#point-set-topology

1 messages · Page 19 of 1

eager herald
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ah yeah i see

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are these conditions usually not called the "first separability axiom" and the "second separability axiom"?

coarse night
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no

eager herald
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so (i) is just the definition of a separable space, and (ii) is the definition of a second countable space?

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(ii) --> (i) generally, and (ii) <--> (i) in metric spaces

ruby crown
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@gritty widget Huh, I looked up open mapping theorem but it is about concluding that a function is an open map. Then I searched about homeomorphism preserving dimensionality and could not find a related proof for that either. Any idea where I can find a proof for:
Let $f: \mathbb{R}^n \rightarrow \mathbb{R}^m$ be a homeomorpic function. Then n = m.

gentle ospreyBOT
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FrankF

coarse night
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if your map f is a homeomorphism, you can use Homology theory to claim m=n

ruby crown
gritty widget
ruby crown
echo oyster
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I took f:R →Rl a continuous function & reached the conclusion that f can only be a constant function, is it sufficient to answer the first part of 7(b) ?

little pulsar
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Could someone help me with this part (c) please? I got this in an exam a week ago and still don't know how to find/show the homeomorphism...

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my tragic attempt:

gritty widget
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this is a map from SO(n) to S^(n-1)

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since SO(n) is compact and S^(n-1) is Hausdorff, this is a quotient map

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now Ae_1 = Be_1 iff A ~ B by definition

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so it induces a homeomorphism from SO(n)/~ to S^(n-1)

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sorry, didn't mean to solve it, I was just trying ideas

little pulsar
gritty widget
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questions are for asking

little pulsar
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why is it closed

gritty widget
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because SO(n) is compact and S^(n-1) is Hausdorff

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so a closed subset of SO(n) is compact, its image is compact, so closed since its a compact subspace of Hausdorff space

little pulsar
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ahhhhh

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sounds good

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ngl, it sounds familiar so I think we proved this in homework but I can't recall it at all

gritty widget
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might be, it's a pretty standard fact

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easily provable though

little pulsar
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yaya

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tydomsadpout

gritty widget
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not a problem

echo oyster
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@gritty widget help please I'm still confused

gritty widget
#

so whatever makes sense to you is good enough imo

echo oyster
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From R to Rl right ?

gritty widget
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both

echo oyster
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R to Rl & Rl to Rl right ?

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I'm confused why the f : R→R is given

gritty widget
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no continuity

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then they ask you what continuous functions from R to Rl and Rl to Rl could be

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but they ask you to conjecture what could they be - so they're not expecting an answer

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not in the sense that you need to give any justification for your guess

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just how intuitively you think those functions could look like

echo oyster
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Oh i see

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Thank you

gritty widget
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no problem happy

steel glen
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exercise from hatcher, states that if $\tilde{X}$ and $\tilde{Y}$ are simply connected covering spaces of the path connected, locally path connected $X$ and $Y$, then $X\simeq Y\implies \tilde{X} \simeq \tilde{Y}$. i don’t know if this simeq is meant to be homotopy equivalent or homeomorphic, anyone know what it most likely is?

gentle ospreyBOT
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maximo

solemn oar
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Probably homotopy equivalent.

steel glen
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thank you that’s what i figured

unreal stratus
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btw are there any cool applciations of the fact that every flow on a compact polyhedron (= homeomorphic to a finite simplicial complex) has a fixed point? I've never worked with flows oop

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i imagine there'd be smth in geometry but idk

gritty widget
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Let p:(Y,y)->(X,x) be a universal cover, g a closed path in X (with start/end = x), and g' the lifted path in (Y,y). Why does there exist an automorphism f of the covering space such that f(y)=g'(1) ?

next crystal
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Let A be a subset of a topological space X
x \in cl(A) if and only if for every open set U containing x, the intersection A \cap U is not empty

Sps x \in X and every open set U containing x, the intersection U \cap (A \ {x}) is not empty. Then x is called a limit point of A

is the only difference between these that a point x can be in the closure if theres an open set U containing it such that A \cap U = {x}. But if this U exists then x is not a limit point

gritty widget
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in fact, if A \cap U = {x} then x is in A so its already in the closure

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points like these are called isolated (in A)

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i.e. {x} is open in A

next crystal
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right got that

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X is an ordered set in the order topology. I've shown that the closure of (a,b) is a subset of [a,b], and I'm being asked under what conditions does equality hold.
when the screenshot says "it has to be that they (a and b) are both limit points of (a,b)" what does that follow from?

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i follow everything up to that quote

gaunt linden
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Can you see that if a has an immediate successor, then it won't be in the closure?

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Ah, no you didn't get that far yet.

odd flame
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is this Q phrased weirdly or is it justme

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in particular the isomorphisms

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one should go the opposite way no?

gaunt linden
odd flame
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actually ig theyre isomorphisms so it doesnt matter bleakkekw

next crystal
gaunt linden
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I don't think I understand your question.

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Proved what exactly using an immediate successor/predecessor argument?

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As far as I understand the problem you're describing "immediate successor/predecessor" is not a detail in an argument -- it is the answer being argued for.

odd flame
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i cant seem to internalize the idea of the fundamental group

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like its elements are equivalence classes of maps right

gaunt linden
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Yes.

odd flame
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bit of a silly question but how is it not just one equivalence class

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it's made up of loops right

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so paths starting and ending at a single point x

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but any path from x to itself should be able to be continuously deformed into another no?

