#point-set-topology

1 messages · Page 182 of 1

pastel linden
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maybe I should take a proper course on topology before I make broad statements about how stupid this text is

gritty widget
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my coffee is done, let me chug it and then write my thoughts

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latter

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ah if $i : \bR^m \to \bR^n$ is the inclusion i described and $f : \bR^n \to \bR^m$ is a homeomorphism, then $i \circ f : \bR^n \to \bR^n$ is an injective continuous map (being a composition of those), but it's certainly not open

gentle ospreyBOT
gritty widget
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i know spivak wrote calc on manifolds when he was young

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unsure about diffgeo series

pastel linden
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I assumed he learned how to write by the time he wrote calculus

gritty widget
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the calculus book is genuinely well written

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iirc

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no "stokes' theorem is trivial" going on in that one

pastel linden
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alright here we go

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never done anything with spivak and this already feels typical of him thonkzoom

gritty widget
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not open = closed catThink

pastel linden
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shit did I write closed

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let me fix that

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corrected

gritty widget
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ill check over it after i check my complex pset

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slim you're up hmm

gentle ospreyBOT
pastel linden
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oh shit, I think I meant to take the inverse of the homeomorphism

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because then the inverse is injective and continuous and R^m is open, so then i[R^n] should be open

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isn't $(\Psi \circ i^{-1})^{-1} : \mathbb{R}^m \to i[\mathbb{R}^n]$ valid? It's a continuous injection from $\mathbb{R}^m \subseteq \mathbb{R}^m$ into $i[\mathbb{R}^n]$ such that the image isn't open, which is a contradiction

gentle ospreyBOT
pastel linden
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it probably is, I just took the inverse of what I had before because I realized my mistake

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sorry if I've been confusing you, I appreciate the help

gritty widget
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~~bacono i wrote a proof some ways up if you wanna check 😉 ~~

pastel linden
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yeah that works too, I think we had the same thing but yours is simpler in that you applied invariance in R^n instead of R^m

nimble cipher
quiet pilot
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Open in A does not imply open in X

nimble cipher
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So I start from the open cover of X?

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Then from then I just take the open cover of A by intersecting the open cover with A

coarse kestrel
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No you go backward

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Starting with an open cover of A, for each set U in A, there exists open set U’ in X such that U=A intersect U’

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By definition

nimble cipher
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Then I can build the open cover for X as these open sets U' right?

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then I take a countable subcover. So when I intersect them with A, they are a countable subcover of A

coarse kestrel
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Yes

nimble cipher
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Thank you

tight agate
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Does anyone have an intuitive explanation of what a flattening stratification does?

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an equivalent thing in topology land might also help

digital peak
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how does one prove that closure(interior(-)) is idempotent?

sweet wing
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prob can use int(X) subset X subset closure(X) a few times to prove c(i(c(i(x)))) subset c(i(x)) and c(i(x)) subset c(i(c(i(x)))

digital peak
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oh that's clever

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$$iciX \subset ciX$$
$$ciciX \subset cciX = ciX$$
$$ciX \supset iX$$
$$iciX \supset iiX = iX$$
$$ciciX \supset ciX$$

gentle ospreyBOT
sweet wing
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hence conclude there are like 14 sets you can make from using closure and complementChuckle_RF

digital peak
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yeah that's what I was trying to do

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except in coq

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this probably has terrific generalizations

gentle ospreyBOT
feral dragon
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Okay, so finally, 😰 Does this proof make any sense ?

little hemlock
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looks good

gritty widget
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i like the excited "contradiction!" at the end

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I like to keep my math assignments not so dry too

sweet wing
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i prefer presenting refined sols ngl feels neater

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tho it looks super emotionless

zealous glen
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just looking at which spheres can be quipped with a structure of a lie group, so far i have the trivial case of dim=0.. the unit circle case on the complex numbers with length 1, so dimension 1 but having a hard time showing for dim=3

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anybody got any ideas?

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and concluding why only these dimensions can be equipped with a Lie Group structure?

zealous glen
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@gritty widget could you help here? I know you're good at topology 🙂

tight agate
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it isnt a very easy problem to solve

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you can conclude S2 isnt a Lie group if you know the hairy ball theorem

zealous glen
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my main problem is finding the algebraic structure for the lie group of dim=3

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for this

tight agate
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do you have a guess?

zealous glen
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nope, so any hint would be good :x

tight agate
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it's a matrix group

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or another hint would be think quaternions

zealous glen
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number system of quaternions?

tight agate
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yeah the quaternion algebra

zealous glen
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Ah kk

tight agate
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you can think of the quaternions as R4 with a special multiplication

zealous glen
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and proving that these dimensions are the only dimensions is

tight agate
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that's not very easy

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at least the proof ive seen

zealous glen
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any theorems off the top of ur head

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that I can just look up without looking up the proof

tight agate
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do you know about lie algebras?

zealous glen
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ye

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well

tight agate
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and their connection with simply connected lie groups?

zealous glen
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im studying it

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yes

tight agate
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oh then you might be able to do it yourself

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the argument did involve a wee trick tho

zealous glen
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mhm

tight agate
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if you've never seen that sort of thing before

zealous glen
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does this involve Hopf's Theorem?

tight agate
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do you mean hopf invariant one?

zealous glen
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yes i think so

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homotopy invariant

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trying to find a way to prove that the even dimensions of a sphere cannot be a lie group

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but i iz stuck

tight agate
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the idea to do it in general is show that you have a nonzero 3 form on the lie group

zealous glen
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O

tight agate
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for even dim spheres you can do it using hairy ball

zealous glen
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i can do if the lie group is abelian or not

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whats hairy ball

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Oh

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hedgehog theorem

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kk

tight agate
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no nonvanishing vector field on 2n sphere

zealous glen
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yeah we have a different name of it here

tight agate
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yeah that implies that tangent bundle is not parallelizable

zealous glen
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right right

tight agate
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but a lie group is parallelizable

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so that gets rid of the 2n case

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finding the 3-form is where the trick is

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because once you get it then you know the 3rd cohomology is non-trivial

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which implies that it has to be a 3-sphere

zealous glen
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well we can just consider some map a(x,y,z)=<[x,y],z>

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and changes sign swapping any of these values

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so a is a 3-form

tight agate
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noice

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you have the right idea

zealous glen
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and assuming this is nonabelian then we find some stuff that dont commute

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mhm maybe i can do this, but i think im ganna be stuck on the rham cohomolgy

tight agate
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wut why lol

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you just did the hard bit

zealous glen
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oh kek

tight agate
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do you know the de rham cohomology of spheres?

zealous glen
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not very well

tight agate
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no i mean the cohomology groups

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anyway, if you don't know the groups then they are not very hard to compute

zealous glen
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sorry nope

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i was just looking at the left-invariant apart

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and trying to equate it to the right

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of the diff-3-form

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yeah im way too tired for this rn, hehe 6am ... so will look at it in the morning :x

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but thank you!

tight agate
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aight, it's a reasonably fun exercise to compute the cohomology of spheres

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if youve never seen it before

zealous glen
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mhm ok, ill look into it

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im trying to complete all these problem sheets

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and running out of time, but hopefully tomorrow if i finish some QFT stuff

tight agate
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QFT eh

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fancy

zealous glen
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cry

tight agate
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i will stick to reading about hairy balls

zealous glen
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Haha

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we can always swap

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you do my qft assignments

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ill dive into the hairy balls

tight agate
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i know absolutely nothing about qft

zealous glen
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yeah more than me bro

tight agate
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you'll get a 1-sphere as your score

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i hope to read about it sometime tho

zealous glen
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cheeky

tight agate
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they keep mentioning physics stuff in my diff geo class

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but i have no idea on what theyre talking about

zealous glen
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mhm like what?

tight agate
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yang mills stuff

zealous glen
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i mean QFT ⊂ Lie Groups ⊂ Topology ⊂ Diff Geom etc

tight agate
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how is topology included within diff geom

zealous glen
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tangent spaces?

