq \theta < 2\pi$. Let $R$ be the map which sends $f(r, \theta) \to f(1, \theta)$, then $R$ is a retract of the inclusion of the circle into $X$. On the other hand $H(f(r, \theta), t) = f(r(1 - t) + t, \theta)$ is a (strong) deformation retract. Intuitively a deformation retract is a space where every point can be moved along a path to lie in a subspace in a way where the paths vary continuously, and a retract is a space where every point can be assigned a point in the subspace continuously, but not necessarily moved there along a path in such a way that the paths vary continuously. Perhaps the hardest thing to understand is a strong deformation retract, because most deformation retracts which are geometrically intuitive are strong deformation retracts.

gentle ospreyBOT
#

Topos_Theory_E-Girl

lime sable
#

hmm i'm wondering if there's some niceness condition on a pair for deformation retracts to automatically be upgraded to strong deformation retracts

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nlab and hatcher are of no help, although nlab gives a fancy definition for a strong deformation retract

willow vapor
#

how can I understand an identity map between 2 metric spaces?

#

like, I get that every element probably gets mapped to itself, but how do the metrics play a role?

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like say from $(X,d_\infty)$ to $(X,d_2)$

gentle ospreyBOT
#

WasMachenWirDennDa

lime sable
#

i guess hegel figured out what an adjunction was over a century before mathematicians did

languid patrol
umbral panther
lime sable
languid patrol
#

The definition

pastel linden
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Is there a global G-action on the associated bundle to a principal G-bundle?

languid patrol
pastel linden
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Yes, sorry

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(Nontrivial action and associated bundle)

languid patrol
#

So given some representation (\rho, V) the associated bundle is V \times^G \mcal{G} so there is a canonical G action coming from the one on either side.

pastel linden
#

Could you elaborate? I was under the impression we have
((g_a ā—‹ g_b^-1)(x, v)) ā— h = (x, r(g_ab)v) ā— h = (x, r(h^-1 g_ab)v)
(g_a ā—‹ g_b^-1)((x, v) ā— h) = (g_a ā—‹ g_b^-1)(x, r(h^-1)v) = (x, r(g_ab h^-1)v)
which isn't global

languid patrol
#

I don't know what you mean by not global

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Also it would be nice if you could TeX what you write so I can read it more easily

pastel linden
#

As in, if we define it as $(x,v) \cdot h = (x, \rho(h^{-1})v)$, this is not independent of the trivialization

gentle ospreyBOT
#

bacono

lime sable
#

so that's what i'm asking

pastel linden
#

Also, the global G action on P becomes trivial when we pass it down to the associative bundle by construction

languid patrol
#

It is equalized with the left G-action on V.

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The action which becomes trivial is the action $g*(v, s) = (gv, sg^{-1})$

gentle ospreyBOT
#

Topos_Theory_E-Girl

pastel linden
#

What do you mean by the "it is equalized by the left G action"?

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I'm not familiar with that terminology, sorry

languid patrol
#

But yes this action is not a "global" one, in general there cannot always be such a "global" action even for $G = Gl_n$.

gentle ospreyBOT
#

Topos_Theory_E-Girl

languid patrol
lime sable
# languid patrol The retract

so it's actually "every retract is gives a strong deformation retract" not "every deformation retract is gives a strong deformation retract"

pastel linden
languid patrol
#

So if G is abelian this exists, but for general G even for G = Gl_n you can see that such an action can't exist in general

pastel linden
#

Thank you! This is what I've been thinking but i thought i was going insane

languid patrol
lime sable
pastel linden
#

Yeah, this came up in the context of nonabelian gauge theories in physics which involves connections on associated bundles to principal SU(3) things

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Physicists like to pretend that global actions on sections exist (when in fact, they do not)

languid patrol
umbral panther
chrome ridge
#

Orbits of the action on deck transformations on the covering space are of the same sizes?

languid patrol
#

For instance if X_2 is a double cover of X then X \coprod X_2 has two orbits for its deck transformations of different sizes.

chrome ridge
#

Very vague intuition coming from the fact that only the identity transformation fixes a point.

#

But I guess the set on which we are acting is not finite so it is not necessarily true that orbits have the same sizes

solemn oar
#

If your space is connected (plus the other usual assumptions) it's true.

pseudo coral
#

question, how do i prove the case riguourusly that $\pi_n(X)$ is abelian for $n \geq 2$ specifically the case $n=2$

gentle ospreyBOT
#

MyMathYourMath

pseudo coral
#

for $n=2$ can this be made rigorous easily?

gentle ospreyBOT
#

MyMathYourMath

pseudo coral
#

let $\alpha, \beta \in \pi_2(X)$ for some top space $X$ then $\alpha,\beta:(S^2,a) \to (X,x_0)$

gentle ospreyBOT
#

MyMathYourMath

pseudo coral
#

is it the extra dimention that allows for this "Hop" so i can commute them? i can see it but

fading vale
#

There are quite a few ways to do it