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i guess that doesn't account fo orientation but i feel like im still missing part of the picture

gaunt linden
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Suppose your topological space is the unit circle and x is (1,0). One path from x to x is gamma(t) = (cos(2 pi t), sin (2 pi t)), another is the constant function gamma'(t) = (1,0). How would you deform the former continuously into the latter?

odd flame
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so are there things in general that distinguish loops? or is it always specific to a space

nocturne basalt
odd flame
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i sense a chicken or the egg situation

nocturne basalt
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well we have loops, but we want to treat some of them to be the same so we add this equivalence relation

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which we can furthermore endow with an algebraic structure

odd flame
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also the change of basis point isomorphism

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that's always conjugation right?

nocturne basalt
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yeah

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well technically the path which induces it isnt part of either pi_1

odd flame
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wdym

nocturne basalt
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conjugation is usually defined in terms of a group right

odd flame
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ohh do you mean like

nocturne basalt
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but the path which induces the homomorphism isnt part of either fundamental groups

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since its not a loop

odd flame
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conjugating a subgroup of a group is usually done by an element outside of the subgroup

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is that how you mean?

nocturne basalt
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well it doesnt need to be, but its just usually done by any group element

odd flame
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also mildly related but how does "isomorphism equivalence" work

odd flame
nocturne basalt
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wdym isomorphism equivalence

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an isomorphism can be thought of a version of "equivalence"

odd flame
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like the claim in that problem

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part of it is if the two change of base point iso's are equal

odd flame
nocturne basalt
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ohh

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well

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you can have multiple isomorphisms between groups right

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this is a matter of are the isomorphisms the same

odd flame
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yeah but that just feels like a weird question

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like theyre both isomorphisms

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it's like an equal equivalence bleakkekw

nocturne basalt
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yeah i get what you mean

odd flame
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at least this is more fun than point set

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how do you even show equivalence of isomorphisms then?

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like the backwards part of that iff

obtuse meteor
nocturne basalt
odd flame
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imma try the forward direction then try that catthumbsup

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for each h and h' it doesnt matter if we distinguish their directions right? since theyre both iso's

odd flame
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repost for convenience

odd flame
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like saying that h is a path from x0 -> x1 and h' is a path from x1 -> x0

nocturne basalt
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well gamma and gamma' are both paths from x0 to x1

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usually the reverse is denoted with a bar

odd flame
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oh

obtuse meteor
odd flame
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then tbh im not sure what the two isomorphisms are

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oh wait nvm

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it's just conjugation by either gamma or gamma'

nocturne basalt
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yeah pretty much

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since that lets you take any loop at x0 to x1 and vice versa

obtuse meteor
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And any loop in S^1 can be “lifted” to paths (not necessarily loops) in R, and upon lifting homotopic loops in S^1 are exactly the ones with the same endpoints in the universal cover

nocturne basalt
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what's the difference between that and a covering space?

odd flame
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homotopic = continuous map between them right?

obtuse meteor
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Er kinda a homotopy is a map X x I -> Y which is the same as the two specified maps X -> Y at the endpoints

obtuse meteor
nocturne basalt
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gotcha

odd flame
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so is saying h = h' the same as saying that conjugation of loops centered at x0 by gamma is equivalent to the conjugation of those loops by gamma'?

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i guess based at is the proper term

odd flame
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the operation of the fundamental group is just loop composition right

coarse night
odd flame
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never been sullied in this way beforee

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to what do i owe the honor

coarse night
#

My \amongus got rejected

odd flame
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$\amogus$

gentle ospreyBOT
odd flame
#

skill issue

coarse night
odd flame
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dont snitch ryu

coarse night
#

Lmao illegal

odd flame
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operation is homotopy class of...?

coarse night
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elememts of π_1(X, x0) are not paths but homotopy equivalent paths

odd flame
coarse night
#

[f]*[g]=[f*g]

odd flame
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i get that much

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i was asking how we operate on two equivalence classes

coarse night
odd flame
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that's just composition right

coarse night
#

pick representative and concatenate then take it's equivalence class

coarse night
odd flame
steel glen
odd flame
coarse night
#

yes

odd flame
coarse night
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that what it is

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what's the rule for a base point chage?

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is it aba' or a'ba

odd flame
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a'ba

steel glen
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$$[f][g] = [f\cdot g]$$ where $$(f\cdot g) (x)= \begin{cases} f(2x) & x\in[0,\frac{1}{2}\ g(2x-1) & x \in [\frac{1}{2},1]\end{cases}$$

gentle ospreyBOT
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maximo

coarse night
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so it's saying a'xa=b'xb

odd flame
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it's actually abba, the genius artist behind global sensation Dancing Queen

coarse night
#

or (ab')x(ab')'=x

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the conclusion is clear

odd flame
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are you talking about the forward direction?

coarse night
#

There's a reverse direction?

coarse night
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all these are iff so

odd flame
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perhaps im overthinking then

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how do we know the gammas commute with each other tho

steel glen
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gamma and gamma bar?

odd flame
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gamma and gamma' bar

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actually i dont think we need that

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one sec

steel glen
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id imagine you would otherwise why would it be included

odd flame
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,rotate

gentle ospreyBOT
odd flame
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mildly related

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is it really fucking weird that conjugation just happens to have all these magical properties in different scenarios?

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first conjugation with normal subgroups and whatnot

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now conjugation defining a change of base pt isomorphism

steel glen
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well a normal subgroup is defined by conjugation, so it's really no coincidence there

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here it is interesting but it's very clear why this "conjugation" makes sense

odd flame
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i just mean that it seems like a random thing to do that gives very useful consequences

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but then again why does anything in math work

steel glen
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yeah i do see that

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we learnt about the sylow theorems and conjugates are just flying around being crazy useful

odd flame
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i had a similar experience

odd flame
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bc im not really using h_gamma

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walter

dry jolt
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I mean, conjugation is a "change of basis" in some sense of the word so I don't find it's prevalence too surprising

odd flame
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yeah i forgot it appears in linear algebra too

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which i'll assume implies that it appears in R-modules too

steel glen
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if it appears in linear algebra then it is immediately three times as important and prevalent

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so yes it is no surprise i guess

odd flame
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i suppose

odd flame
steel glen
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i did this exercise a few weeks ago

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let me look

odd flame
#

you also doing an alg top class?

odd flame
steel glen
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the first thing to note is that w does not equal (gamma gamma'bar) w (gamma gamma'bar)

odd flame
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also the next question is to prove that h_gamma = h_gamma' iff the fundamental group based at x0 is abelian

steel glen
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at best they are homotopy equivalent (and only sometimes equal)

odd flame
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ok nvm about what i was gonna say

steel glen
odd flame
#

same bleak

odd flame
steel glen
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note im not saying they aren't the "same"

