#point-set-topology
1 messages · Page 230 of 1
Okay suppose we know it for affines
We have a V < Y such that f^-1(V) is a finite union of affine opens U_i which are finite type blah blah so they're finite
Yeah
well okay, just pick out some affine open, call it U
You get subsets of Y for each i
and suppose you have a V for that U
In X?
yeah
Sure
Does U contain all fibers of eta?
So cover X by finitely many affines
Then for each apply the affine case
this gives Vi in Y with f^-1(Vi) intersect Ui -> Vi finite
We intersect because you're applying the affine case to the restricted map Ui -> X -> Y
I don't see why it would have to
But I'm also not sure why you're asking
Oh wait
It does
Sorry
oh it does?
can you force one to?
For a second I thought it did but I don't see why it would
Why are you asking it to? How does that help?
If you can, you can look at its complement
it doesn't map to eta because no fibers of it are in it
call this thing Z for now
sure
Z is also quasicompact
Because it's closed in a qcompact space?
Lets go with what I said
sure
anyway
if you have a qc morphism (so automatic when the source is qc)
f: X -> Y such that it misses the generic point
you can find a nonempty open of Y, containing the generic point with empty inverse image
wait so are we giving Z a closed subscheme structure?
sure
Also yes I agree with this
Just take the complement of the closure
I guess this is totally topological
yeah, basically
anyway, this solves the problem
because this gave an open of eta
which has empty inverse image in the complelemtn of U
aka the inverse image is in U
so now by being local on the target
you have f^-1(V) < U
is finite to V
Solvrss the problem as in, reduces to the affine case?
yeah
I think I follow this
like, if we know the affine case right
right
(assume U can be chosen to contain the fiber of the generic point)
such that f|_U^c^-1(V) is empty
Yes okay
so this says f^-1(V) < U
yeah
sure
right
Well I mean it does need an affine containing all fibers of eta
but it doesn't use affineness all that much
yeah
Sorry I just meant like
This reduction isn't really a reduction to the affine case
It gives us a way to shrink X
And maybe we can find an affine fitting the shrinking conditions
Rip
Oh okay
so like, you have U -> Y, both affine
Oh wait yeah
How do you know the smaller map is affine still
I guess you just choose V to be affine
And then you're fine
right
okay so
all we need is
to find an open U < X, such that f|U: U -> Y is finite
and that all fibers of eta are in U
And we can also shrink Y if needed
Yeah you will need to shrink Y in some cases
to any open
A^1 \ {0} -> A^1
So this almost directly follows from the affine case
in that case we have U -> Y finite type
get a V < Y such that f^-1(V) -> V is finite
Sure
oh wait, but then f^-1(V) automatically has all fibers of eta?
as long as V contains eta
oh sure
You apply the affine case to the restricted map
right
I can't think of a case where the fiber has multiple points lol
Oh I guess a dvr going into the localization maybe?
Or even Z -> Q?
No
That's backwards sorry
Z -> Z/pZ?
k[x] and k[x,y] I think?
oh that's just not genericdally finite
Oh right
maybe if it's F_p?
From or to what?
Oh for k[x] -> k[x, y]?
yeah
I think it's still not generically finite
Spec F_p[x, y] still has a lot of primes
yeah
Wait actually
Why isn't it finite for k = C?
Oh I guess like the generic point of a horizontal line
Yes
yeah
generic points of irreducible curves usually sit over 0
I think
When I workeed through it earlier
Makes sense
hmm
I'm thinking of primes whcih split
So in Z -> Z[i], the prime (5) is the preimage of the primes (1+2i) and (1-2i)
We can localize both at the multiplicative set S = Z\(5)
So we have Z_(5) -> Z_(5)[i]
Oh but rip the generic point of the left is (0)
Not (5)
Are the fibers of eta
generic points of irreducible components of X?
wait
X is also integral
wait wait
is what I originally asked true?
Which part?
fibers of eta
X has exactly one irreducible component
yeah
so like, no
I'm trying to understand the following calculation using the tetrad formalism
However for the coefficient of gamma_2[12] I don't quite get why is there a factor of 2 in the denominator
Anyone have any idea?
Moth In Shambles
The first direction is trivial: if f extends to f' then pf' extends pf
The second is harder though
I'm not sure where being a cofibration comes into this
I guess we have $q \colon Q \to P$ with $H \colon P \times I \to P$ and $K \colon Q \times I \to Q$ where $H(x, 0) = qp(x), H(x, 1) = x, K(x, 0) = pq(x), K(x, 1) = x$
Moth In Shambles
I'm self studying basic topology atm
considering R with it's usual topology
are closed sets the union of intervals?
not necessarily closed intervals--just intervals in general
and also we let singletons be intervals
As in, you would want to include open intervals?
Then anything is a union of intervals.
(I think the answer is yes, closed sets are a countable union of closed intervals, including singletons and rays, but I'm not sure)
It is true that open sets are a countable union of disjoint open intervals, maybe there is an easy argument to prove the thing about closed sets
okay hmm, perhaps not including singletons
Ah, damn
oof
Wait
The corresponding statement for open sets would be that they're countable intersections of open intervals, which isn't true
It is, R is second countable
with only intervals in the countable basis
we also get disjointness as 8da said
I don't see how that applies to intersections
Oh sorry I misread
Yeah I wasn't saying anything much of substance, but I feel like these sorts of intuition traps are avoided better by thinking of open sets rather than closed sets
Wait Cantor set is an uncountable totally disconnected subset of R, so it seems intuitive that it would divide R into uncountably many components, but the complement is open so must be a union of countably many path connected open sets
Wtf
Yeah, that is weird to me

