#point-set-topology

1 messages · Page 222 of 1

sleek thicket
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This isn't a joke, I think a lot of math is justified in itself. Geometry is interesting because I like shapes. Number theory is interesting because the integers behave in bizarre but still vaguely predictable ways

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You can argue that this is bad and math needs external justification, but I think people tend to apply this principle selectively

gritty widget
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how dare you do something because it's interesting to you!?

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i don't like it therefore you can't do it

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(/s)

sleek thicket
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tterra I'm on your analysis TAs side now, you deserve it

gritty widget
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ok

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i dont give a fuck about that course anymore

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lol

sleek thicket
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based

gritty widget
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what i submitted on the final problem set is what im submitting

sleek thicket
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> submitting a screenshot from the student guide

gritty widget
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multiple people have already emailed the department and theyre going to look into it

shut moat
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I'm still stuck on the "on which topology" thing

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like there is no way the TA was serious

gritty widget
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:)

shut moat
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like that has to be spite

sleek thicket
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:)

obtuse meteor
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which topology of what?

gritty widget
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this person wasnt specifically talking about that course but, it was in the course's group chat, so probably

sleek thicket
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Which topology the determinant is continuous on

obtuse meteor
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b-bruh

sleek thicket
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Apparently this was unclear to the TA, faye

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anyways tterra yall should start a Google doc or something

gritty widget
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someone wrote "det is continuous" and lost marks for not specifying what topology

sleek thicket
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Put everything on there

gritty widget
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look i already started a list of infractions early in the semester but they picked up so quickly i had to stop

sleek thicket
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email the dept and ask for a refund or whatever opencry

gritty widget
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my last complex analysis problem set has three short problems

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and then three extremely long problems

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ugh i dont want to check these

obtuse meteor
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my last algtop pset

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makes me want to die

sleek thicket
gritty widget
sleek thicket
gritty widget
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my last analysis pset has killed me

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the job is done

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i am now dead

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👻

shut moat
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do some nice diff geo to revive you satisfiedblob

gritty widget
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yeah!

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im gonna work on my symplectic presentation tomorrow

sleek thicket
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Nice!

gritty widget
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i hope im not presenting first stare

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right now im the earliest time scheduled monkaS

obtuse meteor
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introducing the universal coefficients theorem

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on homework

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without defining tor

gritty widget
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one letter away from ugct

sleek thicket
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I'm typing up a long angerysad post on the discussion board for my cs course

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I just went to OH

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Showed up at 6pm, the start

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They didn't get to me by 7pm

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And this was the 2nd OH I tried to go to today

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So now I have to ask convince them that the homework is wrong via the discussion board

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Which is going to be a huge pain

fading vale
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????????????????????????????????????????

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????????????????????????????????????????????????????????????

gritty widget
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are u gonna upgrade from "firebomb?"

fading vale
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yes

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literally what????

gritty widget
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:)

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i need to add the disclaimer

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that this person was not specifying what course this was in

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but

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it's highly likely it was analysis :)

fading vale
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thats so fucking bad holy shit

gritty widget
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im losing good things to say about this school's math undergrad lmao

fading vale
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god.

gritty widget
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hold on

fading vale
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thats literally so fucked up holy shit

gritty widget
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completely normal grade distribution on a problem petTheCat

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ah yes

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93% of the class made the same mistake

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||"mistake"||

obtuse meteor
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so

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I have no idea how to compute

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tensor product of modules lol

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namely I need it over abelian groups

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oh wait hm

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I claim

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and this feels right

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that tensor product of G with Z/2Z is just G + G

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no

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G + G/2G?

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nah but it's like a graded thing

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idk how to write this with the structure theorem is the problem rip

tight agate
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it should be just G/2G

obtuse meteor
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yeah just found that out

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should thonk this for a bit

tight agate
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you can try proving something more general

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If R is a ring

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M an R mod

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I an Ideal

obtuse meteor
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sounds like effffort

tight agate
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them R/I (x) M iso to M/IM

obtuse meteor
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mhm

tight agate
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where the tensor product is taken over R

obtuse meteor
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yeah

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need to go over this bit of algebra

tight agate
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the proof is pretty much "choose the correct exact sequence and tensor with the right thing"

obtuse meteor
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hmm

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idk how tensor preserves exactness

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or when it does

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is tensor like always left exact?

tight agate
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right exact

obtuse meteor
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ah

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so can someone sanity check this computation?

marsh forge
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I believe it should be Z/2 in all degrees leq n

obtuse meteor
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oh yeah I cannot compute lol one sec

sleek thicket
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A more low tech proof would be to use yoneda

fading vale
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for a moment i thought you meant the homology sham and i was so confused

sleek thicket
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Oh lmao sorry

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I meant show that M (×) R/I has the same universal property as M/IM

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I guess this is just proving it preserves quotients, which is short of showing right exactness

fading vale
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hm cant you take ||0 -> I -> R -> R/I -> 0 and tensor by M? you get in general that I otimes M -> A otimes M -> R/I otimes M -> 0 is exact so if you prove that the first map is injective you're done?||

tight agate
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the first map is not injective in general

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but you dont need it

fading vale
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oh wait yes i am silly

tight agate
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IM is the image of the map

fading vale
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yeah

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haha

tight agate
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but yeah that's the proof

fading vale
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I otimes M is not always isomorphic to IM anyway hmmm so if it was exact you would have some problems lol

obtuse meteor
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@marsh forge I think you might be wrong when n = 1

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then I think H_1(RP^1, Z/2Z) = Z/2Z + Z

tight agate
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RP1 is the circle

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it should be just Z/2

frosty sundial
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(co)homology with coefficients in a field F will always be a vector space over F

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so you shouldn't have the Z term there

tight agate
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i think it's a typo

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probably missed the /2Z

sleek thicket
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Oh, max left again

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Maybe because they demoted him

frosty sundial
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i think that's the reason :(

shut moat
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why tf isn't ultraproduct honorable btw

frosty sundial
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we are trying

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ive suggested him several times

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the last reason was that they weren't going to promote anyone new while they were reworking the roles

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now that the roles are reworked, maybe some action will actually happen soon

gentle ospreyBOT
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No selfroles matching honorable.
See ,selfroles --list for the list of valid selfroles.

obtuse meteor
dusk heron
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The thing under the red line must surely be a typo, no?

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The negative sign should be on the y^k instead of the x^k.