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and all that fancy stuff

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oh

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mbe otherway round

tight agate
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geometry is sorta topology + extra structure right

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yeah it should be the other way

zealous glen
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yeah im tired catwiggle

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af

tight agate
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do you know any yang mills stuff

zealous glen
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is that shiz on feynman diagrams

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because i think thats in the next 2 weeks

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Lecture 08: Feynman Diagrams for the Yang-Mills field

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yeah i have that in 2 weeks

tight agate
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i dont think so

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theyre probably related

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but that's not what they were talking about in my class

zealous glen
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semisimple lie algebra and an abelian lie algebra with compactess

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mhm apparently is YM theory

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which its based on SU(N)

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mhm it seems quite interesting actually

tight agate
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I have heard the word SU(N) guage theory thrown around, yes

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but in the lecture they were looking at this functional

zealous glen
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describing the behaviour of elementary patricles using non-abelian Lie groups and is the core unification of the EM force and Weak forces

tight agate
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given by taking the inner product of the curvature with itself

zealous glen
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mhm

tight agate
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and integrate

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(with the volume form)

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and then they started looking at critical points of that

zealous glen
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idk why

tight agate
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and finally concluded that self adjoint connections are solutions to whatever

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yeah idk

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the whole thing was similar to Chern-Simons theory stuff

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where the critical points of the functional turn out to be flat connections

zealous glen
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mhm ok

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interesting

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i havent read about chern-simons theory

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or mbe i have an just cant remember

tight agate
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say you have a complex manifold

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and a trivial bundle E over it

zealous glen
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yeah

tight agate
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then d (exterior derivative) is a connection

zealous glen
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if i remember does this have some intergral with wedge product?

tight agate
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look at the one paramter family d + tA

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where A is a End(E) valued 1 -form

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yeah and then the transgression is the chern simons form

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A wedge dA + 2/3 A wedge A wedge A

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I assume that's what youre talking about

zealous glen
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yesyes

tight agate
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yeah and you integrate that

zealous glen
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oooo

tight agate
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and then look at e^-k of the thing you get

zealous glen
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so you take some path intergral over all SU(2) connections on the manifold

tight agate
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yup yup

zealous glen
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kewl

tight agate
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and the critical points of the functional are flat connections

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but yeah in general it's a path integral over End(E) valued 1 forms

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the space of connections is an affine space over that

zealous glen
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does this have properties of ricci flatness

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or am i going in the wrong direction

tight agate
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idk

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by flat I just mean delta^2 = 0

zealous glen
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the curvature vanishing right

tight agate
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yup

zealous glen
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Moduli space of flat connections on a riemann surface is naturally a complex manifold

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so maybe it does exhibit some properties of ricci flatness

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?

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who knows

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do a phd paper about it

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yoour welcome

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OOHH

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maybe this comes into play with calabi-yau manifolds

tight agate
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holy crap it's the jacobian

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never thought of that before

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flat U(1) connections

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on a riemann surface

zealous glen
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yeye

tight agate
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if the mathoverflow post im reading is correct

zealous glen
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link me broskarian

tight agate
zealous glen
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mhmm

tight agate
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you have supplied me with the hype I need to get through next week

zealous glen
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ha! no problem

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now i go for a smoke and I shleep or mbe some maff

tight agate
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I need to write a history essay lmao fml

zealous glen
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something cool to look at: The complex tangent bundle of the Riemann sphere

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then corellate this with chern class

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then calabi-yau manifolds

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some cool stuff all coming in to play

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wait wut history?

tight agate
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im doing a history class

zealous glen
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how u do history and maff

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or its the history of math

tight agate
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we need to do a bunch of 'general education' classes

zealous glen
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:fivehead:

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are u in uni?

tight agate
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ye

zealous glen
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"This is America"

tight agate
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quite a lot of general ed classes actually

zealous glen
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ah im from the UK we just study what we want

tight agate
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sounds fun lol

zealous glen
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mhm yesyes

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oki i need a smoke but gl with the essay 😉

tight agate
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cya

zealous glen
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ciao bella

feral dragon
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i like the excited "contradiction!" at the end
@gritty widget Well if you're someone like a logician that's the only thing in a proof to excite you

burnt spruce
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Which scheme should be called 'The Ponzi Scheme'?

meager python
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The scheme without closed points

hard wind
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To show a space is connected, does it suffice to find a contradiction from supposing there is a pair of disjoint, non-empty, open subsets that cover the space, or must I suppose more generally there exist a collection of disjoint, non-empty, open subsets that cover the space?

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I would think it does, since if I had A, B, C disjoint open subsets of a space X that covered X, B union C is itself open, so A and B U C do the trick.

tight agate
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yup a pair works

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a space is disconnected iff it is the union of two disjoint open sets

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nonempty

feral dragon
sweet wing
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art major chad

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now help me draw H^3/<z->z+1,z->1/z>

feral dragon
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haha I can be pretty decent at pencil drawing sometimes

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now help me draw H^3/<z->z+1,z->1/z>
@sweet wing now help me understand what that creature is, firstpandaThink

sweet wing
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it may just be a cusped torushank

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with a funny metric

night parrot
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does anyone have any good resources for learning more about discrete differential geometry? i have a pdf from keenan crane's course that looks pretty good, but wondering if there are other books out there

quiet pilot
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What's the main use of topology in algebraic geometry? I know we introduce the Zariski topology, but do we use any theorems from topology that helps us study it?

tough imp
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It is t very heavy

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If you know basic point-set, that’s most of what you end up using most of the time. Other stuff about codimension and stuff are sort of topological I guess but you wouldn’t talk about it in a general topology course

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From what I gather AG doesn’t really need all that much of topology other than the notion of open covers since eventually you’ll abstract away from even topological spaces into Grothendieck topologies and stuff which mainly only retains the notion of open covers and the property of continuous maps we care about is that they pullback an open cover to an open cover

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This isn’t to say topology plays no role, my professor published a paper recently which shows for some class of varieties the topological space actually determines the variety up to isomorphism which is pretty interesting

quiet pilot
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Ah I see, I know some basic point-set and algebraic topology

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The course I'm taking is called "Intro to algebraic geometry" and seems to only cover classical algebraic geometry so I don't think we'll cover schemes

tough imp
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Oh okay, yeah you should be fine

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You’ll have to learn new stuff since there’s topological properties you won’t cover in a normal point set class since they’re super weird

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Things like an irreducible topological space, Noetherian topological space, etc

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But that’s really easy to pick up

quiet pilot
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Ah I heard about the first one in my commutative algebra course at least

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Thanks for the answer, and thanks for the help with commutative algebra btw. Wrote the exam yesterday

tough imp
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Uhhh, I don’t actually remember exactly what it was I helped you with but I’m glad I could help 😂😂

quiet pilot
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Classification of prime ideals in Z[X], and a few other things 🙂

tough imp
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Ahh, no worries haha

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I worked through a classification of maximal ideals in Z[x] with someone once but I realize I made a slight error with it 😂

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So if that was with you my bad OOF

quiet pilot
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Yeah that was probably with me. The explanation made me look up a lot of things about ideals and quotients though and we covered it more extensively than the book did on a later lecture anyway

tough imp
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Ah, okay. The part where I failed was showing that the maximal ideal has to have a prime number p. I think I said to intersect with Z, but you have to rule out the case that’s empty and in order to do that you have to extend the ideal to Q[x] I believe.

quiet pilot
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Yeah, we did that and then used Gauss' lemma to show the ideal was principal and generated by the primitive polynomial of the polynomial with least degree in that case.