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just that they aren't equal

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the notion of same here should be homotopy equivalent

odd flame
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can you define that for me then pls i think i have the wrong idea of what that means

steel glen
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the other important thing is that you're assuming (gamma gamma'bar) is homotopy equivalent to the constant map

steel glen
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and paths are just functions from I to the topological space

odd flame
steel glen
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so the loops are equal iff f(t) = g(t) for all t in I

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when talking about fundamental groups we usually only really care about being the "same" up to homotopy, so up to continuous deformations

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so what I assume you meant to say is $$\omega \simeq (\gamma \overline{\gamma'})\omega (\gamma\overline{\gamma'})$$

gentle ospreyBOT
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maximo

steel glen
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where \simeq is just homotopic to each other

odd flame
#

i see what you mean

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i'll make a note of it in the proof then

steel glen
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the other thing to note is that while (gamma gamma' bar) is indeed a loop, it may not be homotopic to the constant map

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so that \simeq may actually be false

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let me draw up a quick example of what that might look like

odd flame
steel glen
#

you can't contract that gamma gamma' bar to a point

odd flame
#

shouldnt it be (gamma gamma'bar)w(gamma' gamma bar)

steel glen
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if we want to show (gamma gamma'bar) is in Z(pi) then no

odd flame
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hmmm

steel glen
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another notation nitpick before we get into the proof

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your map h_g is not well defined

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it should go

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$[\omega] \mapsto [\sigma \cdot \omega \cdot \overline{\sigma}]$

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owo

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sorry

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instincts got the better of me

odd flame
gentle ospreyBOT
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maximo

steel glen
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the dots are implied but let's keep them for clarity

odd flame
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it's okay i use omega bc it makes it look like an owo whatcanisay

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my prof has the sigma bar come first tho

steel glen
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i would start by assuming $h_\gamma = h_{\gamma'}$

odd flame
#

that's just preference right?

gentle ospreyBOT
#

maximo

steel glen
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so the proof is a bit tricky as you might imagine

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and start by taking h_g[w] = h_g'[w]

odd flame
steel glen
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yes

odd flame
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i'll use g and g' instead of gamma

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but then (gbar)(w)(g) = (g'bar)(w)(g')

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this is the same as what i have written up to now

steel glen
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note it's [gbar w g] = [g'bar w g']

odd flame
#

but then we can separate right

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[gbar] [w] [g] = [g'bar] [w] [g']

steel glen
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we can't actually

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because those aren't loops

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(only w is)

steel glen
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start with [g g'bar][w] as you had

odd flame
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it's [g' gbar]

steel glen
#

oh thanks

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[g' gbar][w]

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i would multiply the right side by [g gbar]

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since it is the identity in pi_1

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[g' gbar][w][g gbar] = [g' gbar w g gbar]

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note that since we assumes h_g = h_g', we can say gbar w g is homotopic to g'bar w g'

odd flame
#

i was about to say that WanWan

steel glen
#

great

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so how would you continue

odd flame
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[g' gbar w g gbar] = [g' g'bar w g' gbar] = [w g' gbar]

steel glen
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= [w][g' gbar]

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so what is the conclusion

odd flame
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silly q but why can we break it apart there but not before

steel glen
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because both w and g' gbar are loops

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but g' and gbar are not loops alone

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that is

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[g'] is not in pi_1(X)

odd flame
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i think i mostly see it.

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it's still a chain of iff's

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just a little different

steel glen
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remember g and g' are just paths from x0 to x1

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or x1 to x0, doesn't really matter

steel glen
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it's just equality, which i guess is kind of an iff

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but we only did the => direction

odd flame
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oh bleak

steel glen
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the <= is not much more difficult

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did you understand the => direction completely though?

odd flame
#

lemme write it up

odd flame
steel glen
#

yes

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in particular

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$[f][g] = [f\cdot g]$

gentle ospreyBOT
#

maximo

steel glen
#

where the dot is the path product i defined way up above

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this is the group operation on the fundamental group

odd flame
#

ok fully understand forward direction

steel glen
#

great

odd flame
#

the backward direction is almost the same then

steel glen
#

hm im not sure just yet

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id say not exactly though

odd flame
steel glen
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be careful with rearranging

odd flame
#

bc you can only rearrange loops right

steel glen
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yes

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and only if they commute

odd flame
#

not individual gammas

steel glen
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let's start with h_g[w]

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= [gbar w g]

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multiply the left by [g'bar g']

odd flame
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i was about to say lol

steel glen
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what do you get?

odd flame
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[g'bar g'] is a loop so we can "operate"

steel glen
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yes

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by the way, when we multiply by [g'bar g'], you should be making sure we are respecting the basepoint of the fundamental group we're working with

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i'm taking it as a given, but you should probably confirm all that in your proof

odd flame
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proof: trust me

steel glen
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damn

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can't send gifs ig

steel glen
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we should have $[\overline{\gamma'}\cdot\gamma'\cdot\overline{\gamma}\cdot\omega\cdot\gamma]$

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cursed

gentle ospreyBOT
#

maximo

odd flame
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but g'gbar commutes with everything

steel glen
#

with every loop

odd flame
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well it commutes with [w] which is what we need

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to then cancel out gbar and g

steel glen
#

in particular, [g' gbar][w] = [w][g' gbar], which is to say (g' gbar)(w) is homotopic to (w)(g' gbar)

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so we can indeed commute the (g' gbar)(w) in the class there

odd flame
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the result is then obvious

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reduce to [g'bar w g']

steel glen
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i would write the intermediate steps

odd flame
#

we have our desired equality WanWan

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yeah im being verbose enough

steel glen
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[g'bar w g' gbar g] = [g'bar w g'][gbar g] = [g'bar w g']

odd flame
#

in what i write

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thank you so much for the patience btw

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like i genuinely understood the steps WanWan

steel glen
#

np, this is probably the only thing i properly understand from this class so far so im happy to discuss it

odd flame
#

i still dont really know what a projective plane is

steel glen
#

me neither but i keep pretending i do and it keeps working

odd flame
steel glen
#

but jokes aside you can think of it like s^n under the quotient topology relating antipodal points

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im not sure if youve been introduced to that notion or not

odd flame
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yeah i can regurgitate the definition

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just not 100% comfy with it

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needs a bit of time is all

steel glen
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i don't think you ever become 100% comfy with AT lol

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but yeah

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it eventually becomes natural-ish

odd flame
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what's your algebra class like btw

steel glen
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it's called algebra 2 so we're continuing ring theory, field theory, and hopefully getting to galois theory

odd flame
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mine is the same!