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Well, I guess multiplication by $-i$ is also a complex structure on $\mathbb{C}^n$, but the standard complex structure is here referring to multiplication by $i$.

gentle ospreyBOT
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gustavn64

dusk heron
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@gritty widget Well, if the vector $(x^1,\dots,x^n,y^1,\dots,y^n)\in\mathbb{R}^{2n}$ corresponds to the vector $(x^1+iy^1,\dots,x^n+iy^n)\in\mathbb{C}^n$, then the complex structure should take it to $i(x^1+iy^1,\dots,x^n+iy^n)=(-y^1+ix^1,\dots,-y^n+ix^n)\in\mathbb{C}^n$, which corresponds to $(-y^1,\dots,-y^n,x^1,\dots,x^n)\in\mathbb{R}^{2n}$.

gentle ospreyBOT
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gustavn64

dusk heron
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Yeah, but on the previous page it seems like they're talking about i.

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The book is "Foundations of Differential Geometry, Volume II" by Kobayashi and Nomizu

plush needle
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If I have a space that is both arc and path connected, and given that hyperconnected spaces need not be path connected and ultraconnected spaces need not be arc connected, is there a stronger named condition that this space fulfils, like superhyperconnected?

gritty widget
strong heron
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This is the standard delta-complex structure on RP^2. My question is what goes wrong if we reverse the direction of c in this diagram?

honest narwhal
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Does something go wrong? Do a handstand and look at it

strong heron
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I mean, will it still be a delta-complex structure? I'm not very comfortable understanding this.

gritty widget
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it will be

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and it'll still be RP² is what sloth said (just swap U and L after reversing c)

strong heron
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Ah, I see. Thanks both!

fading vale
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pull a francaise and just call it miconnected

long hornet
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I want to show that, given any two points p, q on a connected topological manifold M, there is a chart domain containing both. I tried to use the fact that M is path connected and used a path p joining them, then I have a series of charts (V_t, g_t) for each point p(t). Now I let V be their union, and tried to show that it is a chart domain. But I am not sure about that.

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There is no obvious way to patch the g_t's together

sleek thicket
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A connected chart domain?

long hornet
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Oh, well, by chart domain I really mean a "coordinate ball"

sleek thicket
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Ah okay

long hornet
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So yes

sleek thicket
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In the terminology I'm familiar with the codomain of a chart can be any open subset of R^n

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This seems very very hard

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And possibly not true

long hornet
sleek thicket
long hornet
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Well, I know it's true for smooth manifolds (saw an answer online)

sleek thicket
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oh wow

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Can you link a proof?

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I'm surprised

gritty widget
sleek thicket
shut moat
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was just looking at a stack exchange answer

long hornet
shut moat
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oh wait this is smooth

sleek thicket
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I don't see at all why a chain of charts would have union a chart

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Np approx I was asking for thst

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Yeah, I think this same argument works

long hornet
sleek thicket
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So to prove there's such a homeomorphism

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Take a path connecting them

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Cover by finitely many charts

long hornet
sleek thicket
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Then do it in each chart

tight agate
long hornet
shut moat
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yeah I haven't gotten my head fully around it, but I'll think about it more after I finish this last min pset catThink

sleek thicket
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I outlined how to do so, right?

long hornet
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The proof I saw uses the "tubular neighborhood theorem". I think the idea is to take a path joining them and then a small neighborhood around it.

long hornet
tight agate
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I thought that this was false lmao

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wait

sleek thicket
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Ah yeah I don't think that argument would generalize

tight agate
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so we do not need to assume that mflds are hausdorff?

sleek thicket
tight agate
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or does the proof that there is a function taking one point to another use the fact that mflds are hausdorff

gritty widget
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I feel like the stack exchange answer just offloads the hard work to this theorem about f(a)=b (is it supposed to be obvious?)

sleek thicket
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I think it does brofib

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The proof I'm using would rely on compact sets being closed

long hornet
sleek thicket
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So brofib

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Connect the two points with a path

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Take a finite union of overlapping balls

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The union is your connected nbhd

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It suffices to show that in any coordinate ball, you can find an automorphism of the manifold sending one point to the other which is the identity on the complement of the ball

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Yeah?

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I would want to send the point to the other in R^n via a homeomorphism which is the identity outside a compact set

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These can be constructed in R^n by like, ODEs or whatever

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Then the compact set is closed in the manifold, so the complement is open and we can define the map globally to be the identity on the complement of that compacr set

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This is continuous by the gluing lemma

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Yeah?

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This uses that compact sets are closed in all of M

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Yeah?

tight agate
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ye

sleek thicket
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Which relies on hausdorffness

tight agate
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neat!

long hornet
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But isn't the union of these overlapping balls homeomorphic to a ball?

sleek thicket
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yeah

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You take a point in the overlaps

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Keep swapping

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x -> x1 -> x2 ->...-> y

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Each map is the identity outside the union of our balls

long hornet
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Yeah

long hornet
# sleek thicket yeah

So the tubular neighborhood theorem (if I understand it) also holds, I mean we can take a neighborhood containing the path

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Namely, the interior of the union of these overlapping balls that cover the path

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Is that right?

long hornet
sleek thicket
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What do you think the tubular neighborhood theorem says

long hornet
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I think it says what I said in the second message

sleek thicket
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That any path is contained in a connected neighborhood?

long hornet
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Yes, and that this neighborhood can be taken to be a coordinate ball.

sleek thicket
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this is not what the tubular neighborhood theorem says

sleek thicket
long hornet
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Well, I am not surprised. But I don't think it matters (I am interested in the statement I gave)

sleek thicket
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You don't know all of W is a a coordinate ball

long hornet
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W = union of the balls covering the path?

sleek thicket
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Wait I thought you were going off of the argument in the MSE post

long hornet
sleek thicket
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Must have misread, sorry

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I'm not sure what I was replying to there

sleek thicket
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Consider a path connecting the north and sole poles

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Of a sphere

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The union is a whole sphere

long hornet
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The union of what? I mean, which coordinate balls did you use?

sleek thicket
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The complements of the north and south poles

long hornet
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We can use a single coordinate ball, of course, but I think you mean some choices don't work

sleek thicket
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yes

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I mean when we choose finitely many coordinate balls covering a path

long hornet
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What if we take the minimal number?

sleek thicket
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We didn't have much control over it

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I don't know

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It seems unlikely

long hornet
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I agree. Too good to be true.

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Is there a nice bound on the least number of charts needed to cover a compact manifolds?

sleek thicket
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Do your charts need to be connected?