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A nice proof now that I understand it haha

tough imp
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Ah nice. I don’t remember if I actually did do that lmao

delicate hollow
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What is definition of a separation? I can't find rigorous definition online and making my own doesnt seem to work well.
So far I have, two sets A,B in M are separated iff
1.A U B = M
2. A intersect B = {}
3. A,B Nonempty.

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But I can think of examples that counter this.

tough imp
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I think this is commonly referred to as a disconnection, and we require A and B open

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This doesn’t always exist, and if one doesn’t exist then we call that space connected

delicate hollow
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oh A and B have to be open and I think the fixes the problem

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before I was having a problem where I was giving two sets that were touching

ivory dragon
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yep, if you require A, B open this is precisely the usual definition of a disconnection

delicate hollow
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🙂

ivory dragon
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we say M is disconnected if there exist such A, B open [with AUB = M, A and B nonempty and disjoint]

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and otherwise M is connected

delicate hollow
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proving connected seems hard

ivory dragon
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generally speaking, yes

tough imp
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Generally you show it can’t be disconnected

ivory dragon
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fortunately there is a useful theorem:

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the image of a continuous function on a connected set is connected.

delicate hollow
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yes

tough imp
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I think like all my connectedness arguments are by contradiction.

delicate hollow
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I was going to ask that question

tough imp
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It’s just much easier to attack that way IMO

ivory dragon
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yeah, certainly if you want to do it "directly" from the definition the usual way is

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"suppose we have a disconnection {U, V} for this set S. then consider this other set T that we know is connected. then we can construct new sets out of {U, V} by... and this is a disconnection of T because... but that is a contradiction."

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in some cases this can be done very "directly"

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for example, proving the closure of a connected set is connected

delicate hollow
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  1. Say you want to prove there is no homeomorphism between two sets A,B then is it enough to show that A-S is connected and B-S is disconnected, for some subset S in A and B .
  2. Is homeomorphic an equivalence relation?
    Two questions ive been thinking about
ivory dragon
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homeomorphisms preserve connected components, yes

tough imp
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Uh, you have to be careful right?

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If you show this over all such S then you’re good

ivory dragon
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oh yeah good point @tough imp

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homeomorphisms preserve number of connected components

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so you'd have to show it for all such S

tough imp
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You can like, assume the S’s in each set have the sane cardinality

ivory dragon
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(i.e. that A has one connected component, while B has >1)

tough imp
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But besides that it’s pretty general

cursive glade
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You can extract the number of connected components from betti numbers of the space

tough imp
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I’m trying to understand the characterization of morphisms into P^n from a scheme X as being equivalent to an invertible sheaf L on X and a set of n + 1 sections which generate L

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I’m following Hartshorne, and on page 150 he says given a map phi: X -> P^n we get these sections s_i = phi^*(x_i) which generate phi^*(O(1))

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I don’t understand what phi^*(x_i) is

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For a second I thought it could be anything in the fiber of x_i... but that doesn’t even make sense!

meager python
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Why doesnt that make sense?

tough imp
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Umm, I think the ring map is going the other way actually

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So these are the images of the x_i under the ring map on global sections?

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I realized that given an invertible sheaf and sections which generate it you have to make a map into P^n and given the construction in Hartshorne this at least seems to be what’s going on?

meager python
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Well if you have X into P^n then you have a map of sheaves

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And x_i are elements of that sheaf

tough imp
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Right, but this actually goes the other way

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I thought it would be thinfs in the fiber

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Aka stuff mapping to x_i

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But the map goes the other direction so actually it should be the image of the x_i I think

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I think this actually makes sense. Geometrically if we think of these as homogenous coordinates we want to define stuff by just saying “this is where this coordinate goes” which is what this does. But if you look at the actually construction of the map, since a homogenous coordinate isn’t well-defined, only ratios of them we define stuff by sending x_i/x_j to s_i/s_j

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Which is really just the proper way to say we send x_i to s_i

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Or something

nimble cipher
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Is ${(p,q):p,q\in\mathbb{Q}}\cup{(p,q)\setminus K:p,q\in\mathbb{Q}}$ where $K={\frac{1}{n}:n\in\mathbb{N}}$, a countable basis for $\mathbb{R}_K$?

gentle ospreyBOT
digital peak
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So consider $[0,1]^{[0,1]}$ in product topology, what's a subset that's sequentially compact but not compact?

gentle ospreyBOT
digital peak
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I could probably construct something isomorphic to the long ray, but is there possibly a lower tech example?

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actually now I doubt the ability to construct a long ray here...

digital peak
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maybe if I took one of the connected components

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nope not seq compact

digital peak
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Let $\phi : [0, 1] \to \omega_1$ be a bijection, then
$$A := \left{ f \in [0, 1]^{[0,1]} \middle|\exists \alpha \in \omega_1 : \begin{array}{l}\forall \beta > \alpha, f(\phi^{-1}(\beta)) = 1 \ \forall \beta < \alpha, f(\phi^{-1}(\beta)) = 0\end{array} \right}$$
is homeomorphic to the long ray

gentle ospreyBOT
digital peak
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oops

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swap 0 and 1

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but it doesn't matter I guess

digital peak
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would appreciate a simpler example still

hard wind
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"Find a subspace of R^2 that is path connected but not locally path-connected at any of its points."
Is this even possible? I've been racking my brain for hours trying to think of how to modify the topologist's sine curve or something. Any hints?

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Please ping me.

gritty widget
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Do you mean the opposite? Locally path connected but not path connected? (I think path connected implies locally path connecredl

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In that case, maybe like 3 topologists sine curves connected end to end

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So that from each point there exists another point that you have to pass the fucky part of the topologists sine curve to get to

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@espio

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@hard wind

coarse kestrel
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no, path connected does not imply locally path connected

hard wind
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Nope, that was the exact wording.

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Path connected but not locally path-connected at any of its points.

coarse kestrel
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and also the problem wouldn't have made sense if you switch it since path connected at a point doesn't make sense

hard wind
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Attaching those three topologist's sine curves wouldn't be path connected

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Ye

gritty widget
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Path connected means between any two points there is a path, and locally path connected at a point p means there is a neighborhood around p that is path connected, right?

hard wind
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Yes

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An open neighborhood specifically

gritty widget
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Then doesn't path connected imply locally path connected?

hard wind
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Errr, no

coarse kestrel
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no no no

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that's not the definition

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locally path connected means for every point p and open set U containing p, there is a smaller open set V that is path connected

hard wind
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Sorry, yeah thats the real definition

gritty widget
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But your definition implies mine, and my definition implies yours

hard wind
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Take the topologist's sine curve and connect the two ends (0,0) and (1,0) with a curve

coarse kestrel
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your definition doesn't imply mine

hard wind
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Actually not quite

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I meant not quite at mathbath

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Thats an example of path connected but not locally path connected yeah

coarse kestrel
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yeah at every point

hard wind
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But i need every point

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Which honestly, makes no sense to me

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I dont see how thats possible

