#point-set-topology
1 messages · Page 177 of 1
i think one of the things tu means to get at here is that when you consider how tangent vectors act on (germs of) functions, you get a map T_p(R^n) x C_p^\infty(R^n) -> R. tangent vectors act on functions by fixing the first component, which you should be familiar with. however, if you fix a (germ of a ) function in the second component, you get a map that sends tangent vectors to real numbers. if you do this pointwise with a smooth function on R^n, you get the differential (a 1-form)
(this isn't in response to anything anyone said, just interjecting and giving my interpretation of the page of tu bacono linked)
takes vectors to the dir derivative of f
sorry wait I think I understand what's been fucking me up now
the notation just writes (df)|p which hides the reliance on choice of X_p
what is (df)|p defined as?
so I've been thinking the differential is invariant no matter what vector we choose in the tangent space
(df)_p isn't defined relative to a tangent vector X_p. (df)_p is defined as a covector, which takes a tangent vector X_p to the real number X_p(f)
OH
there's no reliance on tangent vectors in the definition of (df)_p
ok that's exactly what I needed
and when you do that pointwise, you get the 1-form df
its expecting a tangent vector in its argument for it cooom and give you a dir derivative
(the thing (df)_p is called a covector because it's an element of the dual space to T_pR^n)
ok that makes a lot more sense
don't worry tu is relatively light on the notation
except for the lie derivative section
oh god oh fuck
that's section 20 though so dw
this book seems really fun
I'm actually really enjoying it so far
I tried learning classical diff geo first and it was terrible but this is significantly more intuitive
it's a great book but i think the one major downside is that it doesn't cover a whole lot of stuff
always fun when they define concepts
not fun when they use them abusively and you have to recall
which could be seen as a plus as well, i guess
I used O'neil for diff geo
said elementary, but its more like between elementary and modern
I just think modern approaches work significantly better
theyre also significantly harder tbh
looking at it from a much more algebraic standpoint does wonders
old approaches were like
hey look at this arrow with a direction
new approaches were like
hey look at this derivation over smooth functions in a tangent space
well in do carmo he does fucking everything in 2 and 3 space
virtually every proof involves the fucking jacobian
the jacobian is a good tool in diff geo tho
it becomes the basis matrix for maps from Rn to Rm
tu is much more of a differential topology book than a differential geometry book
but that's me being pedantic
since do carmo does everything in R2 and R3 there is already a riemannian metric inner product
tu's introduction to manifolds doesn't even touch that kind of stuff
@pastel linden when you're going through the first 5 sections of tu, see how much of it uses the fact that Rn has a standard inner product
might be a fun thing to keep track of
given i'm on section 4 and he hasn't used it once I doubt it'll be non-zero
he mentions the cross product like once in the lie algebras section
apart from that you can forget all about those geometrical concepts from R3 and R2
gustavn64:
I am trying to understand the following construction, where $\sigma^i$ are the standard left-invariant one-forms on $S^3\cong\operatorname{SU}(2)$. As far as I can see, this really only gives a Riemannian metric on $(0,\infty)\times S^3$. How does one go from this to a metric on $TS^2$? My guess is that we are at least supposed to quotient the $S^3$-factor by $\mathbb{Z}_2$ (by identifying antipodal points) to obtain a metric on $(0,\infty)\times(S^3/\mathbb{Z}_2)=(0,\infty)\times\mathbb{R}P^3$, since $\mathbb{R}P^3$ is diffeomorphic to the unit tangent bundle of $S^3$. This gives a metric on $TS^2$ minus the zero section, but how do we show that this metric extends smoothly across the zero section?
gustavn64:
Let φ : G -> H be a lie group homomorphism with dim G = dim H and H connected. If Γ = ker φ is discrete, is φ surjective?