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I think an n manifold can be covered by n charts

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Let me find the reference

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No, that's not right

long hornet
sleek thicket
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It fails for the circle

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I know something about this though, hunting for it

long hornet
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Oh

sleek thicket
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n+1 charts

long hornet
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Neat

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Is it an easy exercise or a deep theorem?

sleek thicket
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idk

long hornet
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I see, thanks!

shut moat
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homework submitted hype

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it took me a concerning while to figure out how to show that a retract of a hausdorff space is closed

shut moat
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ok so this is unrelated to the main proof, but I've wondered why manifolds ppl more commonly define charts as maps from M to U

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like i get that it's equivalent

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but from an operational standpoint the way you use charts by, say, composing the inverse with functions suggests that embeddings from U to M might be more natural

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like just good ole parametrizations

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like even when defining vectors. Usually you take a chart phi, right. ∂i at p is the inverse dphi^-1(∂i_phi(p)), whereas with a parametrization it's more naturally just the pushforward of ∂_i

sleek thicket
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Sorry it's n+1 buncho

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Not n

shut moat
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same difference \o/

sleek thicket
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also maybe it makes it easier to talk about the overlaps of charts?

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I don't really know why we prefer charts to parameterization

shut moat
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so many conventions to get to the bottom of hmmm

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i rly want to be able to sit down at some point and motivate geometry/difftop with no ambiguity, but that's going to take a lot of experience

sleek thicket
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it's pretty cool

shut moat
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indeed

kind sluice
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Hey there

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im struggling with a problem regarding zariski's topology

sleek thicket
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hello

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What's the problem?

kind sluice
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Hi :D

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Ok so

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Im studying it from a topological point of view rather than algebraic

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Let $F$ be an infinite field

gentle ospreyBOT
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Maikel

kind sluice
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and let $\tau$ be the coarsest topology in $F^{2}$ such that every polynomial in F[x,y] is continuous

gentle ospreyBOT
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Maikel

kind sluice
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We are considering the cofinite topology in F btw

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I want to prove that the sets of the form {(x,y): p(x,y) != 0} are a basis for tau

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I used that fact to prove that $\tau$ is not the cofinite topology neither Hausdorff

gentle ospreyBOT
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Maikel

kind sluice
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I just havent been able to prove that tiny fact

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Sure, im sorry, its an arbitrary polynomial in F[x,y]

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Heck yes, its the preimage of F{0} by p

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i meant F - {0}

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which is an open set...

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and thus the proof is done

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How couldnt i see it

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hahah

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the set of all preimages by arbitrary p's in F[x,y] is a basis for the topology tau, right?

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Now i want to prove that the support of polynomials in F[x,y] is also a basis

gritty widget
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It is for sure a sub basis, I'm not sure how to show it is a basis

kind sluice
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isnt it closed under finite intersections?

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Hmm yeah it might not be a basis

gritty widget
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Wait

sleek thicket
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Ah sorry maikel

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I was distracted by irl stuff

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And forgot about your question

gritty widget
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But p!=0 and q!=0 iff pq!=0

kind sluice
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dw

sleek thicket
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So you want to show the zariski topology on F^2 is neither cofinite nor hausdorff?

kind sluice
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i already proved that, using this basis of the topology were talking about

sleek thicket
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Ah okay

kind sluice
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i just can prove its a basis

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Sorry, i proved its actually a basis, i just cant prove its a basis for the zariski topology

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The coarsest one that makes every polynomial continuous

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idk if thats the correct definition, its probably a particular case

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Im studying it as an interesting example in an undergrad topology course

remote beacon
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Zariski is non hausdorff right?

kind sluice
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Not if the field is infinite

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I cant use that fact though, since i just proved that using this basis

sleek thicket
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In which case?

sleek thicket
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Slim's is easier to work with

kind sluice
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yeah, im working with an infinite field

sleek thicket
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Slim I think "not if the field is infinite" was agreement

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Not a double negative

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It's emphasizing that it is hausdorff in the finite case

kind sluice
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Oh

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Yes, i was saying if the field is infinite, it is not hausdorff

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Basically, for any preimage U of any open set in F (cofinite top) by any polynomial in F[x,y], and any x in U, i want to find a set of the form V={(x,y):p(x,y)!=0} such that x in V c U

sleek thicket
kind sluice
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i.e i want to show the sets like V form a basis for that topology which i know as zariski's

sleek thicket
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Ah this is a good problem. These are called "distinguished opens"

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So what does an arbitrary open set look like?

kind sluice
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hmm

sleek thicket
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Also I agree, this is a bad topological space. It doesn't even have a generic point for each irreducible subset!

kind sluice
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i dont really know

sleek thicket
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Sure, so how did you do the previous part of the problem?

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Slim they said the definition wasn't in terms of closed sets

kind sluice
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the non.hausdorff part?

sleek thicket
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Yeah

kind sluice
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i proved every pair of elements from that basis couldnt be disjoint

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which in particular implies not-hausdorff

sleek thicket
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Right, so what's the basis? The preimages of cofinite sets in F?

kind sluice
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No, thats the thing. The basis i used is exactly the one i want to prove its actually a basis for the topology

sleek thicket
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Oh

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Okay I see the issue

kind sluice
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Basically i just need to prove this to end the proof

sleek thicket
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I want to make sure they know what the open and closed sets are

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And can justify it

sleek thicket
sleek thicket
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Ahh, I see

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Sorry, I didn't see that

kind sluice
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No worries!

sleek thicket
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I think it would be best if we tried to think about what the general open sets of F^2 look like first

kind sluice
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Seems like a good idea

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I just know they MUST be infinite

sleek thicket
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Hahaha

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They certainly are

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Okay so

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We know that they're all unions of the basis sets

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Yeah?

kind sluice
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Indeed they are... but whats the basis?

sleek thicket
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The cofinite-preimage basis I mean

kind sluice
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hmm ok

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So it was a basis at the end of the day?

kind sluice
sleek thicket
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I think it is a basis in this case but maybe that's not obvious

shut moat
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the set of (x,y) st p(x,y) !=0 can be rewritten as p^-1(F-0), yea?

sleek thicket
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So we would want to know that the intersection of any two basis set is a union of basis sets

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Right?

shut moat
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so doesn't that automatically grant that p^-1(F-0) is also open in the other topology bcz F-0 is cofinite

kind sluice
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hmm

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wouldnt we like to know if its closed under finite intersections?

sleek thicket
shut moat
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right, and the topology is formed by the subbasis of preimages of cofinite sets

sleek thicket
shut moat
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so double inclusion would do the job, I thought (as in for all x in one basis element, there's an element of the other basis contained in it)

sleek thicket
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Approx we're still working on the other inclusion

sleek thicket
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I know you can do this directly, I just wanted to give a more complete description of the zariski top

kind sluice
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what i said there is actually enough right?

sleek thicket
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It would be sufficient, yes

kind sluice
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its the definition of a basis

sleek thicket
kind sluice
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At least it implies it being a basis

digital peak
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if it's closed under finite intersection it's a basis

sleek thicket
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we need to know the sets p^-1(U) are a basis too

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Yes, I agree with that mniip

kind sluice
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Oh you were talking about an earlier message

digital peak
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(I have no context here)

sleek thicket
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My concern was with a different claim

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Yes maikel, sorry for the confusion

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What you said about bases is correct

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Sorry, we sort of fractured into two topics

kind sluice
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nice

digital peak
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zariski top PandaOhNo

sleek thicket
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Okay, let's back up

kind sluice
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Thanks

sleek thicket
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And know that the collection of sets of the form {x : p(x) ≠ 0} is a basis

kind sluice
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I already proved that second fact

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pretty straightforward

sleek thicket
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That you can cover intersections of any two elements by a union of others?