It kind of feels like I'm misunderstanding something
Could be legit
Would definitely not be legit if Cantor set were discrete
But I don't know how to think about totally disconnected sets that are not discrete 
Oh yeah countable cover of complement by open intervals is also kinda obvious
Following the construction of the Cantor set
By removing the middle thirds
It feels unintuitive because it seems that you could take any countable cover of the complement by intervals and get a surjection onto the Cantor set by taking infimums of all the open intervals, but that doesn't work because there are decreasing convergent sequences in the Cantor set 
One thing you can do is you can define discrete partitions of R. A discrete region = a union of parts in a discrete partition. Closed sets are exactly the intersections of discrete regions. [By discrete partition I actually mean a cover of R by intervals which intersect at end-points]
the same thing happens here than with R\Q, no ?
Q won't be closed
oh huh yeah, but still
like I'm trying to relate this counter-intuitive fact to something I understand a bit better
that Q is countable, but dense in R (so rational between irrationnals and conversely) which is uncountable
the unintuitive part in both claims seems related

(not sure if I'm being clear here)
I mean Q complement can't be a union of open intervals because it's not open
yes, I get that
I'm not speaking about the open/closed stuff here
just that you can fit uncountably many elements between countably many elements in R, or the reverse

A friend of mine always says that R isn't nice. As I learn more maths, I more and more lean toward agreeing with him 
what's nicer
F_2
true, in R you can't always do sqrt(x), but in F_2 you can always do sqrt(x)
in fact you can do nth roots for all n
which, by definition, means thst F2 is algebraically closed
I have written this proof of orientability of the cover of an orientable manifold. Can someone verify it and let me know? Thanks.
why is the set of all smooth vector fields on a manifold infinite?
i.e. why is the vector space of all smooth vector fields an infinite dimensional R vector space?
I can see it is a vector space,but can't see why inf dimensional
try to list out its basis vectors
Hm, a guess: the space of tangent (cotangent?) vectors at a point is finite dimensional (the dimension of the manifold). Along these lines, if you could extend a set of k tangent vectors at various points on the manifold to a full smooth vector field, then letting k go to infinity would show that it is infinite dimensional.
On the other hand, maybe another approach is to consider some path on the manifold, and consider various parametrizations of it. All the various parametrizations should give ride to an infinite dimensional vector space of vector fields along the path, which can probably be extended to the whole manifold
(I am just sort of bullshitting out loud, so no guarantees this is correct. And I do not even remember enough about manifolds to know tangent vs cotangent 🙂 )
that's like asking why the space of smooth functions is infinite dimensional
yes this is what I can't see
yeah, sounds like you're conflating it with the tangent space or something
a vector field is a smooth map $X:M \to TM$
ProphetX
but why is the collection of all such objects infinite dimensional?
if you pick M = R^n then it's a smooth map R^n -> R^n
and like
you can have polynomial maps
that's already infinite dimensional
Ah yeah, I guess it's easier to just reduce to the Rn case immediately
Yeah it's a fun exercise to try and show why already all the monomials 1, x, x^2, ... on an open interval of R are linearly independent
honestly a picture might help
there's a lot of ways to put vectors on a manifold
@cursive flume don't delete your messages
I thought it was very stupid what I said that's why I deleted
I wanted to ask whether thinknig of assigning a vector to each point of the manifold would make this infintie dimensional
but that's not true,because by definition one vector field is such an assignment 
You can just pick an infinite sequence of disjoint open balls on the manifold and put a smooth vector field on each of them that extends to zero outside its little ball
Kind of the same idea as this except it's smooth
the space of all functions from R to R is.. like... cardinality-of-P(R)-dimensional, so very very big infinite
for smooth functions I don't know if it's cardinality-of-R-dimensional or cardinality-of-N-dimensional
most likely cardinality-of-R-dimensional
so very big infinite
yep constant functions are smooth
oh wait you said dimensional
Handsome
silly question, but when we define the commutator of vector fields, when we write $[X,Y]:=XY-YX$, do we mean $[X,Y]:=XY+(YX)^{-1}$, where - denotes the additive inverse of YX?
ProphetX
since in particular there is a vector space structure,we can make sense of an additive inverse
thanks I was just not sure about this and wanted to clear it down 
😮 this is enlightening
I never thought about it like this
but now it makes sense
commutator in the uhhh ring of linear operators on smooth functions
to be pedantic
ring commutator and group commutator are slightly different, which is why i butt in
but nevertheless this holds in ring case too?
or not anymore
I think it is just a notation to make life simpler and not write (YX)^{-1} always
what I meant is the remark here
cause if I just write XY-YX i'm not sure what - means
rings have additive inverses
ahh right
so the ^-1 denotes the additive inverse always
but not in cae of rings
if I write out explicitly additive inverse then even though we ahve algebra structure the sentence is correct,right?
ahh so it's the convention
I see
lie bracket 
Wait, if a set is both closed and open then the closure of that set is the set itself, right?
if a set is closed then its closure is itself, so yes
okay good, thank you!
this is probably an extremely stupid question but if A is a retract (though not necessarily a deformation retract) of X why does the inclusion map induce an injective homomorphism of the fundamental groups
couldn't there be 2 paths that are homotopic through points in $X\setminus A$ so they are separate elements of $\pi_1(A,x_0)$ but the same element in $\pi_1(X,x_0)$
Lagrange the Multifarious
The injectivity says that exactly that thing cant happen
injectivity of the inclusion map?
or of the homomorphism between fundamental groups
injectivity of the homomorphism
well yeah that's what I'm asking. Why is the map injective
saying "it's injective because it's injective" doesn't really help
ah so if r is the retraction, i is the inclusion, then ri is identity, so r*i* = id, so i* must be injective
oh right that makes sense I think
is U(1) simply connected?
I found that U(n) is not simply connected,but it did not specify if n>1 or n>=1
U(1) is the circle S^1 right
ah
then why are we allowed to get the group U(1) from its lie algebra u(1)?
ProphetX
but then the exponential map won't be surjective, or?
also is the statement right that u(1)=purely imaginary numbers? I didn't find it anywhere in books/internet but I computed it myself and seems to be so
i believe so
could you elaborate? i'm not too comfortable with lie theory, but i know that if we have a lie algebra g then we ought to be able to find a simply-connected lie group whose lie algebra is g, but i don't think that theorem says anything about not-simply-connected lie groups
i am interested in knowing the answer 
yes this is my question too
in physics we always simply write u(1)->exp(u(1))
I know that we can lift any rep of a lie algebra to a rep of a smiply connected lie group
what would be the simply connected lie group to u(1)?
ProphetX
this is what we always write in physics
the lie algebra of $U(1)$, i.e. $\text{u}(1)=i\alpha$, then why can we 'just exponentiate it'?
ProphetX
or we actually are not allowed but we are sloppily doing this? 