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At least not as a subspace of R^2

coarse kestrel
#

i was thinking of maybe take $\br{\bigcup_{x\in\bQ}\brc{x}\times\bR}\cup(\bR\times\brc{0})$

gentle ospreyBOT
coarse kestrel
#

But the Rx{0} part doesn't work

hard wind
#

Interesting idea, I had thought about comb spaces earlier

#

Yeah... it's hard

#

I couldnt seem to find a comb space that works

coarse kestrel
#

Oh I found the answer on stackexchange

gritty widget
#

Hm, I guess I fail at topology

hard wind
#

Damn, impressive whoever

coarse kestrel
#

welp

hard wind
#

I could not find it on stackexchange

coarse kestrel
#

do you want it?

hard wind
#

Can i have a hint first

coarse kestrel
#

the answer kind of used my idea

#

except it's

#

connecting (0,0) to (1,p) for every rational p in [0,1]

#

and you try to do something else to make the space not locally path connected at (0,0)

hard wind
#

hm

#

oh ok i get it

#

now i must mess with (0,0) yeah

digital peak
#

hmm

#

subspace of [0,1]^[0,1] in product topology whose sequential closure is not sequential closed

nimble jolt
#

Pasting here so not lost in the clutter of chill:

Consider the indicator functions of an algebra of sets (e.g. the opens). If a sequence of these indicators converges pointwise, then both the liminf and limsup converge to this same limit, which is the indicator of the set A that is either the union of cofinite intersections or intersection of cofinite unions we discussed earlier (these must coincide in fact). This already shows that if you start with the opens, a convergent sequence can only give you something at most two steps up the Borel hierarchy.

On the other hand, as each step of the Borel hierarchy forms an algebra, you can always write an arbitrary union or intersection of sets in one step as a monotonic union or intersection. This shows that a convergent sequence can get you anything in the next step up the Borel hierarchy.

Paragraph 2 shows you get get arbitary finite step Borel sets by repeatedly taking sequential closures, Paragraph 1 shows you can't get all of these with only one sequential closure operation. Hence the sequential closure is not sequentially closed.

meager python
#

Why is there no channel for algebraic geometry alone? sadcat

honest narwhal
#

Algebraic geometry \subset algebra \cup topology and geometry

ancient zenith
#

if you are however looking for algebraic geometry discussion, Ravi Vakil runs a math discord (I kid you not) called the algebraic geometry syndicate

#

that's the only reason I have the (CA) in my name; they wanted us to indicate our locations

honest narwhal
#

@ancient zenith one thing that's worth noting is that discord has a way to have a nickname on a server separate from your global username

#

So if you'd rather not use your real name and location here you can change your overall user to something more anonymous and then set a nickname on AGS that complies with what they want

ancient zenith
#

oh my god

#

you're telling me I've been unnecessarily doxxing myself this whole time

#

rest in rip me

gritty widget
#

but u need to solve a challenge problem to get nickname changing privilege, better get solving quick!

sweet wing
#

ripppp

red garden
#

Algebraic geometry \subset algebra \cup topology and geometry
@honest narwhal algebra is a subset of topology and geometry?

honest narwhal
#

Huh

rugged swan
#

Algebraic geometry = Algebra tensor Geometry

meager python
#

Dynamical systems why? When theres analysis

#

Category theory? You mean foundations? Etc

gritty widget
#

I claimed that the set $A$ defined by
$$A={ (x,y,z)\in\mathbb{R}^3 \ \lvert \ x+y+z\in\mathbb{Q}}$$
has interior point as $\varnothing$ and closure as $\mathbb{R}^3$? But how to show that? I have shown that set $A$ is a neither open nor closed set in $\mathbb{R}^3$.

gentle ospreyBOT
tight agate
#

Proving the closure is R3 should be easy, as A contains Q^3 (and Q is dense in R)

#

To show that the interior is empty, fix (x,y,z) in A, for any epsilon ball in A, pick an irrrational delta such that (x + delta, y, z) is contained in the epsilon ball.

gritty widget
#

So we pick $\delta=\dfrac{\varepsilon}{2}$ for irrational $\varepsilon$ and $\delta=\dfrac{\varepsilon}{\sqrt{2}}$ for rational $\varepsilon$ to show its interior?

gentle ospreyBOT
tight agate
#

yeah those work

gritty widget
#

Nice

#

Proving the closure is R3 should be easy, as A contains Q^3 (and Q is dense in R)
@tight agate But I still don't get the idea since set $A\subseteq \mathbb{Q}$.

tight agate
#

no, A contains (sqrt(2), -sqrt(2), 0), which is not in Q^3

#

Q^3 is contained in A

#

So Q^3 closure is contained in A closure

#

And what is Q^3 closure?

gritty widget
#

R^3

tight agate
#

so?

gritty widget
#

We can conclude that cl A=R^3!

#

Thanks

#

I get it now

tight agate
#

yeah A is a lot bigger than Q^3

#

Q^3 is countable

#

A is not

gritty widget
#

I understand now, so formally written, Q^3 ⊆ A ⊆ R^3 => R^3=cl Q^3 ⊆ cl A ⊆ cl R^3=R^3 yields the result

tight agate
#

yup

little robin
#

Hey I'm looking for an academic journal that contains a proof of the Hyperplane Separation Theorem. Does anyone know where a good place to look would be?

tough imp
#

Why do you need a journal?

#

I think you can find proofs just out on the web

little robin
#

Dumb reasons. XD
Basically I gotta get 12 citable items for a survey research paper

#

Web proofs =/= citable items

tough imp
#

gross

little robin
#

ikr

tough imp
#

Good luck lol, don't think many people consider this theorem "journal-worthy"

#

maybe try some computational geometry shit or something idk, some applied geometry journal

little robin
#

Yeah, but I can't get ahold of books in time because I kinda blew this off. XD

#

Yeah, it's my own fault and I'll suffer for it. Thanks anyway

#

Thank you so much

#

I'll look into it.

summer jolt
#

Hi, I am trying to prove that the real projective plane is NOT homeomorphic to a circle. However, I am a bit lost. I'd like to argue in terms of connected components but not sure.

gritty widget
#

aren't they both connected?

#

how overkill do you want your solution to be

#

the universal cover of RP^2 is S^2 and the universal cover of S^1 is R opencry

#

another maybe overkill solution is that RP^2 has fundamental group Z / 2Z and S^1 has fundamental group Z

#

but connectedness is not the topological invariant that fails here

coarse kestrel
#

idk i wouldn't say that's an overkill solution

gritty widget
#

im blanking on a non-AT topological invariant that breaks here

#

maybe manifolds are too nice

#

true

#

@summer jolt what level is this?

#

line goes that way or line goes this way catThink

summer jolt
#

@summer jolt what level is this?
@gritty widget undergrad

#

The circle is oriented
@gritty widget we haven't covered orientation yet

#

but connectedness is not the topological invariant that fails here
@gritty widget I was thinking that if I remove two points on the circle then I form two connected components and RP2 you don't? But I don't see the picture

gritty widget
#

everything i mentioned is undergrad level to me, i meant if this is a gen topology class or an AT class lol sounds right

#

i like that argument

#

(if you want a picture)

summer jolt
#

i like that argument
@gritty widget the only thing I am unsure is what would be the number of connected components in RP2 if I remove two points.
Thanks for the pic, but I really don't get why it represents RP2. I am used to thinking that RP2 like a half sphere with antipodal points but even that is hard to grasp.

gritty widget
#

i strongly believe it will again be one connected component

#

im writing something down to convince myself lol

#

think of it like this maybe: if you remove two points from RP^2, how many points do you remove from the hemisphere with antipodal points identified? could you possibly disconnect it?