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If so, nice

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It is straightforward, p(x) q(x) ≠ 0 iff p(x) ≠ 0 and q(x) ≠ 0

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So with these two facts we can say that the collection of sets of the form {x : p(x) ≠ 0} is a basis for the zariski topology

kind sluice
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exactly

sleek thicket
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Yeah?

kind sluice
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The open set of pq does the job

sleek thicket
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I'm just making sure we're all on the same page

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Is why I'm reiterating stuff

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Because there were a couple discussions happening

kind sluice
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ok nice

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seems we are

sleek thicket
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Right

kind sluice
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we need to prove my earlier message

sleek thicket
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So what does U look like?

kind sluice
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Ok, it looks like {(x,y): p(x,y) in A for p in F[x,y] and A cofinite in F}

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By definition... idk if youre seeking for a different answer

sleek thicket
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That's all I'm asking

kind sluice
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Ok nice

sleek thicket
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Let's enumerate the complement of A

kind sluice
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Ok

sleek thicket
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b1,...,bn

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Yeah?

kind sluice
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Perfect

sleek thicket
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So what does p(x, y) in A mean in terms of these bi?

kind sluice
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p(x,y) != b_i for i in {1,...,n}

sleek thicket
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Right

kind sluice
#

oooh i think i see it

#

are you going to try the product of (p-b1)...(p-bn) ?

sleek thicket
#

Right, so this is zero iff p = bi for some i

kind sluice
#

which is not

sleek thicket
#

So this is nonzero iff p ≠ bi for all i!

kind sluice
#

Niceee

#

i knew it was something like this

sleek thicket
#

Hahaha

kind sluice
#

So thats the V i was seeking for right?

sleek thicket
#

Yup

#

And actually V = U

kind sluice
#

Wow

sleek thicket
#

But maybe you need to union some of these together for varying p

#

To get every open set

kind sluice
#

so its the same V for any x in U...

sleek thicket
#

Yeah, but only because the U we started with is super special

kind sluice
#

Oh, yes

#

Youre right

#

for a more general open set i'll have to consider unions

sleek thicket
#

Yup

#

Here's a tricky problem

#

So let D(f) = { (x, y) : f(x, y) ≠ 0 }

#

We've shown this is a basis

#

It's closed under finite intersections and any open set is a union of things like this

#

yeah?

kind sluice
#

Yeah

#

this feels so AG although ive never taken a course

#

Not yet hehe

sleek thicket
#

Show that for any open set U, there are finitely many f1,...fn where U = D(f1) union ... union D(fn)

#

Well that's because it is AG!

#

This is saying that any open set is compact

kind sluice
#

Oh so its a special basis in which all open sets are generated by finite unions? :O

sleek thicket
#

Nah, it's about compactness

#

Not the basis itself

#

If you have a basis B for a space and a subspace Z, Z is compact iff every cover of Z by elements of B has a finite subcover

kind sluice
#

I mean i see the compactness def in there actually

#

Yeah, exactly that hehe

#

But is what i said wrong?

sleek thicket
#

It's not wrong but it's the same as saying "every open set is compact"

kind sluice
#

That means open sets are finite unions of the basis

sleek thicket
#

And it works for any basis

#

It's a property of the topological space which doesn't depend on any particular basis

sleek thicket
#

Wait, no

#

I am lying

#

Yeah sorry you're right

#

If we required this for all possible unions of basis sets it would be compactness

#

But you're just saying there's some union

kind sluice
#

Yeah yeah

sleek thicket
#

Anyways, the property that all open subsets are compact is called being noetherian

#

It's pretty important in AG

kind sluice
#

Ooooh

#

Ive heard about that rings before

#

just the name

sleek thicket
#

Yup! It's equivalent to the ascending chain condition on open sets

#

For rings it's the ascending chain condition on ideals

kind sluice
#

the one in PIDs?

sleek thicket
#

Hm, I'm not sure what you mean

#

PIDs are noetherian, so they satisfy the ACC

kind sluice
#

PIDs are the ones in which that condition holds for ideals

#

If i remember correctly

#

Ooh i think i see

sleek thicket
#

No, this is not true

#

also mniip sorry for clogging chat

#

Feel free to ask your questions about spherical stuff

kind sluice
#

Hey thanks for all the help

#

it was quite easy actually, i was just too tired to think properly

gritty widget
sleek thicket
#

It happens to all of us :)

#

Except tterra

#

He's just like that by default

kind sluice
#

lol hahahahaha

gritty widget
digital peak
kind sluice
#

now i gotta figure out some ergodic theory stuff

sleek thicket
#

Ooh

#

Very exciting

gritty widget
#

role collector

sleek thicket
#

That's me but in 2022

#

Let's go people

#

#shamforowner

gritty widget
#

,ban mniip

gentle ospreyBOT
#

This may only be done by a moderator!

kind sluice
#

wanna help me too? hahah

digital peak
#

We have $SO(3)$ acting on $\mathbb{S}^2$ in the usual way, and is thus acting on the vector space of functions $\mathbb{S}^2 \to \bR$. I'm being asked to find invariant subspaces under this action. Now I'm vaguely aware of the spherical harmonics being related to this but I'm struggling to find a concrete connection. How does the laplacian come into play? Why do the polynomials have to be homogeneous? $\dv[2]{x}+\dv[2]{y}+\dv[2]{z}$ seems to suggest a connection to $x^2+y^2+z^2=1$?

sleek thicket
#

Rip

kind sluice
#

F

gentle ospreyBOT
sleek thicket
#

All functions?