lol wtf
if it helps, im pretty sure this is the example the exponential map in lie theory is named after

this is so confusing 
Hi, I have a question about metric spaces
If I have a compact space and a convergence sequence. Is the set of point of the sequence a close set?
include the limit and the answer is yes
Only if you include its limit
hmmCat
Ty
for example, the sequence 1/n in [0, 1] (a compact metric space!!) is convergent, but the set {1, 1/2, 1/3, ...} is not closed (after all, it doesn't contain the limit point 0). append 0 and it is
isn't the simply connected lie group with lie algebra u(1) just (R,+)
that's what i tried to say, but yours is clearer ig
Hi guys, I have a question about the calculation of the Riemann curvature tensor. To calculate the Riemann coefficient for a metric $g$, one can employ the second Cartan's structure equation:
$$\frac{1}{2} \Omega_{ab} (\theta^a \wedge \theta^b) = -\frac{1}{4} R_{ijkl} (dx^i \wedge dx^j)(dx^k \wedge dx^l)$$
and using the tetrad formalism to compute the coefficients of the curvature tensor.
Now I'm trying to properly understand this method, I was doing this exercise for which I obtained:
$$\frac{1}{2} \Omega_{ab} (\theta^a \wedge \theta^b) = -\frac{1}{4} A (dx \wedge du)^2 -\frac{1}{2}B(dx \wedge du) (dy \wedge du) - \frac{1}{4} (dy \wedge du)^2$$
However, from here I'm not quite how I would read the coefficient for the Riemann tensor. From here it seems for example that we have:
$$-\frac{1}{4} A (dx \wedge du)^2 = -\frac{1}{4} R_{xuxu}(dx \wedge du)^2$$
$$-\frac{1}{2}B(dx \wedge du) (dy \wedge du) = -\frac{1}{4}R_{xuyu}(dx \wedge du)(dy \wedge du)$$
The answer is supposed to be $R_{xuxu} = \frac{1}{2}A$ and $R_{xuyu}= \frac{1}{2} B$, however I don't quite understand how this would be obtained from the equation above. I assume it has something to do with the symmetries of the Riemann tensor but not quite sure.
snypehype
not being simply connected isnt a problem
not being connected is
the conditions you want are compact and connected I think
so the exponential map is surjective iff the group is connected and compact?
not iff
for example the exponential map R --> R_+^* is surjective
but the space of positive real numbers is not compact
okay, so it is true that if the group is compact and connected then the exponential map is surjective
but that's not the only case when it is
and there are tons of examples where the exponential map surjects onto a non simply connected thing
all compact connected complex lie groups
that's how you prove all compact connected complex lie groups are quotients of C^n by some lattice
the exponential map is surjective, with discrete kernel
do you by chance know a self contained reference where I can look this up?
so far all the books on compact lie groups I found are so advanced 
I think mumford's abelian varieties does it
but it depends on what you mean by self-contained
for someone who hasn't done proper math undergrad courses
I try to catch up by learning what I need in between
When we write S1× S1 as the torus, which component is the meridian? Is there a standard convention?
if two lie algebras have the same structure constants, they are isomorphic
is the converse true aswell?
is this an iff statement?
ττερρα
how can I see this?
ττερρα
first equality b/c phi is a lie alg homomorphism

gotta be careful when you say "structure constants of a lie algebra"
structure constants are always relative to a basis
why is $\dot A(0)$ in o(n)?
ProphetX
I thought tangent vectors to curves live in the tangent space, this lives in the tangent space at identity
it is true that the tangent space at identity is isomorphic to the lie algebra,but it's not strictly the same
the tangent vectors live in a different space,not in the lie algebra
what's your precise definition of "lie algebra of a lie group?"
some people define it to be the tangent at the identity
lie algebra of a group=set of left invariant vector fields
they are isomorphic
yes,isomorphic but not the same
right
so strictly speaking M above isn't an element of o(n), rather its image under the isomorphism is, right?
sure
it usually doesn't hurt to just pretend they're the same, but it's good to recognize there's two equivalent definitions
if $G$ is a lie group then the isomorphism between $T_eG$ and the space of left-invariant vector fields is given as follows: if $v \in T_eG$, then associate to $v$ the vector field $V$ defined by $V_g=d(L_g)_e(v)$, $g\in G$.
ττερρα
you're just using the left-multiplication to push tangent vectors at the identity around. this gives left-invariant vector fields, and conversely, every left-invariant vector field arises from this
Z_6 is compact right? ( the finite group)
then the product of SU(3)xSU(2)xU(1)xZ_6 is compact,right?
i.e. product of compcat groups is compact even if some are lie groups,some are discrete
wow this theorem seems to be powerful
I bet it's hard to prove 
oh this works for infinite products too

