#point-set-topology

1 messages · Page 223 of 1

delicate hollow
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ok

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question

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if I want to construct smallest open ball around a set

barren sleet
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that's not well defined

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in general

delicate hollow
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would it be B = {x| d(x,A)<M}

barren sleet
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there may not be a smallest open set

delicate hollow
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if its bounded

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there is

barren sleet
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no

delicate hollow
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?

barren sleet
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what's the smallest open set around [0,1]

delicate hollow
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ok

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ive been beat

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damnit

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so I can just say that there is a ball

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around a set

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i dont really need it to be smallest );

barren sleet
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yes

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I see where you are going with that

delicate hollow
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i glanced at the stack overflow answer he provided qq

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i feel bad

barren sleet
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just use def of boubdef

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pick SOME ball that contains your set

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doesn't need to be smallest

delicate hollow
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ok

barren sleet
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just needs to be bounded itself

delicate hollow
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yeah the se gave entire answer

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so like

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if B in C where B is the bounded set and C is the open ball

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then X/C is in X/B

barren sleet
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indeed

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by the way

delicate hollow
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and the points in X/C are connected since X/C is connected

barren sleet
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the problem never requires that the complement only has one component

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it requires that it has only one unboundef connected component

delicate hollow
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yea

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all points in X/C make one unbounded connected component

barren sleet
barren sleet
delicate hollow
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wait

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did I say thaht?

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i didnt mean to say that

barren sleet
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ok

delicate hollow
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wait

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why might X/C might not be a component

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or atleast not a complete one

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needs more elements maybe?

barren sleet
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it might not be a complete one

barren sleet
delicate hollow
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yea

barren sleet
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that is tricky to work with though

delicate hollow
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but

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i got one thing

barren sleet
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try to assume that there are 2 disjoint connected unbounded components and get a contradiction

delicate hollow
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the needs more elements cant be in X/B - X/C

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i can try that too

barren sleet
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that set*

delicate hollow
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yeah

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woops

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again

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i meant to say that

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i wonder if there is a more straightforward way to argue without contradiction that elements of component of X/C cant be in X/B - X/C

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the two sets do form a seperation

barren sleet
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uh

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idk what you're saying

delicate hollow
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ok

barren sleet
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elements of X\C cannot be in X\B-X\C by definition

delicate hollow
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yeah

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but can they share componenets?

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components

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like there might be a connected set D that contains both of them

barren sleet
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yeah

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do you have a clear direction on this proof

delicate hollow
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i might?

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um

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arguing by contradiction

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wait

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you were saying 2 disjoint connected unbounded components cant be a thing

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so we have X/C is one

barren sleet
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no

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X\C is not oje

delicate hollow
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ok

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X/C is in one

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is a subset of one

barren sleet
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but there is a connected component containing X\C

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exactly

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that is one

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now if D is another

delicate hollow
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the other one would need to have points in C intersect B

barren sleet
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what does it mean for D to be unbounded?

delicate hollow
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that there is no open ball around it

barren sleet
barren sleet
delicate hollow
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wait what do you mean be fine

barren sleet
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like

delicate hollow
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oh lol u gave me a visualization

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ty

barren sleet
delicate hollow
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ok i see that

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um

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so problem with D being unbounded

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is that it would need to be disjoint from X/C

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and not contain points in B

barren sleet
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yes

delicate hollow
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but in doing this it cant really exist

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it would need to be in X/C

barren sleet
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can you turn this into a formal argument

delicate hollow
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um sure

barren sleet
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you're on the right track

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when you are done I will tell you mine

delicate hollow
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imma just type it

barren sleet
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alright

delicate hollow
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Let B be bounded in R2
Take C to be an open ball containing B
So X/C is in X/B
Since X/C is connected we have that X/C is a subset of a component of X/B.
X/C is an unbounded subset of a component of X/B
Suppose there is another set A that is an unbounded component of X/B disjoint from X/C.
Then There is no open ball containing A.
So A is in X/C, but this is a contradiction, so there is no other set A that is an unbounded component of X/B disjoint from X/C.
So X/C is the only unbounded component of X/B.
QED
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Im going to be honest

barren sleet
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some statements are not justified

delicate hollow
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I am feeling a little insecure

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with this statement

barren sleet
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yes

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here is my hint

delicate hollow
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Then There is no open ball containing A.
So A is in X/C, but this is a contradiction, so there is no other set A that is an unbounded

barren sleet
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it will be a lot easier if C is an open ball centered at the origin and you consider the radius of C as a revelat quantity

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relevant quantity

delicate hollow
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really?

barren sleet
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yeah

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then the complement of C is all points at least some distance from the origin. this will play along well with the definition of unbounded when doing your contraction

delicate hollow
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ok

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so like

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C = {x in R2| d(0,x)<d(sup({p_x}),sup({p_y}))} where p are points in B and p_x,p_y are their x and y components.

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There has to be a cleaner formulation qq

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oh

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gotta add something

barren sleet
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don't try to figure out the radius of C

delicate hollow
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because it wont contain that point

barren sleet
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just call its radius M or something

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and define it to be an open ball containing A

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which exists by definition

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of bounded

delicate hollow
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ok

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that is way easier lol

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so C = {x in R2|d(0,x)<M} where M is the bound of B.