#

that argument might be a little sketchy

summer jolt
#

Yeah you're right it would still be connected.

gritty widget
#

and then RP^2 minus those points is the image under the quotient map of your hemisphere minus some points, which is still a connected domain

#

i like what slimvesus is saying more than what im saying lol

#

listen to them

summer jolt
#

RP2 - point = mobius band
@gritty widget oh wow! I didn't know this.

gritty widget
#

like i said, just nuke it with universal coverings

#

or throw a grenade at it with the fundamental group

#

i don't actually know a lot about the projective plane

#

you're the expert here

summer jolt
#

Isn't that the circle again?

gritty widget
#

so many ways to do this 😌

summer jolt
#

Hmm so you saying that if I remove a point from RP2 you get a circle?

#

Ah!

#

Ok I am getting to understand the reasoning now!

#

Yes, I can imagine. That makes sense.

gritty widget
#

Here I have a question. I am asking to write down a single subset of $\mathbb{R}^2$ that satisfies all conditions: \
(i) $A$ is connected and not pathwise-connected.\
(ii) $A$ contains the set $K={(x,y)\in\mathbb{R}^2 \ \lvert \ x\in[0,1], y=0 }$ as a subset.\
As the example that I know, the set $P=Q\cup R$, with $Q={(x,y)\in\mathbb{R}^2 \ \lvert \ y\in[-1,1], x=0 }$ and $R=\left{(x,y)\in\mathbb{R}^2 \ \lvert \ x\in[0,1], y=\sin\dfrac{1}{x} \right}$ is the most famous example to show that connected does not imply pathwise-connected in higher dimension. Thus I modified a bit for my answer, that is, take set $A=K\cup G$, where set $K$ is given on the question, and\
$G=\left{(x,y)\in\mathbb{R}^2 \ \lvert \ y\in[0,1], x=\dfrac{1}{2}\sin\dfrac{1}{y}+\dfrac{1}{2} \right}$\
Am I in the right track?

gentle ospreyBOT
sweet wing
#

i) you mean not path connected?

#

oh do people use pairwise connected for path connected or is it smt else

gritty widget
#

i) you mean not path connected?
@sweet wing Oops I meant pathwise-connected. It seems I have a typo.

sweet wing
#

icic

#

but yh the idea is that

#

just put the sine curve in the correct location

#

such that Q aligns with K

gritty widget
#

Yeap I wonder if I get the set $G$ wrong because I have to adjust the graph

gentle ospreyBOT
gritty widget
#

If there are other example that satisfies the condition, it would be better

nimble cipher
#

Hi. Why is the subspace topology here discrete? Note X is a metrizable space.

stable lance
#

'A has no limit points' implies that every subset of A is closed in A

nimble cipher
#

Ohh that makes sense, which means that every subset is also open

summer jolt
#

Question: what do you get gluing the opposite sides of 2n-polygon? Square gives the torus, I think the hexagon also gives the torus, the octagon gives the double torus (I looked this up). However, I'm failing to identify the pattern (is there any?)

gritty widget
#

there is a pattern

summer jolt
#

Interesting!

#

So you just glued tori together

gritty widget
#

maybe you can visualize the octagon case like this:

use a line to split the octagon into two halves. if we collapse this middle line to a point while doing the gluing, we'll get two squares joined at a point. each square can then have its sides glued together like you would to get a torus (as pictured). then you have the double torus

#

(i really hope i didn't identify the sides wrong lmao)

#

it's been a while since i did this so please correct me if my square-to-torus gluing is wrong

sharp yoke
#

having trouble proving the map is injective

#

its easy to visualize but im having trouble writing it out formally

gritty widget
#

I think the important thing here is that the interior of A is nonempty

#

Otherwise eg a line segment in R2 through the origin does not give rise to an injective p

#

iirc there is some tricky linear algebra argument about compact convex sets with nonempty interior satisfying some nice properties that are relevant here, but there's a good chance I'm misremembering/talking nonsense

nimble jolt
#

@sharp yoke

If x is a point of the boundary of A with maximal distance from 0 along a given ray L from 0, I claim it is the unique boundary point of A on this ray. To see this, consider apply the convexity condition to an epsilon ball about 0 and x. This gives you a narrow cone of points contained in A, and all points of the ray L other than x are interior to this cone and hence not boundary points of A.

gritty widget
#

but why is there an epsilon ball around x?

#

i think proving this is tricky

#

ah, i am a dumbass

#

i guess i am probably mixing this up with something else

nimble jolt
#

epsilon ball around 0, not x @gritty widget

#

picture x as the point (0,1) in the plane for instance, and you are putting a tiny ball about (0,0) and drawing line segments between every point in this ball and (0,1), forming essentially a cone.

gritty widget
#

yeah i see it, i was being a dumbass

sharp yoke
#

thank you

summer jolt
#

maybe you can visualize the octagon case like this:

use a line to split the octagon into two halves. if we collapse this middle line to a point while doing the gluing, we'll get two squares joined at a point. each square can then have its sides glued together like you would to get a torus (as pictured). then you have the double torus
@gritty widget yeah that's exactly how I thought about it!

feral dragon
#

@oak skiff You're mapping to a set with the same topology (an open set) or something else ?

#

Why don't you send that problem so that it'll be easier to explain with an example.

feral dragon
#

@oak skiff mostly it's obvious, but are you aware of "The Rules for constructing continuous functions" ?

#

ahh,I guess you construct continuous functions by proving that they're continuous over specific topologies

#

So you know these and have you practiced examples on this ? @oak skiff

#

btw what book is your course referring to ?

#

ahh Munkres shouldn't create any confusions tbh. But you should be looking at Chapter 2 Section 18 i believe.

#

That's fine, good luck with that though. Hope you get the confusions cleared up

quiet pilot
#

Do you even need that X1 and X2 are algebraic here?

#

I'm not sure if I'm missing anything because the equality seems to follow straight from the definition

tough imp
#

I don’t think so

#

In response to do they need to be Algebraic

quiet pilot
#

Ok that's good to hear

gritty widget
#

Hi ! Just to be sure : A manifold is simply connected if it is arcwise connected and has the trivial fundamental group (i.e. for all x in M, all loop from x to x are homotopic to the identity) ? (I hope this is the place to ask, I'm new here, just tell me if it is not 🙂 )

#

that sounds like the right definition of simple connectedness yes

#

you only need that the fundamental group at some point is trivial, since you have path connectedness

#

you only need that the fundamental group at some point is trivial, since you have path connectedness
@gritty widget I didn't get that, I think I am lacking something

elder yew
#

If it's path connected, then it suffices to check that the fundamental group is trivial at a single point because you can always use that change of base theorem in Hatcher

#

Showing that the fundamental group at a base-point contained in the same path connected set are isomorphic

#

@gritty widget does that make sense?

gritty widget
#

Yes I get the idea and the intuition

#

but I did not see that theorem

#

i'll check it

elder yew
#

It's chapter 1

#

I forget which theorem it is exactly, but the proof isn't too difficult

#

Just compose paths cleverly

gritty widget
#

ok but basicly it says that if there exist a continuous path between two path and if the fundamental group at one of them is trivial, then it is also trivial for the second one ?