I'm thinking that φ descends to an injection G/Γ -> H which is constant rank since it's equivariant wrt the G action on each (note that G/Γ might not be a group) and thus is an immersion, but since dim G/Γ = dim G = dim H, this means it's also a local diffeomorphism. This means it's an open map, and so im φ is an open subgroup of H. Since H is a connected topological group, it has no open subgroups, and so φ is surjective
I guess this shows more, i.e. it shows that the induced map G/Γ -> H is a (G-equivariant) diffeomorphism
the above proof looks good to me
and i now feel justified to ask my own question: Consider the subspace $A := {(x,y,z) \in S^1 \times S^1 \times S^1 : x = y \text{ or } x = z \text{ or } y = z } \subset S^1 \times S^1 \times S^1$. Is there any smart way to approach calculating its singular homology?
Lartomato:
oh right this is the fat diagonal of the space, maybe that helps
Maybe you can write this as an union of equalizers. But idk if homology is preserved here
actually, i believe this was a silly question to ask
What I'm more interested in is relative homology of the pair $(S^1)^3, A$. That may be actually a bit simpler, since you can use that relative homology is (in this case) equal to reduced homology of the quotient space. But I'm not sure what to do with the quotient space
Lartomato:
nvm i posted it on stackexchange instead
Yeah maybe S1^3/A is a simple spacea
I'd expect it to be something like S^3 times S^2; cause that's what the author in the book I'm reading sort of alludes to...
anyone wanna tackle a hyperbolic geometry problem
Is axiomatic geometry permissable?
?
Foundations of geometry is the study of geometries as axiomatic systems. There are several sets of axioms which give rise to Euclidean geometry or to non-Euclidean geometries. These are fundamental to the study and of historical importance, but there are a great many modern ge...
or is that stuff better placed in foundations?
...
We used a book at my college that taught Euclidean geometry like this. I wanted to go back and give it a shot but I didn't know if I had questions where could I post them.
You kindof just start out with a set of axioms and prove as much as you can with it. So we would start with some undefined terms and a set of axioms like what it means for lines to be collinear and stuff and then once we could prove everything we could with those axioms, we added another.
It's very formal so I didn't really know where it should be. In here or foundations.
@marsh forge No questions atm pertaining to actual math. Just where to post.
@uncut surge could you use excision?
To compute the singular homology of A
We can cover it by A1 = { (x, y, z) in A : x = y } and A2 = { (x, y, z) in A : x = z } and A3 = { (x, y, z) in A : y = z }. Fatten those up a little so their interiors cover A. Then the homology of A relative to A1 is the same as the homology of (A2 union A3) relative to (A1 intersect (A2 union A3)) = { (x, y, z) : x = y = z }
No this is too messy
following a good conversation with mathemagician a few days back i proved some stuff and feel like i have a good grasp on what the image of a morphism phi:F->G of sheaves is. essentially the elements of im(phi)(U) are elements s of G(U) with the property that for some cover {V_i} of U we have that s restricted to V_i is in im(phi(V_i)). so to me this is sort of like enlarging im(phi(U)) in the smallest way possible which allows gluing to work
anyways i'm feeling really good about images now and i'm moving on to quotients of sheaves. i'm looking for some other intuition about what they look like. hartshorne defines the quotient F/G to be the sheaf associated to the presheaf U -> F(U)/G(U). with enough effort i could write out what the elements of (F/G)(U) look like, but i'm wondering if there's a more intuitive description of F/G, similar to the above scenario with the image sheaf
i imagine it's a similar process in that you want to add in the minimal amount of stuff which makes gluing in F/G work, but this time there isn't a larger object from which to pull from like in he image presehaf case
I honestly just think about it in terms of that
I feel like I kinda have a feeling for what a sheafification looks like so in my head it’s just the sheafifcatuin of that presheaf haha
So I'm trying to understand a gauge map transformations wrt a Ehressman one form. I know the first term represents local changes in the one form (vertical projection of tangent base vector via lift) but what does the second term mean? How does the Maurer Cartan form act on a vector within the base manifold? My gut tells me it has to do with how the gauge map transforms the base space (but again how does a group element act on a base manifold not the total principle bundle) and it is the lie algebra equivalent of that transformation wrt a direction. So both terms together would be the change in the lie group due to moving within the base space and the change in lie group due to the gauge map transformation.
tolaria:
@meager python at a glance it seems that you need to show that p^{-1}(V) is preserved by the action?