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well

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that isnt defined

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I should write out definition for bounded first

barren sleet
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yeah

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yeah

delicate hollow
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and then just use that M

barren sleet
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there exists some M

delicate hollow
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probably easier tofolllow

barren sleet
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doesn't need to be a tight fit or anything

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your space could be the unit ball and M could be 500 and nobody cares

delicate hollow
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oh

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ok

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once i do that

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justifying the contradiction is another part

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so

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i assume there is an unbounded component A of X/B

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my guess is to make this all more rigorous

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but when I say there is no open ball of A

barren sleet
delicate hollow
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there is no open ball containing A

barren sleet
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A is already a set, don't use that name twice

delicate hollow
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it is?

barren sleet
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isn't it

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oh oo0s

delicate hollow
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nah i avoided it

barren sleet
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you used B

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I thought it was A

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ok yeah

delicate hollow
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ok

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we can use D tho

barren sleet
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so A

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is the name of the set

delicate hollow
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ok so A

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yea

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unbouned

barren sleet
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there being "no open ball"

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means something better

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it means

delicate hollow
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complement of an open ball

barren sleet
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for each finite value you pick

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it contains points father than that value away from 0

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but R^2\C already contains all points with d(x,0)

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M

delicate hollow
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ya

barren sleet
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so if D really has some points as far away from the origin as you want

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pick M to be your number

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it just contain points with d(x,0)>M

delicate hollow
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so its in X/C

barren sleet
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but R^2\C contains all such points

delicate hollow
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ya

barren sleet
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so it's not disjoint from C

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yeah

delicate hollow
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that makes it way more rigorous

barren sleet
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now I have to go but I will give you my explanation for connectedness

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it helps to have an intuitive sense of open and closed

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closed sets contain everything that is close to them in the metric space

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or topological space (since the topolgies define a sense of "closeness")

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open sets provide "padding" for all of their points

delicate hollow
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contsunf?

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contains?

barren sleet
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sorry

delicate hollow
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ah

barren sleet
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I fixed it

delicate hollow
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yea

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because it includes limit points

barren sleet
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ok read again now

delicate hollow
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and the set itself

barren sleet
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I changed it

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yeah so if a set X is disconnected in the intruitive sense

delicate hollow
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oh wait

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i get it now lol

barren sleet
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it means some set D and it's complement C are "far apart"

delicate hollow
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i get the natural padding part too

barren sleet
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with clopen and everything?

delicate hollow
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ok

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by far apart

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you mean doesnt contain those limit points

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so it cant be closed

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why cant it be open?

barren sleet
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I mean an intuitove sense of far apart

delicate hollow
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wait

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this is how im seeing it

barren sleet
delicate hollow
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oh

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i assumed far apart means not close together

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close together means it contains its liimit points

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far apart should mean it doesnt have its limit points

barren sleet
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D is open because it is far enough from C that some neighborhood of every point avoids C (think intuitively, D and C have some intuitive distance)

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so D is open

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D is also closed because it contains everything close to it

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because C is not close to it

delicate hollow
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wait what is C now

delicate hollow
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oh

barren sleet
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C can't be stealing any limit points from D

delicate hollow
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if it does that means its close to some points in D

barren sleet
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that's how I make sense of clopen

delicate hollow
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wait

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im reading why D cant be open

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why it is*

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oh i guess that makes sense intuitively

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so like

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D's goal is to have all points avoiding C and at the same time not being close to C

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avoiding C means each of its points have an open neighborhood around them, when unioning gives an open set

barren sleet
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yes

delicate hollow
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and not being too close means not having any limit points in common with C which means D can't be closed because inorder to be closed it needs to contain all its limit points

barren sleet
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yes

delicate hollow
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is closed*

barren sleet
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or also

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think

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D is open

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that's all you need

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cause then apply the same reasoning to C

delicate hollow
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oh

barren sleet
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and C being open gives you D is closed

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so whichever of the arguments is easier

delicate hollow
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a set is closed iff it contians all its limit points right?

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and itself

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because Cl(A) = A U A' where A' is set of limit points?

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ok

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ty for intuition

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maybe someday ill make an animation

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or a gif

barren sleet
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yes

delicate hollow
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seems like its easy to visualize euclidean ig

barren sleet
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I'm just explaining intuition

delicate hollow
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idk how notion expands to not R^n

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its not possible to visualize otherwise

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ig?

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maybe there are a bunch of other ways

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i think ill do a presentation on this seems simple and fun

barren sleet
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in math conversations it's easy. get used to everything being rigorous

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but sometimes

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irs ok to not be

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and at this time

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it's just getting intuition for how our idea of connected relates to the topolgical def

delicate hollow
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@barren sleet

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What grade

gritty widget
barren sleet
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wdym

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like year of school

delicate hollow
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ya

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@gritty widget helps me get perspective of my compotition

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wow

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competition

gritty widget
barren sleet
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I'm a junior in highschool

delicate hollow
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really?

barren sleet
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yah

delicate hollow
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damn im doomed

gritty widget
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buddy there are highschoolers in here doing way more advanced shit

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who cares if some highschooler is doing things more advanced than u lol

delicate hollow
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?

barren sleet
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I have no right to tell this to you because I literally such shit about comparing myself to other people, but it's honestly pointless

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there are highschoolers smarter than me like beyong my comprehension

delicate hollow
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oh yeah

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IMO people

gritty widget
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you didn't make IMO????? you're doomed lol gl getting into grad school literally 0.0001% chance

delicate hollow
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I have always had an understanding there are going to be people way ahead of the curve than me

sleek thicket
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I am significantly more competent than all of you and you should quit math now

gritty widget
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compact

delicate hollow
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are you competition chadrock?

sleek thicket
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Especially you tterra

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I am not your competition. You and your competition are like ants to me

delicate hollow
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damn

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comparing myself isnt pointless

barren sleet
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to me it is

delicate hollow
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staying doomed is a good thing though

barren sleet
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comparing to me

delicate hollow
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well look at this