#

Big space

digital peak
#

sure but polynomials are dense or something

sleek thicket
#

Only in continuous functions

digital peak
#

well ok, not "all" all

#

yeah cts functions

sleek thicket
#

Seems hard

digital peak
#

thanks catThumb

sleek thicket
digital peak
#

the thing is that this is a problem that's trying to like motivate irreducible representations of so(3)

#

and all I could find on the internet about this is "follows trivially from irreps of so(3)"

sleek thicket
#

lol

gritty widget
#

Huh, so3 cannot permute (x, y, z) to whatever right? Does this mean the invariant polynomials don't need to be symmetric?

digital peak
#

it's not about the specific invariant polynomials, rather spaces of them

gritty widget
#

Ah right

digital peak
#

for example, restrictions of linear functions to the shere is clearly an invariant subspace

sleek thicket
#

Any function gives an invariant subspace via it's orbit

#

and this will be pretty small

#

Seems really hard to classify all of them

#

I am thinking

digital peak
#

I suspect these are orbits of like x^l

sleek thicket
#

Sorry, I'm not sure what you mean

#

Like I don't think for every f there's such an l

digital peak
#

does it sound believable that any polynomial is a linear combination of rotations of x^l

sleek thicket
#

where f(Ax) = x^l for some l

#

oh only polynomial

#

Sorry

digital peak
#

well

#

for "all cts functions" we use density

sleek thicket
#

To show what?

digital peak
#

this is schauder basis vibes not hamel basis vibes

sleek thicket
#

I feel like moving will fuck up the subspace

#

like if you're in some invariant subspace

#

Which is like a proper subset

#

You can always move ε in some direction and leave

digital peak
#

yes

#

ok let's restrict our attention to just the polynomials

#

the other part is outside of the scope of the problem

#

so we have polynomials in x,y,z restricted to the sphere, with SO(3) acting on them

sleek thicket
#

Right

#

so any polynomial is a sum of things like a x^l

#

but you can't fold like the a into a rotation

digital peak
#

?

#

let A be the 45 deg rotation in the xy plane

#

then A(xy) = (x^2-y^2)/2

#

and A^2(x^2) = y^2

#

so we have A(xy) = A^-1(x^2)/2 - A(x^2)/2

#

so we have
$$px^2 + qxy + ry^2 = (p + \frac{A^{-1}q}{2} - \frac{Aq}{2}+rA^2)x^2$$

gentle ospreyBOT
sleek thicket
#

Hm you're right

digital peak
#

now how does this generalize to higher orders I have no idea

#

there's probably a similar connection in 2D, between fourier and polynomials and the laplacian in the circle

#

damn wish I did more in my first PDE class

#

tf is this notation

#

|.|^2 being r^2?

#

what is this

kind sluice
#

@sleek thicket are you still here?

sleek thicket
#

yup

#

sorry for not being able to help mniip

sleek thicket
digital peak
#

yeah I think I get what it does now

sleek thicket
#

like evaluate the first poly at the laplacian to get a differential operator

#

👍

#

weird that it's like, conjugate-symmetric

digital peak
#

we're defining <x^k, x^m> = k! delta_km

sleek thicket
#

ah okay, less weird

digital peak
#

and <x^k, y^m> = 0

sleek thicket
#

anyways yes maikel i'm here

kind sluice
sleek thicket
#

we showed that they're equal

#

I said iff

kind sluice
#

Right you said they were equal

sleek thicket
#

yup

kind sluice
#

i dont get why tho

sleek thicket
#

(p(x)-b1)...(p(x)-bn) = 0 iff p(x) = bi for some i

#

do you agree with this?

kind sluice
#

Totally

sleek thicket
#

so (p(x)-b1)...(p(x)-bn) ≠ 0 iff p(x) ≠ bi for all i

#

iff p(x) in U iff x in p^{-1}(U)

#

p(x) ≠ bi for all i iff p(x) in U because U is the complement of b1,..,bn

kind sluice
#

Yup, i think its pretty clear put in that way

#

Let me write it to make sure i do get it

#

I do, thanks! :D

gritty widget
#

Does anyone have a good answer to this? Diffeological spaces seems like a very nice generalisation of manifolds. But they do not seem to be very popular?

#

Is this just because, the kind of stuff looked in differential geometry is inhernitaly non categorical, e.g. you often are looking at a specific manifold with a specific metric and really working in that manifold

#

or is it just that the theory isn't well developed

cold vine
#

Does anyone have a hint for the following: Given a cofibration i:A->X and Y contractible, any map f:A->Y has extension g:X->Y

#

This is the definition I'm working with

#

Thus it's quite difficult since it assumes a map X->Y which is what we want here. At least since Y is contractible and if we have that a map X->Y it is is nullhomotopic which gives us a homotopy to extend the restriction to A, but this doesn't immediately help

cold vine
#

Similarly I'm trying to show that fibration p:E->B where B path connected gives us from Y contractible f:Y->B has a lifting f:Y->E but here I have a similar problem

frosty sundial
#

Basically, G should be the homotopy which takes g: A --> {y} to f: A --> Y

#

the first map g is the restriction of the map X --> {y} \subset Y

cold vine
frosty sundial
#

np and gl, sorry i cant look at your second question cuz i have to go run now

#

but maybe a similar idea works

cold vine
scarlet mist
#

Not sure if this is the right place to ask this, but in Example 2.1.6 (b), why is there no square root on the LHS? Are they just not using the Euclidean metric?

gritty widget
#

it doesn't really matter

#

1 = √1

scarlet mist
#

Oh right, yeah

#

Thank you

#

That seems like a really dumb question now

gritty widget
#

lol

cold vine
#

Dont we have that maps from contractible space to path connected space are homotopic? I think this is true since isnt [X,Y] a one point space when X contr. and Y path conn.?

obtuse meteor
#

yes this is true

cold vine
#

great!

uncut surge
#

I guess the proof is as easy as you'd imagine; first you use contractibility to show that any map is homotopic to a constant one, and then path-connectedness implies that all constant maps are homotopic

shut moat
#

Advisor approved, I'm taking grad manifolds next sem pandaHugg

gritty widget
sleek thicket
#

Nice!!!

plush needle
#

I am working on a paper, and I've realized that I can create "boxes" in order to investigate the particular space the box is embedded in. I know x_1 and x_2 are colinear, and y_1 and y_2 are colinear, and I can get expressions for the lengths of the sides of a box. Now I'd like to be able to, given this and possibly other (but few) conditions, figure out the metric. The image shows an example of a box in a familar space.

#

Note that the box is not drawn to scale. In this particular case, letting x_1 = y_1 = 0 will collapse the box to a triangle, for which the side lengths correspond to what you would get using Pythagoras. I would, however, like to find the metric without tricks like that, since I will be getting more exotic boxes than this example.

shut moat
#

I could be wrong but I don't think this is nearly enough information to determine a metric

#

because the metric can change completely arbitrarily away from the box you've drawn

#

well not "completely arbitrarily" but you know what I mean

viral atlas
#

I think the question here probably is: given fixed real values x_1,...,y_2, can we determine a metric which ensures the above dimensions correspond to a convex quadrilateral in R^2?

plush needle
#

@shut moat Indeed. But what if I could arbitrarily move such a box around the space and see how the lengths of the sides change?