But it feels like it's in different order than I want even
sup
Yeah that's the counterexample I know
About path connectedness does not imply locally path connected
ah weird
I thought local properties were made to be more general
well yes
wait
why is that space lpc?
ah
why is it not lpc
does 0,0 have some weirdness
that looks surprisingly similar to the counter example of pc<=>c
can you walk me through why no nb of 0 is pc?
cant immediatelly see
cant I just take nbs which vertically involve the wave
oh
is it
I thought the standard counterexample for one of these is hawaiian earring
ah right
looks homeomorphic to it
but why not lpc?
oh
oh truee
wait
maybe not so true
if you think about it(0,1) is hom to R
so thats not nec so intuitive
ah, but [0,1] compact
wait
oh ye, makes sense
if only there was some lindelof equiv of pc
(there may be)
fking lpc tho
not v pretty of you
I thought of any path
but maybe compact path may be a better way to think
wait so
well ye
the like
I just meant intuitive path
like going from one point to another
let me get my proof back from where I showed this isn't path connected
Without the loop around
I think that's the same proof for it not begin lpc right?
Yeah
is it compact
not sure
is it bounded
totally bounded
but thats not the space
otherwise itd be lpc
same
2am 
closed hausdorff are
but like
uhmm
lemme think
this is weird to think about
it should be compact
but I think the problem is the pseudopath not being
so where is the intuition mistake
for some reason I feel like not using subspace top here
Okay so I'm just gonna show that the set is the sinusoidal thingy
and the line (0,y) where -1 <= y <= 1
yes
well trivially
compact are always closed and bounded
isnt heine borel that compacts are equiv to that in Rn?
ye
but I meant that always is the case
compact is always closed and bounded
even if the rec is not always true
there is something about it being a line there
So suppose you could draw a path between (2,0) and like (0,0) so f(0) = (2,0) and f(1) = (0,0)
then f(t) has to assume all x-values between 2 and 0
as you increase x from 0 to 1
Then this says that you can get t_k such that f(t_k) = (1/2k,0) for all k
and t_k are increasing
pass to a convergent subsequence of the t_k
wait wait wait
why cant I just take the nb to be the whole set?
feels diff than usual local defs
then any smaller one still won't let you
you'd have to make the path through the sinusoidal stuff
But by passing to a convergent subsequence we can assume that t_k convegres to t_0
so that f(t_k) couldn't converge
also
The hawaiian earring is an easier example for pc but not lpc I think
like local compactness
weaker than compactness
It's pc cuz you can go from any loop to the origin
then out on any other path to any other point
but if you draw a circle away from the point all the circles meet
you can't get from one loop to another
No?
Here's a shitty drawing of it
take the open set to be the red circle
intersect it
you can't get from the inner loop to the outer one
??
Oh I think so
you're right
shrink more
lmao
wait
is it locally path connected
but not connected was it?
then...
maybe pc and not c
Although {\displaystyle \mathbb {H} }\mathbb {H} is locally homeomorphic to {\displaystyle \mathbb {R} }\mathbb {R} at all non-origin points, {\displaystyle \mathbb {H} }\mathbb {H} is not semi-locally simply connected at {\displaystyle (0,0)}(0,0).
Im just now realizing that
local compactness, locally hausdorff and locally homeomorphic are completely diff than those connected ones
all of those are implied from their non local counterparts
but connectedness had to be special

This is because connectedness isn't a local condition I think
isnt comp l comp, l comp paracomp and paracomp metacomp
Like I have strong reasons to say this
well
compactness also isnt
but Ig youre right
the motivation for classifying local compactness makes sense
same with local homeomorphisms
and local hausdorffism
wer that means
yeah, you can also be sigma compact and want to be loc compact
like reals
heine borel may be closely related to this
total boundness being equiv to boundness may be similar to the space being locally compact
A universal cover is just like an initial cover in some category of covering spaces, right?