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my goal

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or one of them

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do math research at a high level

barren sleet
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same as me

delicate hollow
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I might be able to achieve my goal

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but not to the most specific degree

barren sleet
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whenever that thought enters my mind my first thought is "I'm never gonna be good enough every9ne else is so much better"

delicate hollow
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well yea

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i know thats true

barren sleet
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do

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I honestly don't know how it works

gritty widget
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the key is to just think you're better than anyone unironically

delicate hollow
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Ive only been the best at a couple of menial things in my life

barren sleet
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and I'm not at that stage anyway

sleek thicket
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I think this is a thorny and complicated issue, but my main take is this

barren sleet
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ow

gritty widget
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@​Moderators

delicate hollow
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I dont get it

barren sleet
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ok everyone shun me until tomorrow

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I need to do homework

sleek thicket
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Remove advanced role

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Add studying role

barren sleet
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good idea

gritty widget
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,ban ethan

gentle ospreyBOT
#

This may only be done by a moderator!

sleek thicket
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Delete discord

barren sleet
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thank you

sleek thicket
#

,ban ethan

gentle ospreyBOT
#

This may only be done by a moderator!

delicate hollow
barren sleet
#

,ban mniip

gentle ospreyBOT
#

This may only be done by a moderator!

gritty widget
delicate hollow
#

wait

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we cant

gentle ospreyBOT
#

No selfroles matching moderator.
See ,selfroles --list for the list of valid selfroles.

sleek thicket
#

Wait was kxrider typing

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I thought I saw someone

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Do they have a real question

delicate hollow
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probably

sleek thicket
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okay whatever ask your stupid integral here

gritty widget
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nvm

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i want to bash my head into the wall some more

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i don't think enough blood has pooled

delicate hollow
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i want to also

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i want to get corona vaccine

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so that my blood can clot in my spine

gritty widget
#

if you're dead you can't get corona

delicate hollow
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and ill die with acute pain

gritty widget
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coronavirus vaccine

delicate hollow
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true

gritty widget
sleek thicket
#

tterra brain damage arc???

gritty widget
delicate hollow
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i mean

sleek thicket
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tterra exsanguination arc???

delicate hollow
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lets be honest

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sometimes there is no solution qq

sleek thicket
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I think this conversation should change

delicate hollow
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what is the question ttera

sleek thicket
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And not continue

gritty widget
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i agree, it should.

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someone teach me about poisson cohomology so i dont have to read

tough imp
delicate hollow
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how did you avoid ping?

sleek thicket
#

Poisson cohomology is a form of sheaf cohomology

tough imp
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wdym

delicate hollow
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how did ytou not ping mods

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dont try and bait me noob

sleek thicket
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Sheaf cohomology is the derived functor of the inclusion of category of sheaves into the category of presheaves

tough imp
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Ohhhhhh right

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delicate hollow
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lol

tough imp
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No it's a cohomology theory of Fish

sleek thicket
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Chmonkey, please do not interrupt my incredibly correct explanation

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Derived functors are when you take F and put a dot over it

tough imp
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but...

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that's...

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the wrong...

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whaaaaaaa

sleek thicket
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chmonkey

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please stop interrupting me

tough imp
sleek thicket
#

I am trying to inform tterra

delicate hollow
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@gritty widget imma pm u but im too lazy to use pointer

sleek thicket
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About sheaf cohomology

tough imp
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Don't listen to Sham, he's a sham

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Sheaf cohomology is the derived functor of the inclusion of O_X-modules into Sheaves

sleek thicket
#

This is so obvious

gritty widget
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actuall

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y

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eh nvm

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im not going to start

sleek thicket
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Oh no was that actually helpful

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wait

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What are you not starting

tough imp
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oh cochain cohomology of its Chevalley-Eilenberg algebra, that makes sense

gritty widget
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i was going to go on a rant about how yesterday i was thinking about poisson structures and how, like, there ought to be some way to measure how much poisson vector fields fail to be hamiltonian

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but

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id literally be the only person understanding it

tough imp
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Hamiltonian like in graph theory?>

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🙂

sleek thicket
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Awww

gritty widget
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anyways it turns out that poisson cohomology actually does measure this

sleek thicket
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I mean you're right

tough imp
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Just like in graph theory

sleek thicket
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It's cool that you figured this out

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nice

tough imp
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Is TTerra actually just UGDG

gritty widget
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the actual definition of poisson cohomology is pain

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but at least the first degree is easy to understand

sleek thicket
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How are you only realizing this now chm

tough imp
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I thought he was just meming

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but the memes never ended

sleek thicket
tough imp
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and now he says something like hamiltonian and poisson cohomology

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so now I know he is serious about his DG memes

sleek thicket
tough imp
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okay...

sleek thicket
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Jesus christ this is

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Very stupid

tough imp
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different DG than what DG means to me

sleek thicket
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not gonna lie to you

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chm

tough imp
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True

sleek thicket
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Do some real geometry...Spec \R

tough imp
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lmfao

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No no remember that a real projective variety

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is a technical term

gritty widget
tough imp
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it really is like Euclidean geometry then

sleek thicket
#

Tterra what is the first degree of poisson cohomology

tough imp
#

How to solve every geometry problem in 8th grad

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draw as many triangles as possible

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stare at it until it becomes obviuos

sleek thicket
#

This is called a "simplicial set"

tough imp
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which is equal to its 1skeleton

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what is a do Carmo

gritty widget
#

i have not

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i wonder if my uni gives me a nice copy