#

It's as if I have two halves of a metric. I know how to measure distance between two points on the same straight line, and I know how to measure the distance between two points on two different straight lines. But, I don't know how to measure the distance between two arbitrary points.

uncut surge
#

Oh, hm, that actually sounds very interesting. So the mathematical version is something like "if I know all values d((x,0),(x',0)) and d((0,y),(0,y')), can i deduce what the metric is on general points d((x,y),(x',y'))"?

plush needle
#

Exactly.

uncut surge
#

It feels like the answer might be no, since metrics can get really freaky, but I'll think about this for a bit

#

Since in this kind of formulation, I will never be able to say anything specific about terms of the shape, d((x,0),(0,y)), except some very very rough estimates, since it's smaller than d((x,0),(0,0)) + d((0,0),(0,y))

#

The French metro metric comes to mind, not sure if that's an interesting example here

plush needle
#

But I know the side lengths too, d(x,y) and d(x',y'), but not d((x,y),(x'y')).

uncut surge
#

Alright yeah I think I getcha; so my original formulation wasn't quite right

cold vine
#

I found a material claiming that from the claim here follows that restriction of a fibration is a fibration. What is the pullback of the inclusion which makes this clear?

uncut surge
#

So this metric looks simply like d(x,y) = |x| + |y| on all sides of squares (outside of sides of squares which lie on coordinate axes), but if x is collinear to y, it turns into a different metric

cold vine
plush needle
#

@uncut surge Ah, indeed. So there would be a way to circumvent most attempts with some exotic metric then.

uncut surge
#

Maybe! I've not thought about all the details yet, but this metric breaks a lot of "intuitive" things that one would like to do with metrics

#

So it's definitely a good example to check

plush needle
#

What if it was sufficient to find a metric, and not the metric?

uncut surge
#

@cold vine I know this more in the context of bundles, but there, the restriction of a fibration E -> B corresponds to taking a subspace A of B, not a subspace of E

#

Then the fibration P -> A is also supposed to have the same fibres as E; so yeah, restrictions of bundles/fibrations are restrictions to smaller parts in the base space; https://en.wikipedia.org/wiki/Pullback_bundle maybe this article gives some better intuition

In mathematics, a pullback bundle or induced bundle is the fiber bundle that is induced by a map of its base-space. Given a fiber bundle π : E → B and a continuous map f : B′ → B one can define a "pullback" of E by f as a bundle fE over B′. The fiber of fE over a point b′ in B′ is just the fiber of E over f(b′). Thus f*E is the disjoint union...

#

@plush needle If you just wanted some metric, you might be able to do something with infimum-constructions perhaps?

#

I'm thinking something like "d(x,y) = infimum of all the sums of sides-of-square-lengths which go from x to y"

cold vine
#

Ah alright! I guess this still helps me since I'm trying to show that p|E0: E0 -> p(E0) is a fibration, where E0 is a path component. I have already shown that image of a path component is a path component

uncut surge
#

So if you have a bundle $\pi: E \to B$ and a map $f: A \to B$, then the pullback bundle $f^* E \to A$ is defined as $f^* E := { (a,e) \in A \times E : f(a) = \pi(e)}$

gentle ospreyBOT
#

Lartomato

uncut surge
#

I suppose you can do exactly the same thing with pullback fibrations; now the only thing to do is to show that E_0 \to p(E_0) is the same as this definition of the pullback fibration under the inclusion map p(E_0) \to B

#

would be weird if it wasn't

cold vine
#

Ahh alright! thanks

obtuse meteor
#

we're spending the last week of my manifolds in R^d class talking about Riemannian metric

#

@sleek thicket would be happy

sleek thicket
fading vale
#

only the personality of his that likes riemannian geometry

#

his other personality is filled with rage

sleek thicket
#

LEVI CIVITA CONNECTION

gritty widget
#

MINUS!

sleek thicket
#

COMPACT

gritty widget
#

STOP

#

,ban slimvesus

gentle ospreyBOT
#

This may only be done by a moderator!

sleek thicket
#

me and the boys proving pi using the Levi civita connection on a compact manifold

gritty widget
#

a smooth function on M is just a section of the trivial bundle M x R cocatThink

#

everything is bundles

sleek thicket
#

correct

fair idol
#

Is convex geometry still an active area ?

sleek thicket
#

Tterra and I were very stupid about compactness in vc the other week

#

> cotangent bundle is the first example he gives me of a symplectic manifold
> on a compact symplectic manifold, all even cohomology groups are nontrivial, and in particular the symplectic form is exact
> the symplectic form on the cotangent bundle is defined as the exterior derivative of something

#

it took us like half an hour to realize that thr cotangent bundle isn't exact

#

It literally contains vector spaces in it as closed subsets. It's a fucking bundle!!!

#

I forget where proving pi is from

gritty widget
sleek thicket
#

oh lol yeah

gritty widget
#

||no longer honorable||

cold vine
#

Hmm, does anyone have a tip on showing that if $Y^I$ is the free path space and $p:Y^I\to Y, \omega \mapsto \omega (1)$ then $p$ is a homotopy equivalence

gentle ospreyBOT
bright acorn
#

While the Eilenberg-Steenrod axioms give you a nice framework to study simplicial, singular homology and other homology and cohomology theories of topological spaces, I was thinking if there is a similar set of axioms used to study homotopy groups.

#

Is there such a thing?

#

I still haven't studied more advanced homotopy theory

#

So I got a bit curious

tawdry widget
#

How is the topology on Y^I defined?

obtuse meteor
#

Presumably C(I, Y), [I, Y], or similar

#

and usually we use the compact-open topology

#

so if you have a compact subset K of I and an open set U of Y, then the set of all functions f : X -> Y so that f(K) is contained in U is denoted V(K, U), and then V(K, U) is a subbasis for the topology on [I, Y]

tawdry widget
#

It’s a little long though...

tawdry widget
#

Wait... I made a mistake at the end,there still remains one step I haven’t completed yet...:

#

done:

cold vine
# tawdry widget

Thanks so much! Yeah C(I,Y) should be good here since it's the free path space. Yeah I got some of that but it was super mechanical 😛

lyric wadi
#

Hey, so I'm trying to prove the universal coefficient theorem for cohomology with integral coefficients directly (so not invoking the theorem for general coefficients), and I've managed to reduce the problem to here but I'm having a hard time working out why the torsion of H^n(X;Z) should be contained in Ker(h)

#

I guess that since we have that every element of the kernel of h is a coboundary, we have that something messes up when we try to extend the element to work on any chain

rotund thicket
#

What is the intuition of having a continuous function f : X -> Y and Y being Hausdorff?

rotund thicket
#

For example, in a problem if f, g : X -> Y and f(x) = g(x) for all x in D where D is dense in X and Y is Hausdorff, show that f(x) = g(x) for all x in X.