where is Tychonoff's theoem usually done? in point-set topology in undegrad?
is the proof for 'every finite group is compact' difficult aswell?
I am not sure how to relate the group elements to topology or how to put any topology on a finite group outside of the trivial ones
No, it is trivial. "Compact" means "every open cover has a finite subcover", basically finiteness of the group directly transfers to compactness
yes,but how can I 'put a cover' or 'put a topology' on a finite group?
if I have that,then sure,there always will be a finite subcover
it's probably with the discrete topology
Maybe it is not too hard to characterize all topologies on a finite set (maybe harder for a group requiring multiplicatjon/inverse to be continuous)
Actually maybe it is not so easy
But anyhow you can write down some topologies for finite sets. For finite groups, you can start with some sets that you say should be open, then close it under the usual topology operations and also under inverse image of group multiplication and group inverse
I can use the discrete topology and in that topology the statement will always work I thnk
is the product of a lie group with a finite group a lie group? 
i.e. is this a lie group?
product of lie groups should be another lie group with the group operations done componentwise
yes,but Z_6 is not a Lie group

is it? 
yeah i guess so
ok I will have to go through this proof 
It is very hard
Iirc every cw complex has the weak homotopy type of a finite space
I guess characterize doesn't mean classify
But my point is finite topologies can be complicated
This fact haunts my soul
is a finite group connected?
elated to yesterday's discussion I found the theoem @tight agate mentioned and I saw that connectedness is also a property required
so Z_6 is not connected? 
it is not
then i'm not sure why I could say that the exp map for SU(3)xSU(2)xU(1)xZ_6 is surjective 
any topological space with discrete topology is going to be totally disconnected
the image of the exp map is always going to be connected iirc
since a lie algebra is connected
and the map is continuous
its image will be the connected component of the group that contains the identity
it's going to be a normal subgroup H of G, and G/H can be any finite group
or even infinite if your lie group is not compact ? idk if that's allowed
so the fact that the image of the exp map is surjective doesn't follow from the torus theorem?
in order for the tous theorem to hold we need the group itself to be connected
but if we have z_6,which is not connected,then thist heoem does not hold
Wdym topological spaces over finite sets are completely given by their specialization preorder
Yeah, I realized I was getting at something different than what was being said
"topologies on finite sets can be complicated" in that "the homotopy theory of cw complexes can be pretty complicated"
Ah, so „homotopical characterization “ 🙃
yes
but if this theorem doesn't hold,how can I conclude that the exp is surjective for SU(3)xSU(2)xU(1)xZ_6
or is it not?
it is not
The reason would be that exp can only map into the connected component of the identity, right?
The image of exp will be connected, but it's not in general equal to the connected component of the identity; SL2(R) is connected, but exp(sl2(R)) is not all of SL2(R)
But yeah, it is definitely always contained in that connected component, so if your group is not connected (like here) then exp will not be surjective
If that above question is cleared up: What is happening here
In the calculation at the bottom of the screenshot: Okay, in the first equation we're using that the volume form is left-invariant, so we can pull an L_g^* out of nowhere. This doesn't necessarily agree with the next equation, though, where we're just pulling the L_g into the summand with the R_g
This is still fine -- we can just split up the R_g and the 1 before pulling out the L_g in one of the summands. Okay, cool. But then the next equation is totally lost
sorry, what's R_g - I?
R and L denote the right and left multiplication, so $L_g h = gh$ and $R_g h = hg$ for group elements g and h
Lartomato
Ah, I see, that might be another notational oddity: We want something like $R_g^* \text{vol} = \text{vol}$, so it should rather be $R_g^* \text{vol} - \text{vol}$
Lartomato
Ahh I see
But I guess they ""simplified"" that to a pullback of R_g - id which doesn't exist lmao
I guess I'm really just here to rant about how badly this is written
lol
My thinking is maybe they mean L_g^-1 instead of L_g
Then Ad showing up makes more sense
Yeah, that's probably true too
But then what's with the subtraction...
And then the last thing: I think if you had a volume form $\omega$, then $f^* \omega = \det Df \omega$ or something like that, which is probably roughly what we want here
Lartomato
Yeah I agree
I was thinking of something hazy like that
But then what's with the subtraction??
Maybe they just dropped a - vol_G(e) at the end?
Oh my god yeah
You don't need the subtraction at all, all you want is $R_g^* \text{vol} = \det(\text{Ad}(g)) \text{vol}$
l o l
Lartomato
How many mistakes can you get away with in a single calculation for a published paper
Incredible
Thank you! That helped
That is the most cursed notation I've seen in a while
So I just learned what a continuous function is in topology and it doesn't quite reach me intuitively. Why is the definition like it is, i.e $f: X \rightarrow Y$ is continuous if for each open subset $V$ och $Y$, the set $f^{-1}(V)$ is an open subset of $X$. It almost feels more natural to define it not in terms of $f^{-1}$ but in term of $f$ instead. Could someone just briefly give me an intuitive description of this?
older sister
try to translate f(xn) -> f(xà if xn -> x in metric topoly, you will see that this is the right definition
Maybe the epsilon delta definition is a bit easier to see
Yeah I searched that up and that makes sense
Or take for instance the 1st projection f : R² -> R² (x,y) ->(x,0), this is continuous since a tiny perturbation of x,y stay a tiny perturbation of (x,0) but the image of an open set isn't open
Yeah that's true
having the condition f(U) open is too restrictive dimension-wise imo
Okay but let's look at an example real quick, hold on
Okay so this one is discontinuous. Is it because if I take a open set/open interval on the Y-axis and "project" it down to the X-axis by the function, I will just have a singleton since there's an asymptote there?
Meaning that if I take a "big" enough open interval that lies high enough in the Y-axis and then do f^-1 on that I will just get a singleton, which in closed in R?
Well "big" enough is the wrong word, but I mean an open interval (a, b) where a is super big and b is also super big
Okay so why is it discontinuous then?
||this function is continuous on its domain||
Hol up, so why does the figure say that it's not?
can u give another picture
that image looks vague
Okay hold on
it'll be discontinuous as a function from R to R if you prescribe it an arbitrary value at a, but otherwise, it's a perfectly fine continuous function R\{a} -> R