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let me check

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it does not

sleek thicket
#

Wait

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A random pdf I found claims poisson cohomology is the same as de rham cohomology

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Ie singular cohomology with real coefficients

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How are all the cohomology theories the same

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It's fucked

gritty widget
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link

sleek thicket
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oh sorry this was for symplectic manifolds I can't fucking read

gritty widget
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anyways

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there is still some checking to be done

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do not fret

sleek thicket
#

Sorry

gritty widget
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you can have stupid poisson structures

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like

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{f, g} = 0 for all f, g opencry

sleek thicket
#

I looked at the definition though and it seems very similar to lie algebra cohomology

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Which ig makes sense

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Since a poisson structure is like a lie bracket on the smooth functions with an extra condition, right?

gritty widget
#

right

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that condition being that fixing one argument gives you a derivation

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ie vector field

sleek thicket
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Right

gritty widget
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so you can ask what vector fields arise as such

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which is what lead me to poisson cohomology (or to looking it up lol)

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i will look into lie alg cohomology

sleek thicket
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Oh so is the first group like all vector fields/Hamiltonian ones?

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Or some subset of all vector fields maybe?

gritty widget
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some special subset

sleek thicket
#

That feels cohomological

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Closed/exact

gritty widget
#

so alternatively, a poisson structure is a special bivector field, and then you call a vector field X Poisson if L_X(bivector field) = 0

sleek thicket
#

Right

gritty widget
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then its {poisson v fields}/{Hamiltonian v fields}

sleek thicket
#

Ooh

gritty widget
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which was very pleasing to me

sleek thicket
#

Wait

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What's L_X? Don't bivector fields eat like pairs of covectors?

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So like it can't be the interior multiplication

gritty widget
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lie derivative

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oops

sleek thicket
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Ahhh

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Gotcha

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That makes sense

gritty widget
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defined as like, time derivative of pushforward wrt flow or some shit

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i dont remember lol

sleek thicket
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Yeah ik how lie derivatives work

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Just take the lie bracket and then use the appropriate product rules 4head

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It is so fucked up that [X, Y] = L_X Y

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What's going on there

gritty widget
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ikr

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like what

sleek thicket
gritty widget
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proof: insane computation

sleek thicket
#

Hahaha

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sad but true

gritty widget
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i had it on an assignment

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pain

sharp yoke
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@sleek thicket thx i think i wrote an 85% coherent proof

sleek thicket
#

Nice!

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I can't believe I missed that detail

gritty widget
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let $(M, \omega)$ be a symplectic manifold. we say a vector field $X$ is symplectic if the Lie derivative $L_X\omega = 0$, and Hamiltonian if $\iota_X\omega$ is exact. by cartan's formula $$L_X\omega = d\iota_X\omega + \iota_Xd\omega = d\iota_X\omega,$$ so $X$ is symplectic iff $\iota_X\omega$ is closed. cohomology.

gentle ospreyBOT
#

TTerra

sleek thicket
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ah that makes sense

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You mixed up the name of the formula though

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It's cartans *magic * formula

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Because every time you see it

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You go

gritty widget
sleek thicket
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"what the fuck is this magic"

gritty widget
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it just works lol

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cohomology.

sleek thicket
#

cohomology.

gritty widget
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i might bring up poisson cohomology during my presentation

sleek thicket
#

That would be neat

gritty widget
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if i can find anything about it that isn't just the definition then i absolutely will lol

sleek thicket
#

You could do a quick detour into lie algebra cohomology

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Lock the doors

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This is now a homological algebra talk

gritty widget
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im finding that literally everything i find to present about is just a generalization of some shit from symplectic

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so

sleek thicket
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hahaha

gritty widget
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i'll feel weird including too many details cocatThink

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nothing im talking about is new pepega

sleek thicket
#

Do you have interesting non symplectic examples at leaat?

gritty widget
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i do

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i think

sleek thicket
#

Nice

gritty widget
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ah yeah

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i wrote down a little bit about torii being poisson manifolds

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just as a cute example

sleek thicket
#

Oh neat

gritty widget
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but since those are lie groups i can probably go more in depth with that example!!

sleek thicket
#

Those are not symplectic

#

Because of compact

#

Wait no that doesn't make sense lol

#

The even dimensional cohomology groups of a torus are nontrivial

#

But because torii can have odd dimension works

#

There

gritty widget
sleek thicket
#

Neat!

#

Tterra did you know that $\binom{n}{k} = \binom{n}{n-k}$?

gentle ospreyBOT
#

Chadrock

gritty widget
#

uh

#

no

#

i didnt

#

mindblowing

sleek thicket
#

Oh okay, here's an easy proof

#

By the kunneth formula, $\dim H_k(\mathbb{T}^n, \R) = \dim H^k(\mathbb{T}^n, \R) = \binom{n}{k}$

gentle ospreyBOT
#

Chadrock

gritty widget
sleek thicket
#

By poincare duality and orientability of the torus, $H^k(n\mathbb{T}^n, \R) \cong H_{n-k}(\mathbb{T}^n, \R)$

#

easy!

gritty widget
#

show this to discrete math students

sleek thicket
#

someday

gritty widget
#

does this end up being circular or is it actually a genuine proof

gentle ospreyBOT
#

Chadrock

sleek thicket
#

I think it's a genuine proof

#

The computation of homology could end up sus

#

But I don't think so

gritty widget
#

handwave it enough and it's fine

sleek thicket
#

Kunneth formula says this

#

Oops

gritty widget
sleek thicket
#

Okay whatever I can't find a pmg

#

*png

gritty widget
sleek thicket
#

It says if you have like finite CW complexes and you're working over a field or whatever