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i had groups and rings last sem

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this sem is fields and modules

steel glen
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yeah so far we've done some g-sets, sylow theorems, and group series. getting into ring theory now

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last sem was all group theory pretty much

odd flame
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wouldve assumed that shouldve included sylow thms tho holothink

steel glen
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we went kind of slow-ish and also lost a lot of class cause of hurricanes and football games

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overall a messy semester

odd flame
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should i chance a guess at florida

steel glen
#

ucf yeah

odd flame
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nowhere else does the sentence "lost a lot of class cause of hurricanes and football games" apply

steel glen
#

lmao true

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i doxxed myself with that kekw

odd flame
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i can delete message

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ive doxxed myself plenty in here idc anymore tbh

steel glen
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but ye im pretty much just exhausting all the algebra, topology, and geometry offered here

steel glen
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idc if people know

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ok im off to bed, got algebra tmrw

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gn and gl with your AT course

odd flame
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mucho thanks

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you'll see plenty of me in here bleakkekw

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,ti maximo

gentle ospreyBOT
#

This user hasn't set their timezone! Ask them to set it using ,ti --set.

odd flame
#

i know this has to do with brouwer fixed pt thm, but can i get some pointers on this pls

marble socket
#

what's the composite S^{n-1} --i--> D^n --r--> S^{n-1}?

odd flame
#

det eeveeKawaii

marble socket
#

sebbb eeveeKawaii

odd flame
#

,ti det

gentle ospreyBOT
#

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marble socket
#

9am

odd flame
#

o

gentle ospreyBOT
#

Member selection timed out.

odd flame
marble socket
#

ye the inclusion into the boundary

odd flame
#

well that's jus the boundary of the disc

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i brush teeth i brb

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i here

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so why do we wanna consider that i first?

marble socket
marble socket
odd flame
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just a start i guess

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i figure it's asking for the preimage of open sets is open defn of continuity

marble socket
#

you mean showing r is continuous? devastation

odd flame
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yeah

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maybe my brain is still stuck in point set

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but isnt that what we need to show

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preimage of an open set of S^n-1 is open in D^n

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tho ig idek the topologies on these things devastation

marble socket
#

yea we do, but most people doing alg top at that point would just agree that the definition of ray intersecting is "continuous" enough and doesn't need a proof KEK

odd flame
marble socket
#

like they say, write a formula

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and use sequential ocntinuity

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everything is a metric space

odd flame
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like explicitly state r?

marble socket
#

that's what they have written devastation

odd flame
#

ok well shouldnt we be thinking first about r \circ f

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that's probably obv ig

marble socket
#

start with x, go at f(x), then make a ray from f(f(x)) to f(x)

odd flame
#

wait why f(f(x))?

marble socket
#

because that's how we define r(x)

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start from f(x) and go to x

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and see where you hit the sphere

#

so r(f(x)) would start at f(f(x)) and would go to f(x)

odd flame
#

,ti

gentle ospreyBOT
#

The current time for stμ₂dying is 03:23 AM (EST) on Tue, 07/02/2023.

odd flame
#

i'll be back in 4 hours det

#

thank you again for trying tho sad

marble socket
#

good night eeveeKawaii

#

(4 hours is too less to sleep tho kongouDerp)

odd flame
#

i'll nap later in the day tooo

odd flame
#

hi @marble socket

marble socket
#

Ohayou eeveeKawaii

odd flame
#

ohio

marble socket
#

3 hours 20 minutes kongouDerp

odd flame
marble socket
odd flame
#

reposting for convenience e

marble socket
#

i wonder what they mean by vector rotation

odd flame
#

where

marble socket
#

to find the formula for r

odd flame
#

i think it says notation

marble socket
#

ah

#

yee so lets find a formula for r

#

what's the equation of the ray from f(x) to x?

odd flame
#

this is where it gets icky

#

doesnt that have to be parametric

marble socket
#

yea parametric is fine

#

we will solve for the parameter which forces it to lie on the sphere

#

and f(x) != x should make sure we're not dividing by 0s

odd flame
#

ok potentially stupid question

#

how do we know if we need the eqn of a line in 2d space, 3d space, etc

#

we cant know right

marble socket
#

D^n lives in the n-d space

#

so the line would also be there catThink

#

since we're writing parametric equation, there shouldn't be any problems. you start at the vector f(x) and shoot in the direction (x - f(x))

odd flame
#

so f(x) + (x-f(x))t

marble socket
#

yep lol

#

now need to find t > 0, such that this lies on the sphere

odd flame
#

in general S^{n-1}

marble socket
#

yep

#

use some inner products to get a quadratic in t

odd flame
#

somehow i feel like this isn't alg top enough

marble socket
#

yea this is just calculation

odd flame
#

nothing to do with retractions or anything

marble socket
#

not so far

#

once you verify this is a continuous map, then we're in business

odd flame
#

i mean yeah after that it's brouwer fixed pt thm

#

we proved that in class and left the continuity of this as an exercise

marble socket
#

the existence of that functor also requires some work

odd flame
#

my next question is actually to verify that a (path connected?) topological space is a category