Here's another one. So, using the definition, how can I see that this is discontinuous?
Agreed but didnt want older sister to be confused by what you meanr
If (f\left( x \right)) is not continuous at (x = a), then (f\left( x \right)) is said to be discontinuous at this point. Figures (1 – 4) show the graphs of four functions, two of which are continuous at (x =a) and two are not. Classification of Discontinuity Points All discontinuity points are divided into ... Read more
take inverse image of y(a)-1, y(a)+1
It's the same reason why it's intuitively discontinuous - there are points arbitrarily close to a on the left such that f(those points) aren't close to f(a)
Im not sure what your definition of continuity is
it is [a, a+something) which is not open
Is it using limits?
open sets
I am refering to the topological definition. I mentioned it above
Ohhh
Because there are no points less than a for which f(c) is near a
The asymptote example is continuous on its domain as @gritty widget wrote. It doesnt make sense to ask if it’s continuous on all of R becsuse it’s not defined on all of R
Yeah that's true
However, it’s a common convention in calculus classes to say it’s discontinuous
Even though that’s being a little handwavy with domain issues
yeah I see the problem. But I am starting to get it now, thank you so much!
And also, a homeomoprhism is basically just an isomophism we see in algebra right? Instead of operations being preserved, we now have an bijection between the open sets in the domain and in the image, right?
homeomorphism is
bijective+ continuous maping with continuous inverse mapping
And since open sets kind of tells us about how all points are connected, two spaces are homeomorphic if they can be "formed" into the other like the coffee cup and donut thing, right?
an open set is mapped to an open set and since this mapping is also bijective
it means ur just changing that names of the points. its literally means both spaces are same in a topological sense
Okay great, so it is equivalent to an isomorphism! Thank you so much!
Well two (for example) groups are isomorphic if they have the same algebraic structure. So I can "rename" all the elements in one group for it to become the other group, just like you described homeomorhpisms!
Yes!
Yeah, homeomorphisms are the isomorphisms of topological spaces @pearl holly
homemorphisms/diffeomorphisms are isomorphisms for some reason :<
This is the right notion to speak about "same" top spaces because it preserves pretty much any topological property you'd want to preserve if two spaces are the same
imagine a world where Top's isomorphisms would just be bijections 
So to show that two "geometric figures" are homeomorphic I want to work with manifolds and somehow come up with some homeomorphic function between those manifolds right?
You don't need to work with manifolds specifically - manifolds carry a lot more structure than topological spaces. You want to find a continuous function with a continuous inverse.
Okay! Manifolds sounds interesting tho, do you know if Munkres talks about it? From the "contents" section it seems like he doesn't, but he might at least mention them in a later chapter
But your geometric structures as top spaces will end up being manifolds anyway 
yes munkres does talk bout manifolds
Okay great!
You could also take a look at Lee's book on topological manifolds
Yeah I am going to take a note of that book! Thank you so much!
Given a Lie group $G$ acting on its Lie algebra $\mathfrak{g}$ via the adjoint action $\text{Ad}_g$ for $g \in G$, the orbits are immersed submanifolds. In this nice situation, are they even embedded submanifolds?
Lartomato
uuuuh if you don't have that this stuff is semisimple, you can probably do freaky things with irrational tori somehow, so feel free to assume semisimplicity
i guess i just need to show that it's a proper action
It very much depends on what structure you're considering.
An algebraic topologist might say things like "the punctured plane is the same as a circle" bc they work up to homotopy equivalence
but this is nonsense to a differential geometer, a punctured plane is a 2-dimensional manifold (I think it's diffeomorphic to a band/cylinder actually) whereas a circle is a 1-dimensional manifold
and it's even nonsense to a general topologist, since if you remove any two points from a punctured plane you get something connected whereas if you remove any two points from a circle you get something disconnected
Okay I get kind of get that, but I still haven't learned what a homotopy is. I'll get there soon I hope! Thank you so much!
gaytopy
homotopy equivalence allows you to squish things more, so for example, a band/cylinder is homotopy equivalent to a circle becuase you can squish the band infinitely down along its axis
"Yeah I've spend decades researching in gaytopy"
@gritty widget did I get it right that a twice-punctured plane is diffeomorphic to a band. I'll be so proud of myself
ohhh okay!
(I have the mental picture)
Basically the picture is map it onto a twice-punctured sphere, then put a cylinder around the sphere to project to from the origin
maybe I should have specified an infinitely tall cylinder/band
boundary is fake lol
Okay that sounds really interesting, hope I'll learn that in depth soon! Thank you!
by any chance anyone has like a visual way to see that $\left(S^1\times S^1\right)\wedge S^1$ is homotopic equiv $S^2\vee S^2\vee S^3$
all i can figure so far is that since $S^1\vee S^1\subset S^1\times S^1$ is a cofibration we have some coexact sequence blahblah yoneda hence homotopic
ari 十年生死两茫茫,不思量,自难忘。
Remember, topologies are just glorified semi-lattices.
If you have two semi-lattices X and Y, and a monotone function f from X to Y then an element a of X is a sufficient factor for b in Y if for any refinement of X W, refinement of Y Z and monotone function f': W -> Z that extends f, for any element w of W, w subs a => f'(w) subs b. Likewise an element a of X is a necessary factor for b in Y if for any refinement of X W, refinement of Y Z and monotone function f': W -> Z that extends f, for any element w of W, w subs a <= f'(w) subs b. An element a of X is a determining factor for b in Y if it is a necessary and sufficient factor. The map f is factorable if every element of Y has a determining factor in X. This means that there exists a function f*: Y -> X.
What it means in topology for a map F: X to Y to be continuous is that the induced map f = cl o image_F, from the closed sets of X to the closed sets of Y is a factorable map.
I'll read that once I've become better at this, but thanks!
I mean if she has the patience to read through Munkres it's plainly appropriate
Learning topology from Munkres is like learning Quantum Mechanics from NewScientist, Munkres is basically popsci for nerds.
I don't know if that's good or bad lmao but Munkres is all I had to choose from. My teacher only has Munkres so he let me borrow it
Munkres is pretty good lol
Nikita and I had the exact same discussion last time older sister asked about how to study top 
Yeah I remember that