#

The kth cohomology of their product is the direct sum of the tensors of the ath cohomology and bth cohomology where a+b = n

#

So you keep pulling off circles

#

you can do an inductive argument

#

And get that it's n choose k

#

Probably not circular

gritty widget
#

i see

#

meh even if it were circular you should still give it to intro discrete math students

#

make them shit

sleek thicket
#

lol

#

Did you give the proof with the weird duality thing on your algebra hw

gritty widget
#

i am back to wondering if there is a link between poisson cohomology and lie algebra cohomology

#

In mathematics, a Poisson algebra is an associative algebra together with a Lie bracket that also satisfies Leibniz's law; that is, the bracket is also a derivation. Poisson algebras appear naturally in Hamiltonian mechanics, and are also central in the study of quantum groups. Manifolds with a Poisson algebra structure are known as Poisson man...

sleek thicket
#

I mean yeah the definition of a poisson structure only involves the algebra of smooth functions

#

Ooh these are allowed to be noncommutative though

gritty widget
#

let me find a definition of poisson cohomology

sleek thicket
#

🐟

gritty widget
#

clearly

sleek thicket
#

How are your fish puns coming along

gritty widget
#

i have not nearly included enough in my presentation

gritty widget
#

here is a more down-to-earth definition

#

P the bivector field

#

and [P, ] being the fucky bracket on multivector fields that i dont understand

sleek thicket
#

This is more down to earth

gritty widget
#

i have written "Is there a link between Lie algebra cohomology and Poisson cohomology?" down in my notes

#

i do not think i will pursue it any more tonight

#

but ty for bringing that up

sharp yoke
#

how do you justify that f is differentiable here?

#

oh wait i just realized how to do it as a posted it

#

nvm

sleek thicket
#

Nice!

plush needle
#

If I am given two geodesics $γ_1$ and $γ_2$ and a distance function $d$ that gives me the distance between any two points on the geodesics, what conclusions can I draw about the geodesics from the information given by $d$?

gentle ospreyBOT
#

Roenbaeck

plush needle
#

(this is a more general question than one I posted earlier about "boxes", but essentially the same problem)

#

I'm also interested in any constraints under which it would be possible to say much more. Like, "if we assume the curvature is uniform, then..."

plush needle
#

I have closed form expressions for $d(γ_1(t), γ_2(t))$ in a set of spaces, as a clarification.

gentle ospreyBOT
#

Roenbaeck

silent oasis
#

Not sure whether this room or the category theory room is more suitable for this question. Let $k$ be some field, $V$ a $k$-vector space. In group scheme theory, people work with the functor $\operatorname{Aut}(V)$ from the category of $k$-algebras to $\mathbf{Grp}$ which assigns to a $k$-algebra $R$ the group $\operatorname{Aut}_R(V \otimes_k R)$, where $\operatorname{Aut}_R$ denotes the $R$-linear automorphisms. What does this functor do on morphisms?

gentle ospreyBOT
#

harraq

silent oasis
#

If we restrict to the finite-dimensional case, for a morphism $f: R \to S$ of $k$-algebras, $\operatorname{Aut}(V)(f)$ goes from $GL_n(V \otimes_k R, R)$ to $GL_n(V \otimes_k S, S)$, where $n$ is the dimension of $V$, and can be defined by pushing forward the coefficients. One could extend this definition to the case when $V$ is not necessarily finite-dimensional using choice to construct a basis $\lbrace v_i | , i \in I \rbrace$, observing that $V \otimes_k T$ is a free $T$-module for any $k$-algebra $T$, hence any automorphism is given by an "infinite matrix" in a sense that can be made precise, and pushing forward the coefficients of that matrix as in the finite-dimensional case. However, it remains to show that this preserves invertibility and is overall a bit cumbersome.

I feel like there should be a more conceptual, diagrammatic way to define how $\operatorname{Aut}(V)$ acts on morphisms. Can anyone help me out here?

gentle ospreyBOT
#

harraq

tawdry widget
silent oasis
#

I'll illustrate the action of $\operatorname{Aut}(V)$ on morphisms in the case that $V$ is finite dimensional. In that case, $V \otimes R$ is a finitely generated free $R$-module and any $R$-linear automorphism of $V \otimes R$ is given by an invertible square matrix with entries in $R$. Let $f: R_1 \to R_2$ be a ring homomorphism. Then $f$ preserves units. If $M$ is an invertible square matrix with entries in $R_1$, then applying $f$ to every matrix entry yields a square matrix with entries in $R_2$. Moreover, the resulting matrix is invertible, because its determinant is a unit in $R_2$. I hope I could illustrate the finite dimensional case. Note that this relies on a choice of basis, which is something that you generally want to avoid

gentle ospreyBOT
#

harraq

timber junco
#

i need help in learning how to factorize

tepid nest
#

@timber junco This isn't the correct channel

timber junco
#

ahhhhhhhhhhhhhhhhhhhhhhhhhh

#

i thought the quadratic formula was geometry based?

tepid nest
#

No, these are the advanced channels

timber junco
#

sorry i'm in AP thats why i put in advanced

weak idol
#

we have a curve r(t).

r(0) = (2019,-1)
r'(0) = (0,1)
the curvature of the curve is fixed to be 1/t^2+5t+6

r(1) = ?

#

im sorry if this doesnt count as advanced, but i asked in #calculus and i didnt get any guidance

weak idol
#

rate of change of the unit tangent wrt the arc length

gentle ospreyBOT
#

slimvesus

delicate hollow
#

typo?