#

but that doesnt seem too hard

marble socket
#

(path connected spaces would form a subcategory :3)

odd flame
#

it doesnt specify path connected

#

but the morphisms are set of equivalence classes of paths x0 -> x1 so

marble socket
#

oh mb

#

so objects of your category are points in X

odd flame
#

i'll do that one in a bit though

#

going back tho

#

we begin by considering r(x) = f(x) + (x - f(x))t for t putting this on S^n-1

#

doesnt continuity of r just follow from the fact that f is cont. (given)

marble socket
#

yea

odd flame
#

oh

#

then QED

marble socket
#

but the important part is that the solution for t exists and varies continuously with x

#

for that you need f(x) != x

#

if f(x) = x, then the ray is just a point

#

so depending on whether x lies on the sphere, there are either no solutions for t, or every positive real is a solution

odd flame
#

im sorry det but i might have to ask you to spoil this one

marble socket
#

you can explicitly write down the equation t needs to satisfy

#

because points on S^n-1 satisfy ||v||^2 = <v, v> = 1

#

this should give you a quadratic equation in t

#

and you can then solve for the positive root eeveeKawaii

odd flame
marble socket
#

say f(x) = a and x - f(x) = v

#

so you want <a + vt, a+vt> = 1

#

which is ||a||^2 + 2<a, v>t + ||v||^2 t^2 = 1

odd flame
#

ngl it doesnt help that i havent parametrized an equation in about 4 years so

odd flame
marble socket
#

yea, i don't think there's more to that

odd flame
#

and the fact that such t always exist makes it cont. right

marble socket
#

yea, and that is because ||a|| <= 1

#

(||a||^2 - 1) + 2<a, v>t + ||v||^2 t^2

#

so if you draw the graph of this, at t = 0 it is <= 0

#

but for t = infty, it must be infty

odd flame
#

where did that -1 come from

marble socket
#

so needs to have a root

marble socket
odd flame
#

ah

odd flame
marble socket
#

yep codomain is D^n, so f(x) lands in there

odd flame
#

is there a name for that test up there

#

i feel likee there was but idk

marble socket
#

you mean intermediate value theorem?

#

but yea these things should be clear from the picture

#

nobody writes explicit maps in alg-top

#

(unless nothing else can be done)

odd flame
odd flame
#

ok this is my last question

#

i think i've got composition and associativity

#

what would the identity morphism be? loops?

#

dont think it's loops

#

maybe fruit loops

#

@marble socket sad

marble socket
#

it's the constant path

#

c(t) = x0 for all t in [0,1]

#

you would need to show the composition is well defined

#

and be a little careful with associativity, as you don't have strict associativity, only up to homotopy

odd flame
#

,rotate

gentle ospreyBOT
odd flame
#

i think that's almost it for associativity

marble socket
#

like if [f] = [f'] and [g] = [g'] then [f*g] = [f'*g']

odd flame
marble socket
#

(also best to not use \circ, as you might confuse with the way you multiply. normally composition is done right to left >.<)

odd flame
#

and this should just be multiplication right

marble socket
#

yea, it's concatenation of the paths

odd flame
odd flame
marble socket
#

not exactly, but there isn't a lot to be done there

#

you would have (path) homotopies between f, f' and g, g' just need to concatenate the homotopies

odd flame
gritty widget
#

If p:(Y,y) -> (X,x) is a universal cover, does there exist a universal cover (Y,z)->(X,x) for any other point z in Y?

odd flame
#

ok i understood that

#

moving on, i didnt finish associativity right

#

im hoping those defn's are right

#

but as for setting them equal to each other i just wanted to draw the picture of I x I with the diagonal lines

marble socket
marble socket
# odd flame im hoping those defn's are right

yee the definitions are right, but the two maps aren't strictly equal. you would have to construct a path homotopy between them so that after going to homotopy classes you have an equality

odd flame
marble socket
#

also you mean 2/4 and not 2/2

#

idk too hard to read, maybe tha'ts 1/2 with a loop which confused me

unreal stratus
#

Is this the composition symbol for concatenation of paths

marble socket
#

yes KEK

unreal stratus
#

Please refrain therefrom

odd flame
#

it's 1/2

#

yeah i changed that ty det

#

alg top is the only hw i dont type up bleakcat

unreal stratus
#

That's how it's always been w me too lol

#

Too many diagrams

marble socket
#

writing feels so strange to me now kongouDerp

odd flame
#

det is too advanced

odd flame
marble socket
#

yea, it's annoying to do that tho

odd flame
#

is there a better way

#

wait there is a better way

#

math overflow

unreal stratus
#

Usually I would just do a diagram

#

I think most people would at least in exams or a lecture

#

Then the homotopy in the diagram can be written down explicitly and this is what you get

odd flame
#

that's just the diagonal lines on I x I right

unreal stratus
#

Yeah

#

Otherwise this is just a pain lol

odd flame
#

ok ty for pointers yall <3

marble socket
gritty widget
#

I'm not sure how to show the existence of the automorphism of the pointed covering space.

#

There's a theorem about the existence of liftings in the case that X is path connected and locally path connected, but I don't have that here.

#

Even assuming that the space is nice, it seems I would need a pointed universal cover from (X',gamma(1)) to (X,x) to lift it to (X',x'), but how do I know such a universal cover exists?

obtuse meteor
#

Some Points are distinguished in the universe cover (these correspond to ones lying over the intersection point)

coarse night
#

Deck transformations may not act transitively unless the cover is normal

gritty widget
coarse night
#

Then it’s normal

#

So acts transitively

gritty widget
#

If p:X' - > X is a universal cover, is p*pi:YxX' -> X a univeral cover where pi is the projection onto X' from YxX' ?

coarse night
#

universal cover is unique upto homeomorphism

#

also that's not even a cover

#

unless for very specific Y's

#

@gritty widget

gritty widget
coarse night
#

no longer connected

gritty widget
#

right

jaunty magnet
#

Hi everyone. Someone have defined an order topology over a poset? How do you work with elements that are incomparable with everything? (that´s an issue when I define the basis for a topology)

gaunt linden
#

The most principled thing to do would probably be to declare the sets {x|x>a} and {x|x<a} for all a to be a subbase for a topology. Then if the poset has a completely unconnected point, its only neighborhood would be the entire poset.