#

if you have a path from a to b, then the fundamental groups are isomorphic by the following map:
-take a loop at b
-map to a loop at a by starting at a, following the path to b
-do your loop at b
-go back to a using the path in reverse

#

in alg lecture rn, can't go super in depth

#

it should be in literally any topology book

#

(yeah yeah, homotopy class of loops, i get it)

tough imp
#

Just use the path a to b (and b to a) to turn a loop at a into a loop at b

#

And a loop at b to a loop at a

#

Conclude these processes are inverses

#

There’s only one way to do this that you should be able to think of

#

I guess verifying this plays nice with the operation or whatever becomes more of a pain but once you have the map you can just verify details

gritty widget
#

Ok so there is a way to map a loop at a with a loop at b but i don't see how this help us to conclude that the fundamental groups are isomorphic

#

And why the fact that they are isomorphic implies that if one is fundamental, the other one has to be

#

one is fundamental GWchadMEGATHINK

#

if one fundamental group is trivial*

#

sorry i'm a little tired 😅

#

why if one is trivial the other is
well if two groups are isomorphic and one has only one element, so does the other

#

oh yes make sense

#

chmonkey described why the map gives you an isomorphism of pi_1(X, a) and pi_1(X, b)

#

you can find the details in e.g. munkres or hatcher or on wikipedia probably (or just do it lol)

#

ok, thanks a lot for your patience 🙂

tough imp
#

If $\mathscr{E}$ is a locally free $\mathcal{O}_X$ module of finite rank, I want to show that
$\mathscr{H}\text{om},(\mathscr{E},\mathcal{F})\cong \check{\mathscr{E}}\otimes \mathcal{F}$ for any $\mathcal{O}_X$ module $\mathcal{F}$

gentle ospreyBOT
tough imp
#

On an open set $U$ for which $\mathscr{E}$ is isomorphic to a free $\mathcal{O}_X$ module, I was able to produce an explicit isomorphism, and was (with trouble) able to show that these agreed on intersections to give a global isomorphism

gentle ospreyBOT
tough imp
#

Is there a way to define such a map globally however, and then to simply check that it's an isomorphism locally? If so I'd much rather do that, but it's really not clear how you can get a map either direction

tight agate
#

We can define the following map from the presheaf that you get when you take the tensor product over each open set

tough imp
#

I figured it out ;w;

tight agate
#

oh okay nvm

tough imp
#

I literally couldn't think of a map Hom_A(M,N) to Hom(M,A) (x) N

#

for like an hour and a half

#

Err, I guess it's the other way around

tight agate
#

yeah the map I have goes the other way

tough imp
#

You send like

#

f(m) (x) n to f(m)n right?

tight agate
#

yup

tough imp
#

I had this like exact idea, but thought for some reason I had to pick an arbitrary n to use

#

forgetting you get given an n to use

#

😔

#

and sat around for an hour and a half mulling about how tf I can do this

tight agate
#

but this is just a map from the presheaf right

tough imp
#

Right, but you can show it's a local iso

tight agate
#

you need to sheafify after that

tough imp
#

so it doesn't matter

tight agate
#

yup

tough imp
#

You don't even need to localize

tight agate
#

or just on stalks

tough imp
#

err stalks

#

the issue is

#

to know that sheaf hom plays nice with stalks you need like

#

the first thing to finitely presented or something

#

at least that's what I saw on Stacks??

tight agate
#

hmm

tough imp
#

And I don't want to deal with that shit right now haha

#

The idea is sheaf-hom_{O_x}(F,G)_x is just Hom_{O_X,x}(F_x,G_x) right?

#

But I think this fails in general

tight agate
#

I think youre fine in this case as they're locally free

tough imp
#

Yeah, but basically

#

I don't want to prove that equality

#

XD

#

I mean I guess I should, but also it's equally easy to just go to a trivializing cover

#

to get the map we defined is an iso

#

but to prove the equality of the stalks above is more work and I'll just... save that for later

brittle widget
#

Omg my geometry lecturer just wrote f holomorphic from compact Riemann surface X to CP^1, d for degree of f, F' for # faces of a triangulation T of X, F for # faces on f[T], and then reasoned F' = dF XD

elder yew
#

Sounds like an analyst

#

That's the kind of Prof. I can get along with

sleek thicket
#

ughhhh my brain is too small for riemannian geometry

#

hello ttera

gritty widget
#

hello shamrock

#

i was typing a witty response to what epicguy posted

#

but then i realized i had read their post wrong

sleek thicket
#

tfw

#

Do you want to help me think about riemannian geometry?

#

My brain is fried

gritty widget
#

it's 4 am for me so the chances i'll be able to contribute anything are infinitesimal

#

but ok

sleek thicket
#

kk

#

Let G be a lie group

#

With a bi invariant metric g

#

And lie algebra \g

gritty widget
sleek thicket
#

I'm supposed to show <ad(X) Y, Z> = - <Y, ad(X) Z> for all X, Y, Z in \g

gritty widget
#

kinda looks like the "connection is compatible with the metric" condition but equal to zero with some terms shuffled

sleek thicket
#

I tried to do this as follows:
Let γ be the one parameter subgroup with γ'(0) = X. Define vector fields V, W along γ by V(t) = d(L_γ(t))_e(Ad(γ(t)) Y) and W(t) = d(L_γ(t))_e(Ad(γ(t)) Z). Then d/dt <V(t), W(t)> = <D_t V, W> + <V, D_t W> by compatibility with the metric

#

By left invariance of the metric <V(t), W(t)> = <Ad(γ(t)) Y, Ad(γ(t)) Z>, and by bi-invariance this is constant

#

(bi invariance is equivalent to the inner product on \g being invariant under the adjoint representation of G)

#

okay so the derivative of a constant is 0

#

So it suffices to show (D_t V)(0) = ad(X) Y

#

(and by symmetry the same thing but for W)

#

This feels plausible to me because ad(X) = d(Ad_e)(X) = (Ad ° γ)'(0)

#

But I haven't gotten any further than that

#

wtf is D_t

#

I hate it

gritty widget
#

V(t) = d(L_γ(t))_e(Ad(γ(t)) Y)
should it be Ad(γ'(t))Y inside? or am i missing something about lie groups

sleek thicket
#

Nope

#

Big Ad is different than little ad

gritty widget
#

in what way?

sleek thicket
#

Ad : G -> GL(\g)
ad : \g -> \gl(\g)

#

Ad(x) is the differential of the conjugation by x map : G -> G at the identity

#

ad(X)(Y) = [X, Y] but also ad is the differential of Ad at the identity

gritty widget
#

i see

#

give me a few minutes to digest everything you wrote

sleek thicket
#

okay well one more thing: if we define $A_x = d(L_x)e(Ad(x) Y)$ then $A$ extends $V$ so $(D_t V)(0) = \nabla{\gamma'(0)} A = \nabla_X A$

gentle ospreyBOT
gritty widget
#

hmmm

#

just write it in coordinates opencry

sleek thicket
#

fucc u

gritty widget
#

lemme try it for a little bit and see if i come up with something

sleek thicket
#

Sure, I'm mostly just trying to sound off the problem again and see if I notice anything new

gritty widget
#

the only technique i know of to make calculating covariant derivatives easier is writing things in parallel vector fields but i don't really see how that'd make this easier lol

#

i'm still thinking on it tho

sleek thicket
#

I think I maybe figured it out but I'm confused by something

#

So like

#

If you instead define V(t) = d(L_γ(t))_e(Ad(γ(t)^-1) Y) then I think V(t) = d(R_γ(t))_e(Y)

#

Because in G if you conjugate by γ(t)^-1 and then multiply by γ(t) on the left, that's the same as multiplying by γ(t) on the right

#

Actually I think I see it now

#

ty for the help

gritty widget
#

does working with this new definition of V(t) and W(t) solve it?