up to unique isomorphism I'm sure 🙂
I think it's unique if you take into consideration the "other data"
namely the projection map
at least, that's usually how categorical constructions work
Lol
I never got that far into topology. All I know is that the circle's universal cover is the line.
and that the covering spaces are just n-fold spinny-wiggle maps
oh neat
Z acts properly discontinuously on R by \phi_n(x) =x+n. Quotienting by this action gives S^1, and shows that \pi_1(S^1) = Z
That's a nice way to think about the relationship between R, Z and S^1
There's a nice story re a space being the quotient of it's universal cover under the action of the deck transformation group
Lol
(Why is there just one overloaded Wiki page for coverings? 😦 )
@gritty widget are these linear transformations from the same degree vector spaces?
If so surjective is the same as injective same as bijective
Is this like smooth manifolds stuff?
ISM?
Oh lol you said that
Well
@sleek thicket
You like smooth manifolds
what
The functionals are the rows of the matrix dg_x, right?
The row rank of a matrix equals the column rank
So the image (= column space) has to be l-dimensional
And thus dg_x has to be surjective
@gritty widget
when I say "rows" and "matrix" I'm saying to choose an arbitrary basis, you don't really need to. I'm sure there's a direct abstract linear algebra way to see this
but yeah this is just the fact that if you have an n×m matrix with m > n and with linearly independent rows the associated linear map is surjective
The term is fullrank
yee
Haha no worries, I didn't really learn linear algebra until I took a course on smooth manifolds
Am I being brainlet? I wanted to show that the composition of quasi-compact morphisms is quasi-compact, but I think you only need one of the morphisms to be quasi-compact lmfao
I am brainlet
thank you for coming to my ted Talk
lmfao
I can't just cover the pullback of an affine by quasi-compact sets, I need to know the pullback is quasi-compact
but if you assume both are you can cover the pullback by finitely many sets which are quasi-compact which means...
😉
we're all varying levels of brainlet
hm it looks like i am just the tiniest bit stuck
this exercise from rotman
so obviously what's being hinted at is that i should construct a function $\varphi: I^2 \to I^2$ such that $\varphi(s,t) = (s,t)$ corresponds to $f(s) = g(t)$ (and derive the existence of a fixed point of $\varphi$ from BFPT, which is theorem 0.3 here)... but i'm a bit lost on how to do that exactly
Ann:
i've tried phi(s,t) = (f(s)+g(t))/2 as the first thing that popped into my mind but beyond this im a bit out of ideas lol
ping me if anyof yall have like. hints or whatever
maybe umm ... ||phi(s,t) = ((1,1)+f(s)-g(t))/2|| could work?
||then the range is definitely in I × I and also phi(0,0) = (1/2+, 1/2-) and phi(1,1) = (1/2-, 1/2+) [where k+ means larger than or equal to k, and the same for k-] so the fixed point(?) can be phi(s,t) = (1/2, 1/2) cause only when f(s) = g(t) we can have phi(s,t) = (1/2, 1/2) .. i dont know how this works but um yeah||
sorry if its not helpful

that is a great idea
but the problem is the point would have to be (1/2,1/2)
we can guarantee a fixed point exists
not which it is
I though of the same with (s,t) initially instead of (1,1)
not sure if it is on range tho
and Id need to use the info of the points in g and f
with I=[0, 1], you can maybe try φ(s, t) defined by
|| φ(s, t) = exp(-||f(s)-g(t)||)(s, t)||
ooh wait so fixed point means somewhere where f(P) = P?
yes
exactly
there is somewhere I need to use the f and g being in those points hypothesis
meaning Im almost sure a,b,c and d will be somewhere
I tried normalizing f and g
but nothig came out
so something like defining
p = (f -(a,0))/(b-a) and q = (g-(0,c))/(c-d)
now p and q go from (0,0) to (1,1)
I dunno what to do with those ideas tho
@fervent citrus yeah I = [0,1]
actually hm. that works 
or does it? 
i think you run into some problems if phi only has (0,0) as fixed point
ah shit
wait @west spindle is I said to be [0,1]?
yeah
thats why it didnt look like an intersection would nec happen at first. I dum
huum a can equal b, no ?