pseudo coral
#

question

gritty widget
#

the answer is yes if it's sunny out

pseudo coral
#

i am showing contractible spaces are simply connected does this suffice for a proof of the pathc onnected ness

#

That last intervals is 1/2,1

#

It’s not sunny out so

gritty widget
#

can u say the proof in words

pseudo coral
#

Lol

#

Yes

#

You travel from a to some fixed p

#

Via the homotopy that sends identity to constant

#

And one from b to p

#

Then take inverse of b to p

#

And compose the a to p with the inverse of b to p which travels from p to b

#

And then run it double time so it starts and stops at a and b respectively

gritty widget
pseudo coral
#

Is that a good or bad emojo lol

gritty widget
#

good

pseudo coral
#

Ok lol

#

Now for showing loops can be shrunken to a point

#

Do I use that same homotpy

#

Define the homotopys first component as gamma(t)

#

Where gamma is my loop

#

Does that work

gentle ospreyBOT
#

MyMathYourMath

#

MyMathYourMath

pseudo coral
#

is homotopic to the contant map at p define

gentle ospreyBOT
#

MyMathYourMath

pseudo coral
#

or do i define a homotopy that sends \gamma(t) to its base point?

#

thats my question

#

so for simply connected define a new map that sends any identity mapping to this constant base point

#

anybody??

pseudo coral
gentle ospreyBOT
#

MyMathYourMath

pseudo coral
#

and all x \in X

#

anyyyyyooonnneeeee???

#

@gritty widget ?

#

so do I define a homotopy whihc i know exists from gamma(t) to its base point via the homotopy which starts at \gamma(t) and ends at its base point

pseudo coral
#

anyone?

steel glen
#

if the space is contractible there is a deformation retraction to a point

#

use the deformation retraction as part of your homotopy

#

let F be the retract. you should be able to define a homotopy H between an arbitrary \gamma starting at the retraction point and the constant loop using F

#

@pseudo coral

pseudo coral
#

so is this correct @steel glen

steel glen
#

is what correct

pseudo coral
#

this

#

wait i used H when i meant F at the end

#

after defining F

#

i need to change all Hs to Fs

#

cause usually u use H for Homotopy lol

steel glen
#

your F is not well defined

#

you only said what F was at t=1 and 0

#

that’s ok if you just state them as properties

#

but that looks like a definition which is missing what happens when t in (0,1)

pseudo coral
#

its my guaranteed defromation

#

from identity to contstant

steel glen
#

yea i’m just saying you’re stating that as a definition of F

pseudo coral
#

continuous defomr

steel glen
#

but that’s not well defined

#

instead i’d say F satisfies those conditions

pseudo coral
#

yeah i wrote such that

#

and i swapped it to an H 🙂

steel glen
#

ok sure

pseudo coral
#

so its consistent

steel glen
#

also it’s not for a fixed p (arbitrary), it’s for the contraction point p

pseudo coral
#

ahh good point

steel glen
#

your proof for path connectedness makes sense to me

#

i’ll read the simply connected now

pseudo coral
#

ok

#

thanks

steel glen
#

i don’t agree with your proof for that

#

have you shown that in a path connected space, the fundamental group is independent of basepoint?

pseudo coral
#

yes we have

#

use that?

steel glen
#

use that and just consider pi_1(X,p)

#

yes

#

let gamma be in the group centered at p

pseudo coral
#

then I need a homotopy from the loop gamma to a single point

steel glen
#

i’m also a little uneasy as to how you claimed existence of the homotopy by just saying the space is contractible

#

i think you should construct the homotopy using the F you defined above

pseudo coral
#

so f(x)=f(gamma(t))=gamma(t) for t = 0

#

as gamma(t) \in X

steel glen
pseudo coral
#

thats sorta what i did

steel glen
#

i believe that’s what you’re saying

#

you should make it clear if so

#

because it just seems like you’re saying such a homotopy exists just by contractibilty, which is the whole point of the proof

pseudo coral
#

I suppose it’s that trivial then that the fund group is trivial

#

Since you’re given a map from identity to some contractible point

coarse night
#

it's trivial that ... is trivial.

gritty widget
agile chasm
#

thx

tidal lynx
#

isn't the definition of Y a category error

#

S^{n - 1} is the boundary of the (n-1)-sphere in R^n, so D_n is the closed ball in R^n

#

meanwhile X is just some arbitrary topological space

rancid umbra
#

boundary of the n sphere in R^n

#

D_n is the closed unit sphere in R^n

tidal lynx
#

right

#

I just said (n - 1)-sphere because people call a circle S^1 and not S^2 for some reason

rancid umbra
#

its because its a 1 manifold

tidal lynx
#

oh each point is contained in an open set homeomorphic to R^1, that would make sense

rancid umbra
#

yes

tidal lynx
rancid umbra
#

im not sure what you mean by category error

tidal lynx
#

I mean that X is not necessarily a subset of R^n

#

so taking its disjoint union with D_n is meaningless

rancid umbra
#

thats fine. you can form the disjoint union with any two top spaces

#

the definition of disjoint union doesn't require that the two spaces be contained in the same larger space

tidal lynx
#

I can take the disjoint union of X = {emptyset, {red}, {blue}, {red, blue}} and Y = R^n ???