It's honestly hard to find any good book on topology. I want to learn more topology too, but the most of it is over my head.
sutherland is good and succint
Starts with metric spaces tho 
the portions are quite disjoint iirc, though I'm not sure why you wouldn't want to see anything about metric spaces first given the motivation for a topological space
You're right, that makes sense to me 
What the fuck
.pin
This is the worst post I've seen since I returned
Jesus christ
Learning topology from Munkres is like learning Quantum Mechanics from NewScientist, Munkres is basically popsci for nerds.
Remember, topologies are just glorified semi-lattices.
I want to learn more topology too, but the most of it is over my head.
You can't estimate my level of thinking if you don't know even elementary terminology, so this is just emotions.
Gee I fucking wonder why
Yoikes
lol
The internet has had disastrous consequences for mathematics
Return to pen and paper
no euler?
Rocks and hieroglyphs? 
how did people even live before $e^{i\theta}=cis(\theta)$
Kaisheng21
down with e^(iθ)
They've played us for absolute fools! 

lmfao
Amazing
That is the best one I've seen here personally, I couldn't stop laughing for a whole minute (like seriously, I'm still giggling
)
actually nevermind
That is funnier

Wait @fading vale have you seen the lattice thing yet?
lmfao
Perhaps if it is all over your head you should not be commenting on whether or not Munkres is rigorous or "serious math."

@fading vale ok popsci-nerd 
Lol nerd, must have sucked to be in that class
it did!
From Munkres, we have the following theorem:
\bigskip
\textbf{Theorem 82.1}.\quad Let $B$ be path connected, locally path connected, and semilocally simply connected. Let $b_0\in B$. Given a subgroup $H$ of $\pi_1(B,b_0)$, there exists a covering map $p\colon E\to B$ and a point $e_0\in p^{-1}(b_0)$ such that
\[p_*(\pi_1(E,e_0))=H.\]
\bigskip
Given the space $B=\bR P^2\times\bR P^2$, we have that $\pi_1(B,b_0)=\bZ/2\bZ\oplus\bZ/2\bZ$. Consider the subgroup $\{(0,0),(1,1)\}$ of $\pi_1(B,b_0)$. Find the covering space corresponding to this subgroup.
\bigskip
I have been trying to solve this problem for hours. Can anyone who's knowledgeable give me any pointers/hints? I'm completely stuck. I found covering spaces corresponding to every other subgroup of $\pi_1(B,b_0)$ besides this one.
Isaiah
Have you found the universal cover of the space?
Right
Is the idea to use some orbit space of S^2 x S^2?
yeah
follow the construction of the cover corresponding to any subgroup H
as a quotient of the universal cover
So my confusion there, like wouldn't any orbit space of S^2 x S^2 correspond to the trivial group since S^2 x S^2 is simply connected?
No, you look at the action of pi_1(B,b_0) on S^2 x S^2
Like for any group G, the map
q : S^2 x S^2 ---> (S^2 x S^2) / G
would induce the trivial homomorphism, namely,
q_*(pi1(S^2 x S^2)) = 0
yeah, but that only means that the range is the zero group
the codomain could be larger
Should I be looking to use this theorem?
Nope
The covering space that you want to construct
Since you would get that its fundamental group is the subgroup you quotient by
[\begin{tikzcd}
{S^2\times S^2} \
& {(S^2\times S^2)/(\pm\mathrm{id})} \
{\bR P^2\times\bR P^2} && {}
\arrow[from=1-1, to=3-1]
\arrow[from=1-1, to=2-2]
\arrow[from=2-2, to=3-1]
\end{tikzcd}]
Isaiah
Yes
awesome thank you so much!