#

also it would be V(t) = d(R_γ(t))_e(Y), can confirm

#

there's a proof of this in do carmo GWchadMEGATHINK

sleek thicket
#

I think so

#

I mean, I actually changed it to d(R_gamma(t))_e(Ad(gamma(t)) Y)

#

but things work out right I think

#

So with this change V has extension the left invariant vector field corresponding to Y

#

hmm no this does not immediately solve my problems

#

but it is insight

#

and I should go to sleep

gritty widget
#

i guess i can give an uneducated hint

sleek thicket
#

Sure

#

That's what I asked for :P

gritty widget
#

it's in the section before covariant derivatives in do carmo so you shouldn't need those

sleek thicket
#

What is?

gritty widget
#

the proof of the thing you wanna show

sleek thicket
#

oh uh

gritty widget
#

(the first thing)

sleek thicket
#

I'm confused

#

The thing about ad(X) being skew adjoint?

gritty widget
#

ya

sleek thicket
#

Maybe I'm fucking this up then

#

It's in the section on the Levi-Civita connection in Lee

#

But there's more to the problem

gritty widget
#

lemme take a peek at lee

sleek thicket
#

So maybe this first bit doesn't use it

#

hmmm

gritty widget
#

i might look at the problem more tomorrow

sleek thicket
gritty widget
#

i don't have a lot of homework this week so i have some spare time to mess around with

#

oh nice copy

sleek thicket
#

It's on my homework so I'm going to think about it more for sure lol

#

Yee

#

I have the trio

gritty widget
#

i am jealous

#

both of my classes concerning smooth manifolds so far have completely ignored lie groups opencry

sleek thicket
#

Oof

gritty widget
#

and my rg prof is speedrunning do carmo, any%

sleek thicket
#

My course last year didn't do a lot with them

#

like

#

The important stuff if at the end of ISM

#

But do to covid we didn't get there

#

and so they did it in prelim prep seminars over the summer

#

But I was doing other stuff

gritty widget
#

ism chapter 19 catThink

sleek thicket
#

I read it on my own but it's not the same

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Oh 19?

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We did that

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We did cover the closed subgroup theorem

#

foliations are cool

gritty widget
#

idk what the lie group exponential is so i don't understand lee's hint

#

is it related to the geodesic exponential

#

where you go along a geodesic for time t = 1

sleek thicket
#

Well uj

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That's this problem lol

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See part c

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if you have a bi invariant metric they're the same

gritty widget
#

oh GWcorbinHolyFuck

sleek thicket
#

but it's pretty simple

#

Same idea I mean

#

You know about like, integral curves?

#

Did you know that left invariant vector fields on a lie group are complete?

gritty widget
#

that's a nice fact

#

i vaguely recall reading about it

sleek thicket
#

Pretty cool

gritty widget
#

i kinda wish my courses would go into this stuff, seems like i have to go read it on my own

sleek thicket
#

well like, the exponential of a vector X in the lie algebra is γ(1), where γ is the integral curve with γ(0) = e and γ'(0) = X

gritty widget
#

oh so it's basically the same thing but the integral curve isn't a geodesic

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lol

sleek thicket
#

So like how the exponential on a riemannian manifold works but with integral curves instead of geodesic

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Yeah

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This is an integral curve of the left invariant vector field which is X at the identity

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and which starts at 0

gritty widget
#

and exists for all time 😌

sleek thicket
#

Yee

gritty widget
#

so you don't have to worry about scaling issues to define gamma(1)

sleek thicket
#

And then conversely γ(t) = exp(t X)

#

And γ is a group homomorphism R -> G

gritty widget
#

👀

sleek thicket
#

Yee

#

This is like

#

"one parameter subgroup"

#

idk I'm too tired for this

gritty widget
#

maybe i'll read the lee lie group stuff over my break catThimc

sleek thicket
#

It's good!!

#

I wish I understood it better

#

Me and a friend of mine are thinking of reading a book on Lie groups/lie algebras

#

But time...

gritty widget
#

how much stuff from algebra actually comes into play? i'm taking algebra right now so it'd be nice to have the two (algebra, smooth manifolds) really mix together

#

(for lie groups)

sleek thicket
#

Idk

#

I assume rep theory of lie groups is different

#

But on the other hand, there's some stuff which is the same

gritty widget
#

algebra has just been "symmetric group goes brrr" and i want to see a little more sadcat

sleek thicket
#

oh okay lol I was gonna ask if you'd seen rep theory for finite groups

#

So like, I was thinking about this on my own the other day

gritty widget
#

oh god no lmao

sleek thicket
#

There's this theorem called maschkes theorem in finite group rep theory

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It's like the first theorem in that

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And it involves averaging something over your group

gritty widget
#

the most rep theory i've seen is skimming the gelfand naimark duality stuff from my func anal book, and it's not like i actually read it opencry

sleek thicket
#

And the proof works the exact same for compact lie groups!!

gritty widget
#

oh neat

sleek thicket
#

You just need to assume your representation is smooth and take an integral to average

#

anyways, I think there's definitely bits that are algebraicy and bits that aren't, but I haven't studied it yet so idk

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My uni is doing a completely algebraic course on lie algebras right now and I dropped it

#

Lecturer was terrible and I want some geometry

gritty widget
#

geometry > algebra

#

tbh

#

anyone who says "but algebra = geometry" is smoking crack

#

good thing it's 5 am and the people who know more mathematics than me can't come get angry at me for that opencry

#

anyways i'm going to head off to sleep now

sleek thicket
#

lmao

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geometry >= algebra

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But also algebra >= geometry

gritty widget
#

order is not antisymmetric

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😌

sleek thicket
#

we're only in a pre-order though so algebra might not be geometry

#

haha

gritty widget
#

if i notice anything when (if) i look at the problem tomorrow i'll post it here

#

good luck on the problem (and rest of hw)

sleek thicket
#

ty

#

I have two weeks so I'm not worried

#

Benefits of being in post-quals courses lol

quiet pilot
#

I'm working in k[X1,X2,X3,X4] over some unknown field, not necessarily algebraically closed. I want to write the intersection (X1,X2) \bigcap (X3,X4) more explicitly. My guess is (X1X3,X1X4,X2X3,X2X4), but I'm not sure how to prove the inclusion to the right

sleek thicket
#

@gritty widget you were right about not needing covariant derivatives

#

any bilinear function T : V x W -> U between fd vector spaces satisfies $dT_{(p, q)}(v, w) = T(p, w) + T(v, q)$

gentle ospreyBOT
nimble flower
#

is there some easy way of showing a function from a compact space to a compact space is continuous with looking at the open sets?

gritty widget
#

Maybe the closed graph theorem?

pastel linden
#

if the domain and range are metric spaces I believe the function is uniformly continuous

little hemlock
#

i interpreted their question as: "is there a quick-shortcut for testing continuity of functions between compact spaces"

tight agate
#

The fastest way I know is to just claim that it is continuous

little hemlock
#

i believe a continuous map between compact spaces is closed. I can't think of a sufficient condition easier than the usual definition of continuity tho

nimble flower
#

i interpreted their question as: "is there a quick-shortcut for testing continuity of functions between compact spaces"
@little hemlock yeah - that's correct

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hmm maybe the closed graph theorem

gritty widget
#

Oh, I misread the original question, I thought it said "without" open sets, not "with" open sets

coarse kestrel
#

what is a visualization of the one point compactification of a countable set with the discrete topology?

gritty widget
#

i guess i have never used this space before, but why not just Z+infinity at the end?

coarse kestrel
#

i meant like a visualization of it

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like how the one point compactification of R is visualized as a circle

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i guess the one point compactification of Z is just the subset of the circle that corresponds to {∞} U Z

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xD

gritty widget
#

I guess that works

river granite
#

a countable set with the discrete topology?
isn't that already Hausdorff (if it has ≥2 elements) and compact?

gritty widget
#

How is it compact?

#

I guess countable to me means infinite countable (maybe some people use it to mean finite?)