#

show connected by not path connected meant to say, show connected but not path connected?

sweet wing
#

probably

delicate hollow
#

☑️

#

quick question

#

for proving connected

#

can you argue this

#

suppose set is open

#

and then suppose that the set contains all its limit points

#

show some contradiction in that?

sweet wing
#

all sets are open in itself

#

recall how we define connectedness

delicate hollow
#

i know how we define it

#

its no clopen sets

#

the problem is to prove topologist sine curve is connected but not path connected

#

i was thinking of doing argument by assuming a seperation, then showing it doesnt exist.
then proceeding to show it isnt path connected, which i honestly don't know off top of my head

sweet wing
#

more accurately there are only 2 clopen sets

#

the empty set and the entire space

delicate hollow
#

ya

#

yea

#

um

#

def is

#

graph of your given f(x) unioned with verticle line from -1 to 1 at origin

#

and subspace topology on r2

#

so yeah the closure of graph

#

its continuous

#

so um

#

open sets get mapped to open sets

#

specifically

#

open in R^2 is open in (0,1]

#

and (0,1] is connected

#

wait uh

#

i can just say connectedness is perserved by continuity

#

and then just move on to arguing not path connected

#

but ig that might be harder

long hornet
#

Let p, q be two points in a connected topological manifold. Shamrock essentially proved that there is a homeomorphism f sending q to p and is equal to the identity outside a prescribed open set containing the path (I think? At any rate, this is possible), but I still wanted to find a coordinate ball V containing p, q. I think the following argument should work, but I feel like I am missing something.
Pick a coordinate ball B around p, and let p' =/= p be in B. Now assume we have f so that it fixes p and sends p' to q, and let B* = f(B), which is also a coordinate ball around p. Now the point is that f(p') = q, so q is in B*.
To make f fix p, we find a neighborhood of p that is disjoint from a neighborhood of the path C = f([0, 1]). This is possible because {p} and C are disjoint closed sets, and M is normal.

worthy canopy
#

how do i parametrize a curve if i know its curvature (as a function itself), a point on the curve, and a tangent vector at that same point?

tough imp
worthy canopy
#

how do i parametrize a curve if i know its curvature (as a function itself), a point on the curve, and a tangent vector at that same point?

delicate hollow
#

@tough imp h

#

yea

#

if f:X->Y continuous

#

then open in Y implies f^-1(Y) is open in X

#

say X was connected

#

then Y is also connected by continuity

#

or wait

#

i think it needs to be surjective

#

i dont remember

tough imp
#

the image of a connected set is connected

#

so it would need to be surjective

#

else every set is continuous by just taking a map from the one point set haha

honest terrace
#

if f: X -> Y is continuous, then f(X) is connected

#

so Y is connected is connected if f is surjective indeed

tough imp
#

why you copying what I'm saying smh smh you gotta change your name to Chika-Blyat now

honest terrace
#

i'm just too slow

tough imp
#

I'm sorry :(

#

it's okay

#

you can stay Shika-Blyat

honest terrace
#

fortunately every connected space is a connected space !

tough imp
#

Ultra you're wrong

#

I care about spaces not up to homeomorphism

honest terrace
supple locust
#

If I have a continuous function from unit disc to circle i.e. D -> S1 , is there always an x in S1 which is fixed under this function?

barren sleet
#

yes but idk how to show it without brouwer fixed point theorem

supple locust
#

but don't we have D -> D map in brouwer fixed point theorem ? I dont see how this follows from that

gritty widget
#

D is the closed unit disk? compose with the inclusion map S^1 -> D if you really want it to be D -> D

#

this makes no difference, a map into S^1 is practically the same thing as a map into D

barren sleet
#

if its continuous from D to S1 its continuous from D to D, just consider the original function to have codomain D

#

oh yeah terra said it better

#

composing with inclusion map

gritty widget
#

hm

supple locust
#

hmm. for some reason I thought that brouwer required the map to be surjective

barren sleet
#

nope

#

it works super well when its not surjective actually

supple locust
#

yea

#

I just checked the statement again

barren sleet
#

special cases of brouwer become much easier if you actually require the range to be "small" enough

gritty widget
#

this is now reminding me of a cute complex analysis problem i did earlier cocatThink

barren sleet
#

idk complex analysis

#

and im not in a rush to learn

#

considering what else i dont know

gritty widget
#

find a holomorphic mapping of the open unit disk into itself with no fixed points. can you pick it to be biholomorphic?

barren sleet
#

idek what holomorphic means

gritty widget
#

everywhere complex differentiable

#

which is magically the same as complex analytic

barren sleet
#

yeah i have heard of thta

#

that seems wild

gritty widget
#

it is!

barren sleet
#

but idk enough complex analtsis

gritty widget
#

follows from cauchy's theorem

barren sleet
#

i could not eyeball a function and twll you whether its complex differentiable or not

gritty widget
#

if i show you the cauchy riemann equations

#

then you will be able to

barren sleet
#

ok i have a question

gritty widget
#

cauchy's theorem is "f is holomorphic only if f dz is closed" (converse is called "morera's theorem" in my notes)

#

which gives you cauchys integral formula which gives you complex analycity

barren sleet
#

if you have the open unit disk D and a smaller disk within it that has opposite points at some bounary point of D and the origin