Getting stuck here even after having gone through homology and cohomology twice before
in the proof of im \partial \subset ker i_*, how do we know that \partial b = 0?
For context, [c] is in H_n(c), b is a pre image of c under j, and a is a preimage of \partial b under i
oh nevermind this was very stupid
[\partial b] = 0 since it is a boundary 
i want a girlfriend that i can do a homology with before bed 
Seems like too big a restriction of the domain 
Maybe that’s why they call it homology

Why do they call it homology when Hom oligy
Suppose you have a metric like this
THen I want to find an orthonormal frame that is dual $dt + e^x dy$, $dx$ and $\frac{1}{2}e^{x} dy$
snypehype
Obviously $\frac{\partial}{\partial x}$ is dual to $dx$
snypehype
but I don't how get to compute the dual to $dt + e^x dy$
snypehype
Given a topology τ and a set S. We have τ=(smallest topology containing S as a subset).
Is there a name for an S with this property?
Eg a basis, an analytical basis, a whatever.
That might be the only name but i thought it had some other one. Ok, ty
Sub base IIRC
yeah I think that's a sub-basis 🤔
🤔
wait it's not clear. Is it S € tau or S \subset tau ?
Google is telling me a sub basis must cover your space, and if it doesn't cover your space, it is called a synthetic sub basis. This is wack tho, never used these terms before.
Synthetic sub-basis I've never heard of
Although the covering requirement makes sense
Although you can just add X
These are just the definitions from the one site I looked, lol. I've never used them so idk.
@empty grove I finally worked this out based on one of those MathSE posts. You don't need U compact but you do need neighbourhood.
Let c > 3; for example c = 5. Let V be a union of open balls covering E with volume < e/c^n.
For each x in E, choose a radius r > 0 around x st
(i) B(x,r) subset E (volume purposes)
(ii) B(x,cr) subset U (cover-inside-U purposes)
In fact, we can avoid Choice here (although needed later) by picking r maximal st
B(x,cr) subset interior(U) intersect V
as you did earlier.
Now use Vitali's Covering Lemma to take a countable subcollection of the above balls which is
(i) disjoint; thus total volume less than e/c^n as it is subset V
(ii) each ball dilated by c is inside U
Then the countable subcollection, each dilated by c, is within U with volume < e.
The same should work if E has non-zero measure, but the tight cover will have volume > 3^n the measure of E.
Hope there are no more mistakes 🤞.
And the definitions are equivalent because intersections distribute over unions. Therefore the finite intersection of a unions of finite interasections is a union of finite interasections.
Understandable. Have a nice day
since finite groups are 0 dimensional manifolds,are they also lie groups?
wikipedia says lie groups are groups that are differentiable manifolds
so finite groups are 0-dimensional Lie groups
if 0-dimensional manifolds are differentiable, sure
actually,how is R^0 formally defined? 
idk that much topology, so should not be talking
In (i), I think you want B(x,r) subset V instead of E. Also c probably has to be ≥5, because that's what you need in the infinite version of Vitali's lemma.
That thing in the last line is pretty nice, at least there's a finite constant you multiply by which feels intuitive if all balls are scaled up by upto a constant
Singleton
what does that mean?
1 point
1 point, and the topology is that all (2) subsets are open
What the element is doesn't matter
If we call it 1 or * or whatever the topology will still behave in exactly the same way
It's a single point, 0
But you can take it to be 0 if you want
so i can take any real number and that is R^0?
R^0={x} ,where x can be any real number?
Eh, depends on how much structure you want on your R^0
If it's a vector space then it should be 0, or you need to redefine addition and multiplication or whatever
Yeah if you're only looking at the topology, take it to be whatever (not necessarily even real)
if I want now to make this into a topological manifolds,I choose charts: {x}->R^0 for any x
R={R}
Yes
To answer your question you can give any set with the discrete topology the structure of a 0-dimensional manifold by taking the charts to map each point to R^0
how is smooth defined on R^0?
Reject regularity 
There are no overlaps phophetx
So the only thing you need to worry about is smoothness of the identity map
How so
my bad
how is smooth defined in this sense? I don't know how to define a partial derivative which should exist and be continuous
continuity is clear from the definition with open sets
you don't need to in this case
Proohetx, there's only ever one map
Everything is smooth lol
Yeah
you're smooth 
Hello legosi
yeah so any finite group is trivially a compact lie group