ye
Is that continuous tho
Is the image IxI?
wha
Well for brouwer to work you need the codomain and domain to be the same
now it is
it still has the same issue of potentially having (0,0) as the only fixed point
ah
only continuous
yeah
I had a question about subsheafs
Let F be a sheaf and f_UV be the family of maps
Then F' is a subsheaf if F'(U) \in F(U) and f'_UV is the restriction of f_UV
Say we are given some U, V open sets such that V \in U. Then how do we know that f'_UV(U) will be contained in F'(V)?
not sure what all the notation is , but I think there's a function $\eta_U$ for each open set U
lorenzo:
(is this Peter May's book?)
ya
His hypersquiggle categories are just an immediate identifier
at first i thought hypersquiggle was a technical term
like, hypersquiggle cohomology
what are those maps though
Lemme pull up Concise and find out
sorry thanks
Oh so, it's like
Given eta
You're trying to verify Pi(X) is the colimit of a diagram, so it's like, alright for each eta build eta squiggly
Say we are given some U, V open sets such that V \in U. Then how do we know that f'_UV(U) will be contained in F'(V)?
@coral pawn This follows fromt he line above
Oh wait
no you also require that
F' need to be a sheaf
oh I see lmao sorry this is confusing
Lol it's all good, the wording threw me off too
someone should write a 'non-concise guide to peter mays concise AT'
I've entertained for some time the possibility of writing an algebraic topology book that's pretty formal and covers a lot, a la Concise, but is longer
Except that book kinda already exists as I've found out
"Algebraic Topology" by Tammo tom Dieck
(Fwiw I don't know the subject myself, the idea was that I'd be writing it as I learn)
(So basically texing lecture notes but without lectures)
writing a book is (ive heard) a terribly time consuming project
like, even writing a paper is terribly time consuming even when you have all the ideas down
so the general advice to grad students is to not write books ( tho some people try and are somehow successful)
i personally like the idea of learning through writing and teaching
generally feels more motivated to me
uhhhgg I forgot that a morphism of diagrams is a natural transformation
yeah isnt that cool 🙂
Yeah I definitely see that if the act of writing something isn't otherwise doing something for you (e.g. lecture notes) then I'd prob be worried to do so pre-tenure
yeah. but honestly maybe for some people it can be a source of energy, not a drain, idk.
personally I find writing math really hard, but maybe being in the practice of writing a lot bc of lecture notes would help
That's prob a good point
Anyway yeah I would recommend checking out tom Dieck lorenzo
I think once I decide to learn algebraic topology "for real this time" it'll be through either that or Bredon's Topology and Geometry
Much more detail than Concise and much more formal than Hatcher
I ended up using Hatcher mostly
Also ninespam in case you get stonewalled in Concise, TD is worth looking into
and supplementing
with lecture notes and stuff
there are some really good lecture notes on bundles and homotopy / BG kind of stuff
yea ok I have a feeling that’s going to happen sooner then later
Oh Behrens
I applied to Notre Dame and was considering him as a possible advisor
Though prob preferred Andy Putman
notes are by mitchell though
this is also a good supplement: https://math.berkeley.edu/~hutching/teach/215b-2011/cup.pdf
people always talk about how cup products are dual to intersections , but this was the only place that I saw it written down in a way that I was able to digest
Ooh I should read this for sure
Yeah same I know what's supposed to happen but not the proofs
I am dumb too
Yes
😦
hey why does chmonkey get to be called dumb and not me 😦
I don't want to claim things I can't back up
fair enough
this exercise from rotman
@west spindle
how about restrict the domain to [a,1] for some a , since there clearly exists a interval [0,a] on which f(s)≠g(t) by their construction
that will resolve the (0,0) being the only fixed point problem
And instead construct phi : [a,1]^2→[a,1]^2
i don't doubt the validity of this fix
it's the inelegance that i'm unhappy about
(also why are you writing your interval boundaries backwards lmao)
it happens to all of us lmao
Also this lol
I think I agree
after algebra it's the most active I think
So I think I'm almost done with II.3.20 a) of Hartshorne, the problem is to assume that X is an integral scheme of finite type over a field k. Then to prove that for any closed point $P \in X$ that dim $X = \text{dim }\mathcal{O}_P$
Chmonkey:
So we can cover $X$ with finitely generated $k$-algebras, and then it follows that $P$ is a maximal ideal in whatever Spec, then for finitely generated $k$-algebras we know that ht $P +$ coht $P = \text{dim }A = \text{dim Spec }A$
Chmonkey:
Vakil says that you can show that a scheme has dimension n if and only if it admits
an open cover by affine open subsets of dimension at most n, where equality is
achieved for some affine open subset. Hint: You may find it helpful, here and later,
to show the following. For any topological space X and open subset U ⊂ X, there is
a bijection between irreducible closed subsets of U, and irreducible closed subsets
of X that meet U.