#

so like

#

radius 1/2

#

and they would share a boundary point with each other

#

if the disks were closed

#

if you shrink the unit disk into that disk

#

there are no fixed points

tight agate
gritty widget
#

cayley transform is so useful

barren sleet
#

but i cant tell if mine is holomorphic cause i just have no clue how to work with that

tight agate
#

holeomorphism

barren sleet
#

whats a holeomorphism

#

google doesnt knpw

tight agate
#

it isnt a thing

#

it will be a thing

barren sleet
#

oh

tight agate
#

someday

barren sleet
#

@gritty widget what is wrong with my answer (unless its magically right)

barren sleet
tight agate
#

it isnt hard if you're willing to accept that there is a holomorphic map from the unit disk to the upper half plane with a holomorphic inverse

barren sleet
#

hmm

tight agate
#

but if you're willing to accept that

#

then map to the upper half plane

#

shift the plane

#

and map back

barren sleet
#

omg

#

that is smarty pants

#

thats a bijection as well

#

mine (if it even works) is only an injection

barren sleet
#

i am trying to think of one rn

tight agate
#

they teach you about those maps in a complex analysis class

barren sleet
#

im confused about why its the half plane

#

cant you just as well shift the whole plane

tight agate
#

this is where the holomorphic-ness comes in

#

there is no holomorphic bijection between the complex plane and the unit disk

barren sleet
#

:(

tight agate
#

but there is one between the upper half plane and the disk

#

weird eh

barren sleet
#

thats so weird

#

like

#

..

#

i feel like i can think of one

#

must not be holomorphic

tight agate
#

it's called liouville's theorem

#

any bounded holomorphic function on the plane is constant

#

so if it maps into the disk

#

it's bounded

#

and therefore constant

barren sleet
#

whats wrong with this?: biject [0,1) with [0,infinity) in a smooth way that has a smooth inverse in R. then send eveythign in the disk to the number in the same direction but the abs value scaled appropriately according to the bijection?

tight agate
#

it wont be holomorphic

barren sleet
#

is complex analysis generally harder than real analysis (at the introductory level, i know each can like get as hard as you want)

barren sleet
tight agate
#

real and complex differentiability are very different things

barren sleet
#

damn it

#

i thought smoothness was sure to be enough

tight agate
#

say I have a function from R^2 ---> R^2

#

and say it's differentiable at some point

#

then you have the corresponding jacobian matrix

#

if it's complex differentiable, the jacobian commutes with multiplication by i

barren sleet
#

am i misunderstandign something

#

or how can it not

#

oh

#

do you mean treating C as R^2?

tight agate
#

sure

barren sleet
#

ok

#

so in the real scenario multiplying by i is multiplying by the matrix:

#

(0 1)
(-1 0)

tight agate
#

so you want it to commute with a 90 degree counterclockwise rotation

barren sleet
#

or something

tight agate
#

ye

barren sleet
#

that is cool

ivory dragon
#

engineering students take complex analysis so

tight agate
#

so if the jacobian is $\begin{pmatrix}
a & b\
c & d
\end{pmatrix}$

ivory dragon
#

im shitposting, they take a non-rigorous computational version

gentle ospreyBOT
#

Brotivic t-structure

barren sleet
#

so like

ivory dragon
#

and even then, only certain disciplines (electrical) do

barren sleet
#

complex analysis\the interestinf stuff

ivory dragon
#

i mean it still covers the important theory

barren sleet
#

it needs to be symmetric right?

#

antisymmetric?

tight agate
#

Then we're demanding that $\begin{pmatrix}
-c & -d\
a & b
\end{pmatrix}$ is equal to

barren sleet
#

oh i see

gentle ospreyBOT
#

Brotivic t-structure

barren sleet
#

its a strong condition

#

a=-d and b=-c

tight agate
#

ye something like that

barren sleet
#

but wait

#

a=d as well

#

so a and d are zero

#

b=-c

#

omg

#

that makes perfect sense

#

the derivative is literallt just like a multiple of i

#

actually

#

that seems very restrictive

tight agate
#

no

#

nothing is zero

barren sleet
#

:(

tight agate
#

lemme write it out

gentle ospreyBOT
#

Brotivic t-structure

#

Brotivic t-structure

barren sleet
barren sleet
tight agate
#

up to a -1

#

so a = d and c = -b

barren sleet
#

oh yeah idk how i got a=-d

#

that makes more sense

#

becaise then it acts like a general complex number

#

which is what i ex[ect

#

expect

tight agate
#

these are called the Cauchy-Riemann equations

barren sleet
#

but the othe way got me a multiple of i

tight agate
#

im pretty sure I did the calculation right

#

ye it's a = d and c = -b

barren sleet
#

yeah

tight agate
#

so you can already see that the jacobian of a holomorphic function is a lot more special than the jacobian of a real diffable function

barren sleet
#

yeah

#

well like

#

in this interpretation

#

R^2->R^2 is like a 1d function

#

and we already know for real differentiable functions, the jacobian is just [c] so it can be thought of as c=f'(x)

#

and this rwsult seems like the same thing

#

the jacobian is like the matrix equivalent if a general complex #

#

c

tight agate
#

right

honest narwhal
#

Ooh complex analysis

honest terrace
#

Hey quick question. What would be the prerequisites to start diving into algebraic topology, on the topology side ?
I've recently opened Hatcher but I was already kind of lost while reading the part on cell complexes in the chapter 0.
Or maybe is there a more noob friendly intro to alg top than Hatcher ?