#

I'm asking how to think about the importance of Y being Hausdorff

#

I guess if $x \in U$ and $y \in V$ both open sets, then $f^{-1}(U \cap V) = f^{-1}(U)\cap f^{-1}(V) = \emptyset$

#

that's the importance

gentle ospreyBOT
#

Trichloromethane

rotund thicket
#

i think i answered my own question lol

#

so $f^{-1}(x) \not= f^{-1}(y)$ if $x\not= y$?

gentle ospreyBOT
#

Trichloromethane

rotund thicket
#

or even stronger that $f^{-1}(x) \not\subset f^{-1}(V)$

gentle ospreyBOT
#

Trichloromethane

rotund thicket
#

I forgot im dealing with pre-images

#

oh yeah you're right lol

#

well im asking how to think about the assumption that the codomain is Hausdorff in the context of a continuous function

#

well for this one U and V are open sets containing x and y respectively

#

I understand that

#

yeah i guess that's sort of what im thinking

#

well my understanding is that for any two points in the codomain, there exists disjoint neighborhoods containing each

#

therefore the pre-image of these sets is disjoint (by prop. of pre-image)

#

i suppose the useful thing about this is that these are disjoint open (by continuity) pre-images

#

well if im trying to solve the problem then yeah

#

well, im asking somewhat of an open-ended question

#

because ive seen this assumption that the codomain being hausdorff quite often

#

oh yeah

uncut surge
#

Hausdorffness is just a very common property in general, and generally tells you that you can freely switch between points and open sets, in a sense

#

There's nothing super special about codomains being Hausdorff, since generally, Hausdorffness is not super special (in most areas of mathematics); but it is very useful, since it means that you can distinguish points, topologically

#

And the way you should use it in proofs is generally always the same: Try to somehow force two points to be unequal, and then Hausdorffness gives you disjoint open sets for free

#

And open sets are cool to combine with continuous maps; specifically, if you form their preimage, you get something open again. Hence, I guess, that's why your Hausdorffness condition may often show up in the codomain: Then the open sets you get in the codomain can be preimaged immediately

#

tru

rotund thicket
#

yeah it feels like most of it is just going back to the definitions

summer jolt
#

What is the meaning of the notation: $([-1,1] \times {-1,1})$?

gentle ospreyBOT
#

snypehype

summer jolt
#

No without the round brackets

obtuse meteor
obtuse meteor
obtuse meteor
drifting sundial
#

the way I like to think about Hausdorffness is that there cannot be "infinitely close" distinct points

#

but yeah to prove stuff you have to fall back on the precise defn

strong heron
#

Let X be the 2-sphere with two points {p,q} identified. I am supposed to find the homology groups of the pair (X,X-[p]), where [p] denotes the equivalence class {p,q}.

#

However, I'm not supposed to use the homology of X for my computation. I feel I must use excision somehow, but can't figure out how.

#

Won't a small neighbourhood of [p] be like a cone with vertex at [p], and then using excision we can conclude that the required homology is same as that of (D^2, D^2-{point})?

uncut surge
#

A neighbourhood of [p] won't satisfy the condition that you need for excision though, right? You need an open set in the sphere whose closure is also in the interior of X - [p]

#

I'm thinking if you take p and q to be the north- and southpole, excision of an open band around the equator might be bettah?

#

Also a neighbourhood of [p] is less like a cone and more like two cones glued together at their vertex

#

@strong heron wheee

strong heron
strong heron
uncut surge
uncut surge
#

I imagine the long exact sequence in homology might bring happiness and good luck then

strong heron
#

U-[p] is two disjoint circles, right?

uncut surge
#

Ye that's what I'd think

strong heron
#

So we get $H_n(U,U-[p]) \cong \tilde{H}_{n-1}(U-[p])$

gentle ospreyBOT
#

whysee

uncut surge
#

For n >= 2 ye

#

In the part of the long exact sequence where degree zero pops up you need to be careful but it doesn't get too complicated there either

strong heron
#

Yeah, that's right. But this means I seem to be getting H_2=Z+Z

#

But when I actually used the homology of X initially and calculated the homology of (X,X-[p]) using the long exact sequence, I got H_2 to be Z.

#

I'm confused 😦

uncut surge
#

hmmm i hope i didn't mess up either

#

mhmmmm maybe i did

strong heron
#

What's that? Did you figure it out?

strong heron
uncut surge
#

Mhm, no, I'm not sure yet; One can think about X as a wedge sum of a sphere and a circle, but even knowing that, the Long exact sequence with the pair X, X - [p] doesn't become immediately conclusive

#

How did you get that?

#

At least H_2 = Z^2 and H_1 = Z would be consistent with the long exact sequence I think

#

but H_2 = Z and H_1 = 0 as well lol

strong heron
#

X-[p] is a cylinder, right? So, it is a circle upto homotopy.

uncut surge
#

Yea

strong heron
#

What I thought is that the map H_1(X-[p]) to H_1(X) in the l.e.s. will be an isomorphism, no?

uncut surge
#

Hm, don't think so actually; if you embed the cylinder back into the space X, then the nontrivial loop around the cylinder becomes contractible on the sphere

#

So I think that map has to be zero, and then the H_2 = Z^2 and H_1 = Z result must be true

strong heron
#

Yeah, I think I can see my error now.

uncut surge
#

But yeah, the analysis of that morphism was exactly the necessary step that I was missing; now I get it too

strong heron
#

So our H_2 is settled with the other method also now

uncut surge
#

Yeah, I believe so!

#

I'm always so happy when these mystical LES-calculations work out, lol

strong heron
#

True, me too

#

Pretty good, thanks!

#

All looks settled now

uncut surge
#

No problem, glad to help!

pastel thistle
#

Hi

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Any way of proving that R^n\Q^n is connected ??

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I prove it for n=2 and I would like to use induction but Im stuck

marble socket
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show that its path connected!

pastel thistle
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I know is kinda obvious but I wanted a formal proof

pastel thistle
marble socket
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yea so take 2 points and consider a 2d-plane passing through the 2 points

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there are uncountably infinite lines passing through the first point lying on the plane.

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but there are only countably many points with rational coordinates

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so you can find lines passing through the 2 points which don't contain any points with rational coordinates

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but since there are many such lines, you can find a pair of intersecting lines, giving you a path between the two points

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(the claim is false for n = 1)

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like the same proof shows that R^n \ any countable set is (path) connected.