I believe this, this at least says that some Spec $A$ has dimension equal to the dimension of $X$ itself, the problem I'm having is to show that the dimension of all Specs in that cover are equal
Chmonkey:
Essentially this says that if $X$ is an integral scheme of finite type over a field that every open affine has the same dimension, now if there is a closed point in the intersection of any two open affines then I can use that closed point to get an equality of the dimensions of those two affines, but I don't see how that's possible? I thought I could look at the generic point but it actually doesn't give me equality of the dimensions I think
Chmonkey:
hey ppl i'm getting introduced to topology since last week, and i've got one question
is the notion of continuous functions between metric spaces the same as a continuous function definition in calculus and the ones in numerical analysis (c0, c1, cn continuity) or more general, or more loose?
or totally different?
from what i could gather, it's the same thing as c0
It is more general. A continuous function on a metric space is, of course, something you can place on any metric space.
Whereas in calculus, you're only looking at continuous functions on R or Rⁿ
Yes, if your metric space is Rⁿ, then the two concepts are the same.
so that would also apply to spaces that are subsets of Rn, or manifolds, or things like projective space?
that's where the difference lies?
just throwing some examples
hello! I have a question, I am missing something, but idk what. somehow it seems to me that every two vector fields commute if you expand them in charts
where do I miss the point?
if you say there are two vector fields X,Y and you take their commutator [X,Y] and expand them in a chart U(x) they will look like $[X^a \frac{\partial}{\partial X^a}, Y^b \frac{\partial}{\partial X^b}]$
ProphetX:
you can take out the component functions I think cause they are just functions and you remain with the two 'partial derivatives' which actually commute because of schwartz's rule
however it is not intuitive, that if X,Y do not commute, in a chart why would they commute..
i'm asking this question regarding Riemann tensor-and deriving its components
Riemann tensor field is defined as follows:
if you want to compute the components it turns out that the last term will vanish.. but if it vanishes then it should vanish for any arbitrary vector field WHEN YOU GO IN CHARTS
however this is not intuitive
what am I missing?
or is it true that every 2 vector fields commute locally, but not necessarely globally too?
When proving surjectivity, how do we know that such s_i exist?
This is just
By definition of surjectivity on stalks
If you have a t in G(U), then t_x is in the stalk, so there has to exist some element of the stalk which maps to it
That’s saying some <s_i,U_i> such that it maps to t_x, so after restricting to the intersection this just says s_i maps to t|_{U_i}
uhhh
Do you know what the maps of stalks look like?
ivory hasn't been introduced yet
Whoops
Map of stalks is a map on the direct limits right?