and it's instructive to think about this specialization, since the representation theory of finite groups generalizes to compact groups by defining the haar measure
i.e. {e}->{0},{g}->{0},{g^2}->{0}
and you give any finite set a measure by the counting measure
There's only one map R^0 -> R^0
So the transition functions will all be this one map
so there is just 1 chart?
Those are what you need to check are smooth for something to be a smooth manifold
No
There are |G| charts, you're correct
But smoothness of an atlas says that the overlap maps are smooth
right
We just declare it to be so
It's the identity map
Any reasonable definition of smooth would call it smooth
so smoothness is not to be understood in the sense of partial derivatives being continuous
it is, but this is kind of a relative sense
Well, you could actually define partial derivatives here
R^0 is a vector space
you can make sense of smoothness of maps V -> V intrinsically by taking limits
But whatever definition you work through it'll end up being smooth
There are no partial derivatives to check so it's vaccuously smooth 
okay,it makes sense now, thanks 
vector space over which field? can be any?
R
I abstain from clarifying whether R^0 = C^0
So one thing is like
Being a vector space or a manifold isn't a property you can have
It's structure
We have to add extra data
Like a smooth atlas, or a scalar multiplication
right,we need to define an addition and s multiplication to make it into a VS
but how can one add elements,if there's just 1 element? 
0 + 0 = 0
everything is 0 so we're good
Even an empty addition won't be a problem lol apart from losing existence of an additive identity
but now comes the strange point, if we say a chart is {x}->{0}
how is {x} still R^0?
we said R^0={0}
There is an empty semigroup, it's true
or R^0={0} and anything else {x} at the same time?
charts aren't equalities prophetx
Right, and here that anything has to be real because you're only defining scalar mult by reals.
a little circle on a sphere isn't the disk
Remember, definitions are upto isomorphism
That's why it's a real vector space
No
What?
Why do people keep mentioning 0 dim vector spaces being iso
That's not relevant here
They asked why these are charts on a manifold
For a discrete group
so my confusion is,we said we have |G| many charts {x}->{0}, therefore this is a map from R^{0} to R^{0} right?
The manifold has no linear structure
no
It's a map from a subset of G to R^0
Namely the subset {x}
But the transition maps are maps R^0 -> R^0
And smoothness of the atlas means that these are smooth
Well he asked wether R^{0} was every singleton, so I just mentioned that you could take any singleton as they would all be linearly isomorphic
and there's just 1 function because there's just 1 way to map 1 element to 1 element
right?
Yes, exactly
math shocks me everyday
this is very nice
I didn't find this in Lee's smooth mfds book
it was an exercise
He talks about 0 dim manifolds
no author wants to write about these things
Jack is careful
I've only caught him on the empty manifolds once (maybe twice?) across 3 books
if jack is so careful why did i spend so long on 3-10 in irm 
lol
You were not careful
fuck that exercise
Isn't it interesting...how the tteppa fails to consider?
I would simply assume as much as I needed to prove it
is it useful for anything to view finite groups as 0 dimensional manifolds?
Eh
you can make your statements say all natural n instead of n >= 1
Everything about 0 dim manifolds is ultimately not using the 0 dim manifold structure
But it can be useful
Like, you can say that the isometry group of a riemannian manifold has a lie group structure
how incredibly useful
Bourbaki style most general way possible
I heard memes about Bourbaki books being super abstract and most general
I think it is nice to not have to think too hard about corner cases
I have this game where I try to gotcha my friend with them (and him me)
It's a cold war so far
and nobody's had a victory
just a sanity check,SO(N) is compact and connected for any N right?
therefore I can obtain SO(N) by exponentiating so(n)?
I can certainly do this for SU(N), but i'm not sure about SO(N)
These are pretty nice lol
Sounds correct to me prophetx
Hm I'm not sure how you can easily show SO(n) is connected
1
Exactly one
You can gram schmidt to show SO(n) is homotopy eqv with the matrices of positive determinant and then find a path in that space, I think
But that's so ugly lol
is it similarly hard to show for SU(n)?
( I took it for granted
)
but for SO(n) i was not sure the statement is even true
I think it's easy for both
I just don't see it lol
God this is just a day for me to do linear algebra I guess
I was helping someone else in #groups-rings-fields earlier
define trace coordinate-free 
Since SO(n+1) acts transitively on S^n with stabilizers SO(n)
So to show SO(n+1) is connected it suffices that SO(n) and S^n are connected
SO(1) = {1} is obviously connected and spheres are connected
linear term of characteristic polynomial (or is it the x^{n-1} term? idr)
Derivative of the determinant at the identity


the trace is the trace.
ttracepa
Ah yeah I love this one
Maybe a really stupid question, is there a way of showing a Vector space is isomorphic to its dual without choosing a basis?
No, but I'm not sure how you could make this formal
Notably it fails in infinite dimensions
I think the question was about finite dimensional vector spaces for that reason
Right, I'm saying this might suggest you need to choose a basis
ooh
Yeah but i mean the question asked for a coordinate free description, that’s why I asked
that makes sense, if you could do it without reference to a basis then dimension wouldn't come into the picture
Well, is that necessarily true? I don’t even know how to properly ask the question in some sense
Wait this is so dumb
I don't know why that link is doing it like this
Being iso to your dual is a red herring
You need to pick a basis to show that the canonical map V (×) V^* -> Hom(V, V) is an isomorphism
then there's a map V (×) V^* -> k given by the bilinear evaluation map V × V^* -> k
idk why you would go through the dual of Hom(V, V)
I think you can't, and that's why we say that V and V* aren't canonically isomorphic while V and V** are ?
🤔
(oh I'm very active now
)
I don't really agree
Idk how you would set it up categorically
It's true that the variances are different, so maybe category theory tells us it'd be weird if they're iso
proving the existance of an isomorphism without reference to a basis is different from constructing a natural isomorphism though
the fact that V and V** are canonically (or more precisely naturally) isosomorphic is definitely something you can express in the categories language
but I may be missing your point shamrock
Sure, and the iso V (×) V^* -> Hom(V, V) is natural in this sense
You don't need to pick a basis to construct it like you do for the dual
yeah sry I was responding to shika blyat's thing
Yes, but what does that have to do with the informal statement "you need to pick a basis to show V and V^* are isomorphic"
No it's a good point, I think it highlights how the duality thing is just a red herring
So I guess I'm saying you have a single map Hom(V, V) <- V (×) V^* -> k
But to show the first map is invertible you need to pick a basis
Just like with the map V -> V**
Even though it's defined defined independent of a basis
What kind of information can you get more about a manifold by computing its compactly supported De Rham cohomology rather than the usual De Rham cohomology?
I don't really get the motivation that much
idk tbh, I was just thinking about the fact that there's some functor that makes V and V** naturally isomorphic but not V and V* because the functor is contravariant, but yeah now that you ask, I'm not sure how this would relate with the question, even though I've always assumed that both facts are related
so nvm me 