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for n>=2

pastel thistle
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I understand

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Mmm okey thank you

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😀

marble socket
uncut surge
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holy shit i've never heard of that proof before this is beautiful

barren sleet
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that is a very nice proof

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and i never thought of that before

summer jolt
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Is there a nice way formula for the deformation retraction of a filled square with its centre point removed onto its boundary?
I’ve been trying for quite a bit and couldn’t find it. What I can see is that the points should mapped along the line passing through that point and the centre onto the boundary.

strong heron
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You can perhaps consider the unit square centered at the origin and then for a point (a,b) just consider the line bx-ay=0 and check where it meets the edges of the square.

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You will get 4 regions corresponding to the 4 edges of the square from the lines x-y=0 and x+y=0.

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This map is from the square to its boundary and it will descend, via quotient maps, to give a map from the torus to its boundary.

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I think writing it out must not be very difficult.

summer jolt
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@strong heron I see yes dividing the problem into 4 different parts seems reasonable as one the end coordinates of the line will be known and I would just have to determine the other one.

gritty widget
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@obtuse meteor I love differential geometry and Topology. Do you love?

obtuse meteor
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I do indeed love

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I love topology and many women

gritty widget
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I agree

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I love Riemann Geometry.

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riemannian geometry is pretty good

barren sleet
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"Do you love?" what a deep question

gritty widget
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$R_{\mu \nu}$

gentle ospreyBOT
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Sigma, o Liestinche

gritty widget
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Look it

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curvature and topology on complete riemannian manifolds flonshed

sharp yoke
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I think i proved the forward direction correctly

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having a bit of trouble with the reverse direction

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i tried some stuff with projections/component functions but nothing was shaking out

sleek thicket
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Huh, that's my first instinct too

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I thought that you could check smoothness locally and in each chart take f to be the coordinate functions

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Then f ° F should be the components of the local representation of F, so if they're all smooth then F is smooth on the chart

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What went wrong for you?

sharp yoke
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i think im doing something wrong proving the coordinate functions are in $C^k(N)$

gentle ospreyBOT
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『Urahairywizard』

sharp yoke
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Around a point in N you have a chart containing that point. And then the chart composed with your coordinate function will be C^k on your coordinate neighborhood, not necessarily on your entire manifold N

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i could be talking nonsense tho

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im thinking that to apply the assumption, we need our small f to be defined on all of N right

delicate hollow
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Quick question: I am told a subset A in R^2 is bounded, prove that A complement has only one unbounded component

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But if I take an example like a closed disc in R2

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that is bounded right?

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but the complement of its components are both unbounded.

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since any number not in a unit disc counts and that can any point where x^2 + y^2 > 1

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or I dont understand what componenets are

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I think I dont :/

sharp yoke
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could be talking about connected components but idk

barren sleet
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complements are everything not in the set

delicate hollow
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yeah its connected componenets

barren sleet
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the complement of the closed disc is one connected component

delicate hollow
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that would only make sense

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I thought components were (x,y) like the individual parts

sharp yoke
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you just gave a counterexample to that so

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pretty sure its the connected components

delicate hollow
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yea

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ok

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any examples of sets not open or closed in R2

barren sleet
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yes

delicate hollow
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ok

barren sleet
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plenty

delicate hollow
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nvm

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i got one

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Q^2

barren sleet
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ye

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yes

delicate hollow
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components are kinda weird for me to visualize ngl

barren sleet
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even simpler, [0,1)x[0,1)

delicate hollow
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so

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thats a box

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where

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top right vertex has two adjacent open sides

barren sleet
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yeah

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kind of

delicate hollow
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does open unit disc with point at (0,1) count?

barren sleet
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wdym

delicate hollow
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is it an example

barren sleet
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oh

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yes

delicate hollow
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of a set open nor closed

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ok

barren sleet
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yes

delicate hollow
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idk

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so

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I think I can give a definition of bounded

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lemme try

barren sleet
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do you know a topological definition of connected?

delicate hollow
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yeah

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like um

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no seperation

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or better

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no clopen sets?

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wait

barren sleet
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using the definition of bounded and the definition of connected makes the exercise easier to prove

barren sleet
delicate hollow
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yea

barren sleet
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other than the empty set

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some people consider that proper

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others dont

delicate hollow
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i like thinking in terms of no seperation though

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thats the definition im super comfortable using

barren sleet
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so getting intuition for why the definition is that way?

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there is some nice intuitiom for it

drifting sundial
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@barren sleet we talked about this before

delicate hollow
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wait

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is it quick?

drifting sundial
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something about sets touching each other

delicate hollow
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oh

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no seperation is super intuitive to me

barren sleet
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it's easy you first consider metric spaces

delicate hollow
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but no clopen is weirder

drifting sundial
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basically if it's disconnected, then there are disjoint sets that don't touch each other

barren sleet
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I can talk later

drifting sundial
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I.e. they have no boundary

barren sleet
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I will explain

delicate hollow
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wait

drifting sundial
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and you can prove that clopen sets are precisely the ones with no boundary

delicate hollow
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bruh

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bounded means no boundary 🤦‍♂️

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wait

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bounded means there is a boundary

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or that the boundary is included

drifting sundial
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uh bounded and boundary are completely unrelated

delicate hollow
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hmm

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ok

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so

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my def of bounded

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A is bounded iff for all x in A m<=x<=M

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but

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in R2

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this means that for all (x,y) in A, m_x<=x<=M_x and m_y<=y<=M_y

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thats what i remember atleast

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and it makes the most sense

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is it right?

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bruh

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i think I found an answer to my exercise by just browsing SE

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i wasnt searching for answer though, this is unrelated

sharp yoke
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literally found this in 2 seconds

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@sleek thicket does my problem makes since btw?

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sense*

sleek thicket
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Ah yeah I see

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This is a really good catch

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But you can extend via a bump function

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So say you want to check that F is smooth on a neighborhood of a point p

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Choose a chart with coordinate x^1,...,x^n containing p

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Choose a smaller neighborhood U of p (one with closure contained in the chart) and a C^infty bump function φ supported in the chart which is identically 1 on U

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Then consider the global functions φx^1,...,φx^n

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does that make sense?

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So these functions aren't defined to be φ(q) x^1(q) if q is in our chart and 0 if q is outside

sleek thicket
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@sharp yoke

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These are smooth inside the chart because they're a product of smooth functions. And they're identically zero on the complement of the closure of U, so definitely smooth there. Thus they're smooth on an open cover of the manifold, so globally smooth

barren sleet
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@delicate hollow are you still working on how to make intuitive sense of the clopen definition of connected?

delicate hollow
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yea

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i wont use it

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but i would like to know

barren sleet
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do you want my explanation

delicate hollow
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yes

barren sleet
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alright just making sure

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I will ping in a we minutes when I can