Yes but there’s an explicit formula for it
In terms of the <s,U>
Definition of elements
If you give me a few minutes I can type it all out
But rn I’m on phone so
Yeah no hurry
Okay so, I will not show why everything is well-defined, you can do so if you wish
but first of all elements of $F_x$ are equivalence classes $<s,U>$ where $s \in F(U)$ and $<s,U> = <t,V>$ if and only if there exists some $W\subseteq U\cap V$ such that $s|{W} = t|{W}$, this is a bit different from what I said before cuz I forgot you need to include $W$
(Here all sets are open sets, and contain $x$
You have a group operation on this, via $<s,U>\cdot<t,V> = <s|{U\cap V}\cdot t|{U\cap V},U\cap V>$
Chmonkey:
Now for each open set $U$ containing $x$, you have a map $F(U)\to F_X$ given by mapping $s$ to $<s,U>$
Chmonkey:
Now, given a map of sheaves $\varphi:F\to G$, we get a map $\varphi_x:F_x\to G_x$ by the formula
Chmonkey:
$\varphi_x(<s,U>) = <\varphi(U)(s), U>$
Chmonkey:
Try to show this is well-defined
but this makes a commutative square with the maps $F(U)\to F_x$ and $G(U)\to G_x$ and with $\varphi$ itself
Chmonkey:
So now suppose you have surjectivity of stalks
given a $t \in G(U)$, we have $t_x = <t,U>$ in $G_X$
Chmonkey:
we then have some element of a stalk, which is something like $<s,V> \in F_x$ such that $\varphi_x(<s,V>) = <\varphi(V)(s), V> = <t,U>$
Chmonkey:
that last equality tells us that for some $W\subseteq V\cap U$, that $\varphi(V)(s)|_{W} = \varphi(W)(s|_W) = t|_W$
Chmonkey:
so let this $W = U_x$, and let $s_i = s|_W$
Chmonkey:
I think I kinda get what you're trying to say
I was using the universal property definition of the direct limit so I'll try and translate this into that
Yeah I mean
there's a time and place for both
100%
But from the universal property you can get it too
I tended to use the universal property in the exercises
but I remember specifically in showing that f_* and f^{-1} are adjoint
I ended up doing an element wise sort of construction
right at the end
since f^{-1}F is defined pretty similarly to the stalk
just you go with a colimit of open sets containing some set, not just a point
This definition confuses me a bit. Why is f# a function into fO_X but f#_x is a function into O_X,x and not fO_X,x?
should i do all the category theory exercises in rotman chapter 0?
i have like... a passing knowledge on the very basics of cat theory
It covers everything it needs in exposition. But the exercises aren't too involved so tbh it's fine if you just glance at it and say
Okay I could definitely write the details down
thats what i did
i just don't know if i should expend my energy (which is a rather scarce resource at the moment) actually writing down the details
Probably not in that case. Having gone through them there's not much to it
Are you asking specifically about these notes, or just how to read mathematical writing in general? @willow spear
@gritty widget both
@gritty widget Any good texts for analysis?
ok ic
how long would it take to go through an analysis book
yeah
Im mainly reading topology as a background for a reserach project
with a professor
no clue lol....i'm interested in pure math and im goign to be contact professors soon to see if i can do something relatated to topology
ok
yeah
so there are two types of analysis right?
real and complex
Yeah eventually my goal si to read through algebraic topology
oh ok
ok cool
yeah so im goign to do some analysis reading then for now
yeah true
so this the track then:
real analysis
point set topology
algebraic topology
no lol im in HS
rising junior
yeah thats what i was thinking too
ive done linear algebra
oh
no actually i learned as part of a AI/ML program
so defintely not proof priented
yeah also....you said a consice book for point set topology
any suggestions
oh lol
alright cool
also is topology a doable field to do research in
are other areas better
yeah fs
true
makes sense
so the recap
rudin would be fine then right for analysis
ok thanks...welll then ive got get to analysis grinding
thanks a lot for your help
yeah caus ei was reading through it and some of the stuff amde sense
its just the notation and stuff that trips me up
^word
oh ic
yeah hopefully
ok
Napkin by Evan Chen is quite interesting
yea im currently doing it now, and i like it a lot
yea that is the plan
as long as it doesnt get too complex but i think it should be ok
wait should i read Napkin...is it a good start
i mena the oarts related to topology lol
i like it as it is mostly goes over the important and interesting parts
not too thorough
ok will check out.....are there any other good youtube video for PS topology and beyond
ok np
how can one define rotations on manifolds coordinate free?
does anyone have a good resource on this?