#

wtf is that

#

well I guess the literal set X = {red, blue} but still

#

that's so whacky

#

what's the topological structed associated with it

rancid umbra
#

in general, X disjoint union Y is the set (X x {0}) U (Y x {1})

tidal lynx
#

do you mean Y x {1}

stark fog
#

it is like you're indexing the elements in the set so that you don't have intersection of elements from distinct (or maybe the same) set

hidden crag
tidal lynx
#

if they're from the same set then you can intersect I would think

rancid umbra
#

we can always form the union of two sets by the axiom of union, nothing is broken here

rancid umbra
stark fog
stark fog
#

like X disjoint union X, but for the first you do it with a_1, the second with a_2

tidal lynx
#

this is like the first time taking the union of two sets with know ambient space containing them, that's why this is weird to me

stark fog
#

in the sense that the elements now given by (x, a_1) and (x, a_2) don't have intersection

hidden crag
#

yeah that's what makes the union disjoint

stark fog
#

you can also make a wedge sum

#

like gluing sets in a point

hidden crag
#

indeed

tidal lynx
#

I see

rancid umbra
hidden crag
tidal lynx
#

formally why do we have to attach index sets to the disjoint union

stark fog
#

I know nothing about category theory yet

tidal lynx
rancid umbra
#

because you want to be able to explicitly distinguish elements from each set, particularly in the case where the two spaces you're unioning have elements in common, for example, the real line disjoint unioned with itself is two distinct copies of the real line

tidal lynx
rancid umbra
#

if you didnt tag the elements via an indexing set, you would just get the real line back, and thats already the regular union

tidal lynx
#

so really you can take the disjoint union of non-disjoint sets

rancid umbra
#

yes

tidal lynx
#

but in doing so you end up distinguishing the common elements anyways

rancid umbra
#

yup

tidal lynx
#

I am still having trouble understanding this definition

#

the set {p ~ f(p) \forall p \in \partial D_n} is supposed to be a subset of X, obtained by identifying points in S^{n - 1} with their image under f

#

but again, same issue (this time I don't see a resolution): what exactly is this identification doing? because points in S^{n - 1} are not contained/related to X

hidden crag
#

They are not contained/related to X yet, that’s what we’re trying to achieve

#

We’re gluing D^n to our space by gluing the boundary to its image under f

#

Drawing a picture will help here

#

I’ll go to sleep now but I’ll elaborate on this if you still have questions tomorrow

tidal lynx
#

alright thanks, I'll try to find images online

pearl holly
#

@tidal lynx I couldn’t resist drawing a small picture. The figure at the bottom is Y and the lines are supposed to indicate that “there’s a bubble within that area”. The boundary of D^2 at the top is marked with “zigzags”. This is when n=2. Hopefully this addresses your issue, otherwise wait for someone else I guess

#

But yeah this is basically what timo said (the map f is laying out the glue on X and you glue the boundary according to f), but I thought I would make a pic because they’re going to sleep soon like they said

stark fog
pearl holly
tidal lynx
#

I think I understand it better now thanks all, will think about it some more

#

Show that every compact subspace of a metric space is bounded in that metric
and is closed. Find a metric space in which not every closed bounded subspace
is compact.
what does "bounded in that metric" mean?

#

does it mean that if Y is the compact subspace in question and d is the metric, then there exists k such that d(x, y) < k for all x, y \in Y

#

i.e., there exists a "diameter"

#

or a better way of saying it: everyone in Y is contained in some open ball

tidal lynx
#

yeah I think this is right

coarse cobalt
#

helloo guys

#

for x,y elements of X does d(x,y) = 0 define a metric??

#

i think it follows all the axioms...

#

or should it be d(x,x) or d(y,y)??

hidden crag
#

you already mentioned an axiom it doesn't satisfy in the other channel

coarse cobalt
#

Thnx man hahahahha

#

i just still wasnt sure

hidden crag
#

if x is not equal to y then d(x,y)>0

coarse cobalt
#

yesss indeed.

willow viper
#

hello how can I determine the inner set of A in R^2 if A = Q x Q?

willow viper
#

uhm

#

like A° = {(q1,q2) ∈ R^2, where (q1,q2) is an inner element of A)}

gritty widget
#

thats called interior

willow viper
#

Oh

gritty widget
#

also idk what inner element is

willow viper
#

i see thanks

#

where (q1,q2) has an epsilon ball around it which is in A

gritty widget
#

what are your thoughts on the problem

willow viper
#

i don't know how to approach it

#

do I need to find an epsilon??

#

like I have to find an epsilon ball for any (q1,q2) in A right

hidden crag
#

maybe try to think about it conceptually first

#

Q in R and it's interior

#

i'm not sure how to give a hint without spoiling it entirely

willow viper
#

so do it for 1 dimensional and then Q^2?

hidden crag
#

yes

#

that would maybe be an easier way to approach it at least

gritty widget
hidden crag
#

hmm

gritty widget
#

you know, guiding someone, explaining the definitions etc

willow viper
#

Do i need to use that for any x in the reals the epsilonball of x always contains rational numbers?

hidden crag
#

remember that the ball you choose has to lie entirely in the rational numbers

#

so what problem might you run into

willow viper
#

that there are irrational numbers?

#

wait what

hidden crag
willow viper
#

so we cant find an epsilonball small enough so that it only contains rational numbers

#

but there are much more rational numbers than irrational

hidden crag
#

why do you think that

#

the rationals are countable but the irrationals are not

odd flame
hidden crag
#

i mean it's just

#

otherwise R would be countable

#

as union of two countable sets

odd flame
#

i mean yeah obv

#

but cantor = cool WanWan

willow viper
#

so A° = {} because there isnt any interior element

hidden crag
#

yes

willow viper
#

and if it's Q x Q then... its {} x {} = {}?

#

or is that a wrong conclusion

hidden crag
#

yes you can argue similarly for epsilon balls in R^2

willow viper
#

for A = Q x Q is the closure of A also = {} ?

gritty widget
willow viper
#

hmm

quick delta
gritty widget
#

I didn't want to tell them the answer but okay

willow viper
#

this definition is wrong for closure right? It should be epsilonball of a cap A is not equal to {}

#

where A is a subset of M and M is a metric space

#

because otherwise it wouldn't make any sense

gritty widget
#

Yeah

willow viper
#

Ok so the boundary of A would be RxR cap bar{RxR} then?

willow viper
#

uhm

#

what is bar{RxR} anyway..

gritty widget
#

closure of RxR

willow viper
#

ah

#

my mistake

#

it's RxR cap bar{CR^2}

gritty widget
#

hm. CR^2?

willow viper
#

the complement of R^2

gritty widget
#

the complement of R^2 is the empty set

willow viper
#

that's what I thought

#

So RxR cap {} = {} actually

#

noooo wait

#

this is getting very confusing now

gritty widget
#

its confusing for me too

willow viper
#

the boundary is defined as A \cap closure of complement of A

gritty widget
#

no

gentle ospreyBOT
willow viper
#

that's what I wrote?