gritty widget
#

rotman

honest terrace
#

ooh

#

that looks a lot more approachable as a beginner

#

thanks a lot catthumbsup

gritty widget
#

i remember briefly reading hatcher when i wanted to learn algebraic topology. it was weird

uncut surge
#

it's a pretty book but somehow i also never liked the style

gritty widget
#

i liked it, however some exercises are a bit too vaguely stated

#

The following problem makes me wonder something

#

Let $$f:\mathbb{R}\rightarrow \mathbb{R} $$ continuous and $$ \lim_{x\rightarrow +\infty }f(x)=\lim_{x\rightarrow -\infty }f(x)=0 $$. Prove f is uniformly continuous.

honest terrace
#

add a _ after the \lim

#

so that you have \lim_ instead of lim

#

so that the "x -> +oo" goes under the lim

gritty widget
#

yea thanks i just copied it from #calculus lol

#

oops

gentle ospreyBOT
#

Carla_

gritty widget
#

If we extended f to the extended real line, it would still be a continuous function i believe. However idk if uniform continuity makes sense in that new space. Could this be somehow used to show f is uniformly continuous?

honest terrace
#

so uniform continuity may make sense in the new space

#

Just see it as a metric space

gritty widget
#

but it is not a metric space

#

what is the distance between -infinity and 0 for example?

honest terrace
#

it is metrizable

gritty widget
#

right

#

its equivalent to [0,1] in some sense

#

but idk if that equivalence can be used to transfer uniform continuity

#

cuz the metric might not be compatible with the original metric in it's interior

gritty widget
#

Hm, I wonder if you can do the trick where you swap the metric d with d(x, y)/(1+d(x, y)), and then define d(x,infinity)=1. I know this generated the same topology, but not sure if the metric is similar enough that uniform continuity transfers over

barren sleet
#

if it forms the same topology how could continuity be ruined

#

oh

#

uniform

tough imp
#

Then on [-a,a] since this is compact f is uniformly continuous, and then use the fact f is bounded on the complement to show its uniformly continuous there as well or something?

#

That’s my first instinct at least

gritty widget
#

Yea ofc, but i'm curious if could use the extended real line somehow instead

tough imp
#

Ahhhh okay

#

Then I have absolutely no idea

bright acorn
#

Ok so

#

I want to have some intuition on the following thing

tough imp
bright acorn
#

Suppose you have an n-dimensional C^{\infty} manifold and you pick a point p in M.

#

We can see that the set of all real valued C^{\infty} functions f : M -> IR that vanish at p forms an ideal on the ring of C^{\infty} functions from M to IR

#

and you can use this ideal

#

call it I

#

To define the tangent space of M at the point p as the dual of the quotient I/I^{2}

#

But I really don't quite get the intuition behind this definition

#

you can define the tangent space of a manifold at a point using curves or derivations

#

and it's all fine

#

But I really don't get this one

obtuse meteor
#

I guess the intuition is

#

you're ignoring higher order information

#

which is what a tangent vector should be

#

only the first order information a la taylor series

bright acorn
obtuse meteor
#

I mean I/I^2 fairly clearly reads as "you have I which is things vanishing at zero, view these as smol bois, throw away all smol bois * small bois which is I^2 and call those 0"

#

so you have only first order smol bois

tough imp
#

This is not for manifolds I will preface

#

This is for varieties, and their tangent space, but I assure you the analogy is very similar

#

On page 38

#

the author goes through essentially this

#

You can identify a local chunk like being in A^n (this is like taking a chart to be in R^n)

#

And then you can define the tangent space via partial derivatives the way we usually think of it

#

From there they show that if you are embedded in affine space that the analogous I/I^2 is isomorphic to this tangent space

#

The analogy for manifolds is practically exactly the same

#

I’d give a manifolds reference if I could, but I don’t know of one

#

This helped me swallow the I/I^2 pill since you see an explicit isomorphism between what you intuitively view as the tangent space and I/I^2

bright acorn
#

I see

#

Yeah from what I have heard

#

this definition is usually more useful when dealing with algebraic varieties

#

But it's a nice little bonus to know that you can also define the tangent space of a manifold at a point this way

#

Thanks for recommending a reference for the subject

tough imp
#

Give me a few minutes, I have a book which might have an explanation for this

#

It’s a manifolds book done using locally ringed spaces

#

So if anything I know of would have this sort of algebraic description, it would probably be this one

bright acorn
tough imp
#

Also for what it’s worth, do you know what the dual numbers is

#

K[x]/(x^2)

#

This is pretty much what Faye was sayinr, and also how I think of I/I^2 sort of

tough imp
#

So elements of this look like

#

a + bx

#

And then multiplication operates like

#

(a + bx)(c + dx) = ac + (ad + bc)x

#

So you’re considering essentially the first order information

#

The way to think of it is like

#

a is a point

#

And the value b is like this infinitesimal information, sometimes people use epsilon instead of x

#

Think of x as being some number thats sooooo small that when it’s squared it becomes 0

#

But it still exists

#

So the idea here is that like a + bx is kind of like the point a

#

(Say on the real line)

#

And b is this tiny little vector at a

#

So say, 1 + 2x is like the point 1 with this vector pointing two to the right from 1

#

So this captures tiny infinitesimal data which is kinda what you want in the tangent space

#

But now let’s consider if we instead looked at

#

(x)/(x^2)

#

Okay, this is a special case of I/I^2

#

Well an element of (x)/(x^2) looks only like

#

bx

#

Essentially the a = 0

#

So now all we’re left with is the vector

#

Aka the tangent vector

#

Also if we looked only at polynomial functions on R, then (x) is exactly the ideal of functions vanishing at 0

bright acorn
#

oooh

#

Ok I see it

#

So the intuition is literally considering information up to a first order approximation?

tough imp
#

Basically

#

You could consider (x)/(x^3)

#

To capture 2nd order info too