#

Eg I think I have heard "enumerable" as finite or cardinality of integers

river granite
#

aaaaah yes you're right. then you can take e.g. an open cover of singletons and it fails catastrophically

#

for an infinite set

coarse kestrel
#

oh yeah by countable i meant infinite countable

#

So in bijection with the set of naturals

gritty widget
#

all sets are finite

#

just as all holomorphic functions are constant

river granite
#

t. wildberger

tight agate
#

I'm doing a problem which is asking me to interpret $\int_{\mathbf{P^n}}c_n(TP^n)$

gentle ospreyBOT
tight agate
#

where c_n(TP^n) is the top Chern class of the tangent bundle of projective space

#

I computed that it is (n+1).Vol(P^n)

#

and I know that this is somehow supposed to correspond to the number of times a generic vector field on Pn vanishes

#

but I'm unable to make the connection

#

no pun intended

tight agate
#

I found an answer online which used Hirzebruch Riemann Roch and the Hodge decomposition lol

#

and the Borel Serre identity

#

there's gotta be a more low-tech way of doing this

fathom radish
#

given I have the radius, the major axis is the blue line, and the minor axis is the red line, how do I find the shortest distance from the major axis for the curve of the circle

#

I was trying to make radial sanding blocks myself because they are expensive and I ran into this problem

#

im taking euclidean geometry next semester but for right now I only have 11th grader education on it

small obsidian
#

Sorry, your question isn't clear. Shortest distance between what and what?

fathom radish
#

oh sorry. Im trying to find how far apart the blue line and the edge of the circle are only on the y axis.

small obsidian
#

What do you know about the circle? Length of the blue line? Radius?

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Angle from center to edge of blue line?

fathom radish
#

the radius, major axis (blue), and minor axis (minor) are all given. I am essentially setting it up by superimposing an ellipse on a circle where the radius is know

#

another thought is to find the velocity of y via partial derivative given that the edge of the ellipse is half of one period. but im also not sure if a formula for the perimeter of an ellipse based upon just the major and minor axis exist (it probably does).

#

and then maybe integrate the partial of y to get the distance from the major axis?

#

im not sure. Im just using my knowledge of calc because thats what I know. there is probably a much better way to do it

small obsidian
#

"Im trying to find how far apart the blue line and the edge of the circle are only on the y axis."
I took this to mean you're trying to find the length of the red line. But you have that as a given?

fathom radish
#

I only have the maximum though

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I need to find it at every point

small obsidian
#

Oh haha I see

#

That would be
√[r² - x²] - height of the blue line

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Height of the blue is just r - red

fathom radish
#

ah ty

coarse kestrel
#

I don’t see how the locally finite collection implies the closure is the union of the same U’s

gritty widget
#

does bredon not mention it?

#

it's like one of the reasons you'd care about locally finite collections ig

coarse kestrel
#

No it did not

#

Goddamnit

gritty widget
#

😔

#

the proof in the mse post i linked is good imo

#

it's good to keep in mind, it comes up sometimes when you work with partitions of unity

coarse kestrel
#

Yeah

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Thanks

#

That proof on mse is good

sharp yoke
#

whoever ur learning topology as well

coarse kestrel
gritty widget
#

Damn, I cannot understand this. I am not sure if this is "Whoever, you as well are learning topology" or "Whoever, you are learning topology as well"

coarse kestrel
#

No idea

#

But I’ll take that as a compliment

sharp yoke
sharp yoke
#

apparently you can do the forward direction using that the identity function is a homeomorphism if you assume the topologies are equivalent

sharp yoke
#

when you assume continuous i can get the upper bound easily but i can't get the lower bound

#

ok i guess my process is wrong because doing the inverse does nothing for me

#

how do you use continuity to find the bound

elder yew
#

Is that true independent of dimension?

#

Even in infinite dimensions?

#

My fcnl background

#

Is a little lacking

#

I only know finite stuff well

#

lol

#

Really?

#

It's that basic?

#

No, it's ok

#

My background is fucking wonky

#

I deserve it

#

Ahh I see

#

That is fair

#

As you can tell, I was thrown into advanced topics courses without a whole lot of background

#

Ahh, bounded if and only if continuous

#

I knew it was true in finite dimensions

#

I didn't know it was true in infinite

#

Bounded if and only if continuous

#

Yeah

#

The proof is the same as the finite version

#

I only took an applied functional analysis class, where we were interested in Boundary Value Problems

#

and using things like compact operators

uncut geyser
#

bounded if and only if lipschitz if and only if continuous at the origin if and only if takes bounded sets to bouned sets yada yada

elder yew
#

To get results

#

Never took a pure functional

gritty widget
#

just read pedersen 😌

uncut geyser
#

isnt it like

#

bounded means |T(x)-T(y)| = |T(x-y)| <= C|x-y|

#

or am I tripping

gritty widget
#

this is correct

hard wind
#

Let p and q be quotient maps, and r be a map. Let p = q o r. Is r continuous? Is r quotient?

gritty widget
#

let q be a constant map lol

hard wind
#

Well, q might not be a constant map.

#

It could be any quotient map.

gritty widget
#

well then the answer is "not necessarily"

#

i guess you could then ask what conditions on q (or p) you need?

hard wind
#

Okay, thank you

#

What if p and r were quotient? Could we say anything about q?

gritty widget
#

q would be a quotient map

#

falls right out of the definition of one

#

well it's not hard to see

gentle ospreyBOT
hard wind
#

Makes sense.

#

Thank you

sharp yoke
#

@limpid vault thx. Also to address what you said before this was just one part of "walk-through" problem for proving that all norms on Rn are equivalent

#

i only posted that one part which is probably why it seemed weird

#

unfortunately that p set took me quite a while so now im gonna have to brew some coffee as i start my physics problem set also due tomorrow

sleek thicket
#

I cannot deal with this level of indices

gritty widget
sleek thicket
#

the proof is just as bad

gritty widget
#

lmao

#

imagine writing it out with all the sums pepega

sleek thicket
#

Dear god

#

I mean it shows how good Einstein summation notation is

dim meadow
#

@sleek thicket you are like little baby

sleek thicket
#

I am very much a little baby

#

Riemannian geometry pushes the limits of my baby brain

dim meadow
#

Oh I meant with the indices

tight agate
#

Does anyone know if there's a pdf of FGA explained floating around?

#

managed to find a djvu file but those are always horrible

sharp yoke
#

what book is that from

gritty widget
#

the book shamrock posted is lee's "introduction to riemannian manifolds"

tight agate
#

they're pretty neat

#

a lot of cool theorems

sleek thicket
#

they're cool but as i said, my brain is too small

#

lots of ugly notation and computation

#

but the structure/geometry is really nice & good when you're able to see past that

gritty widget
#

how is studying riemannian manifolds?
if you can deal with the occasional terrible computation, it's super nice

#

take all the nice stuff about smooth manifolds, and then add some geometry, and now drawing funny warped squares and curvy lines becomes an actual proof technique

#

(/s)

tight agate
#

there's going to be a class on Fukaya cats over here next quarter

#

im not sure if I should do it as I know pretty much nothing about symplectic stuff

#

other than the definition

#

or the Kaehler case

meager python
#

@tight agate you have some of the chapters in draft versions here:

tight agate
#

yeah I looked at that, some of the links seem to be broken

#

but thanks!

#

oh wait nvm that linked to another page and I could access some lecture notes

#

thanks!

#

Here's the link if anyone else cares:

sleek thicket
#

There's a course on "Canonical metrics in Kahler geometry" here in spring and I haven't decided whether I want to take it

#

I've heard bad things about the prof and the course announcement thingy says "Prerequisite: good handling of multi-variable calculus and mathematical maturity"

#

Which is very concerning to me

sleek thicket
#

Right lol