gritty widget
#

no

willow viper
#

wait true

#

Ooooooook

pseudo coral
#

In showing a cont map from 2 sphere to itself such that g(x) \neq g(-x) is surjective do u utilise the Bursak Ulam Theorem

#

And suppose it misses a point

#

Then consider the stereo graphic projection of S2 \ the point to R2

#

Then compost this stereo graphic projection w g then apply the theorem

gritty widget
#

what do you think?

pseudo coral
#

I think that works lol

stark fog
hearty jacinth
#

Alternatively, the closure minus the interior

pseudo coral
pseudo coral
#

Also what’s the standard way of showing R2 minus two points has fundamental group that is free group on 2 generators

plain raven
#

explicitly deformation retract onto the figure 8

pseudo coral
#

Can I use van Jamie a

pseudo coral
#

Can Kampen

#

Can

#

Van

unreal stratus
#

Lol

pseudo coral
#

Lol

#

If I use van kampen I let my two open connected sets be R2 \x1 and R2\x2

#

Then they satisfy van kampen

tidal lynx
#

"a topological space X is sequentially compact if every sequence of points in X has a convergent subsequence converging to a point in"

#

This is probably implicit but the convergent subsequence has to be infinite right?

#

or else for every infinite sequence you could just have the subsequence be the first couple terms, and then the subsequence "converges
to the last term

gritty widget
#

sequences are by definition infinite

tidal lynx
#

oh ok

#

lol

#

this is a proof for:
If X is a metric space with metric d, then if A is a compact subset of X, then d(x, A) = d(x, a) for some a in A

#

basically the idea is, since d(x, A) is the infimum of the set {d(x, a) | a \in A}, we are guaranteed the existence of a sequence a_n such that d(x, a_i) converges to d(x, A). also in metric spaces compactness is equivalent to sequential compactness, so there exists a subsequence of a_n that converges to some a' \in A. Now I don't get why this means that d(x, A) - d(x, a') < eps for all eps > 0 (i.e., d(x, A) = d(x, a'))

untold lily
#

do you remember what the distance of the sequences was converging to?

tidal lynx
#

d(x, A)

untold lily
#

same holds for the subsequence

#

thus?

tidal lynx
#

calling b_n the subsequence, we have that for all eps > 0 there exists an index i such that d(x, A) - d(x, b_i) < eps

untold lily
#

exactly

tidal lynx
#

sooooo

#

is it true that d(x, A) - d(x, a') < d(x, A) - d(x, b_i) for any i though, if so then I will see why

untold lily
#

the b_i are converging to a', I recommend you try figuring out the rest

#

don't think you need more help just more time

tidal lynx
#

is the point that b_i converges to a' means that f(b_i) converges to f(a') for any function f

#

bc that seems sus

untold lily
#

no that's not the point and is nontrivial, f would need to be continuous

tidal lynx
#

if f is continuous probably but I'm overcomplicating it now

untold lily
#

although it is in this case

#

that is not what you are supposed to be seeing here

tidal lynx
#

hmm

#

lemme think some more

#

uhh triangle inequality maybe

untold lily
#

keep going

tidal lynx
#

since b_n is a subsequence of a_n, we have that d(x, b_i) converges to d(x, A)

#

oh

#

is that it

#

wait no

#

for any b_i in the sequence, by the triangle inequality we have that

d(x, a') < d(x, b_i) + d(b_i, a')

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as i gets bigger d(b_i, a') approaches 0

untold lily
#

yeah

tidal lynx
#

hmm I'm clueless

tidal lynx
#

but i don't directly see it in the algebra

tidal lynx
coarse night
#

what's the problem?

tidal lynx
#

I don't understand the last step to a proof

untold lily
tidal lynx
#

I see it geometrically

untold lily
#

if I give any hint here it would just solve the problem

coarse night
#

try showing that your new seq is a cauchy sequence

tidal lynx
coarse night
#

d(a,a')≤d(a, x)+ d(a',x) < 2 ϵ

#

(I should call them a_n and a_n_k but you get the point hopefully)

tidal lynx
untold lily
#

you said d(b_i,a') approaches 0

#

what does d(x, b_i) approach

tidal lynx
#

d(x, A)

untold lily
#

and you want to show d(x,a') < d(x,A) + e

#

or the opposite

tidal lynx
#

oh bruh

untold lily
#

w/e

tidal lynx
#

i just move the d(x, b_i) to the other side

#

d(x, a') - d(x, b_i) < d(b_i, a')

and I can make the d(b_i, a') guy as small as I want

cosmic beacon
#

this is a dumb topology question but I'm struggling to see how an inclusion of a deformation retract is injective

cosmic beacon
# cosmic beacon

The definition should also require that either ri = id_A or i is injective, right?

#

Yea, the assertion is false, right? Take A = R^2, B = R, i(x,y) = x, r(b) = (b,0), H(b,t) = b

broken nacelle
#

how do we know every open set in R is the union of countably many open intervals?

gaunt linden
#

Take all the rationals in your open set and add the maximal open interval that contains each.

#

An irrational element of your set will have an open neighborhood that contains a rational, so it is at least in that rational's maximal containing open interval.

broken nacelle
#

oh, ofc kongouDerp

#

dense sets

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that's clever

#

thank you catlove

broken nacelle
wispy veldt
#

its also the union of countable many mutually disjoint open intervals.

broken nacelle
#

also, @opaque cloud here's another example of why dense sets are useful

gaunt linden
#

No, the maximal open interval in an open set S containing a point x is well-defined and doesn't require choice.

#

It is (a,b) where a is the infimum of all y such that (y,x] subset S, and b is the supremum of all z such that [x,z) subset S.

opaque cloud
#

catking right

broken nacelle
#

the crucial part is this

#

oh, also

#

you can also use the fact that rationals are countable to disprove the fact that open sets with uncountably many disconnected components can't exist

#

since every open set contains rationals