search for manifold isometries, probably
Let $X$ be a topological space, then call $X$ irreducible if whenever $X = Y\cup Z$ can be written as the union of two closed subsets, then either $Y = X$ or $Z = X$. Now suppose that $X$ is a topological space, $U\subseteq X$ an open set, and $V\subseteq U$ an irreducible closed subset of $U$. Show that there exists some irreducible closed subset $Z\subseteq X$ such that $V = Z\cap U$
Chmonkey:
Essentially I want to show that I can extend $V$ to a set which is irreducible and closed in $X$, not just $U$, but I'm not sure how I can go about this. I know I can embed it into some irreducible closed set, but I don't see how I can do this
Chmonkey:
Is your problem statement correct? Otherwise what prevents$ Z = V$ so that $Z \cap U = V \cap U = V$
Lunasong:
Ah, can't read :(
No worries
I had a solution, but now I think it doesn't work unless I have some brilliant fix
Idea, let $V\subseteq U$ be an irreducible closed subset, then let $Z\subseteq X$ be minimal among closed sets such that $Z\cap U = V$ (this is the issue, why does $Z$ exist?). Suppose that $Z$ weren't irreducible, then $Z = Z_1\cup Z_2$ for proper subsets, but then $V = (Z_1\cap V)\cup (Z_2\cap V)$, since $V$ is irreducible this implies that $Z_1$ or $Z_2$ contains $V$, WLOG $Z_1$ does, but this contradicts $Z$'s minimality.
Chmonkey:
So can we show there must exist a minimal such $Z$?
Chmonkey:
Isn't it always the case that if V is closed in U then V = U int Z for a closed set Z in X?
Oh, I see
What stops there just being an infinite chain down?
Oh wait,
I can just take the intersection of an entire chain I guess?
I can do Zorn's lemma I think
Yeah
Yay
the minimal closed set would be taking the closure of V relative to X, right?
thats the def of closure
I already know that the closure of V is irreducible in X
..............
Lol
This is like a fact I have seen proven before
☠️
Bruh moment
Lmao
You know what this isn't even the worst, I spent like 3-4 hours stuck on a problem over two days, and I knew if I can show that the intersection of two open affine sets has a closed point, that I would be done
After struggling wondering "how can I show that's true" I emailed my professor and he told me to prove that the set of closed points are dense given my conditions, so that I don't just have 1, I have a dense set of them
Then I realized the last problem I proved was showing that the closed points are dense...
Does anyone have mumfords abelian varieties in pdf form?
@meager python I don't, but I checked and it's on libgen
Can’t find a download link there 😦
@meager python Can you send documents on discord? If yes, I'll download it and dm to you
I think so, yes. Would appreciate it
Okay np
What's a simple way of computing the homology of $(S^2\times S^1)/\sim$, where $(x,y)\sim(-x,-y)$?
gustavn64:
@dusk heron can we say that the given space is homeomorphic to RP2 x RP1?
Nah that's probably not even true
why is the metric defined on a smooth manifold different from the one on a set?
one can make a set a manifold, do the tangent space,bundle structures and then talk about the metric
why is the thus defined metric different from the one defined on a set?
it should be just merely a special case of that
but on a set we define the metric as follows:
and on a smooth manifold, we define the metric as follows:
well its defined on the manifold
and the manifold is a special structure of a set
is this not a riemannian metric?
im not sure,he defines it as just a metric
if it's a riemannian metric / related to a riemannian metric then it's just abuse of terminology i guess
later on he says riemannian metric is just where the sign is +++++
so they have nothing to do a-priori with each other?
the thus defined g should be a special case of the metric on a set
semi-related is that a riemannian metric gives you a "topological metric"
hmm yes this makes sense
but my brain somehow cant take it that we could take a bare set,equip it with a metric
or we could add more structure and just then equip it with a metric
why are these 2 not related?
it makes no sense to me
not really
i just studied this
but yes you ae right,you measure on tangent spaces
but that induces a notion of length of a curve on the manifold
first you have tangent space-velocities(as vectors), inducing metric you get speed, and integrating speed you get length
yes,at each point of each tangent field
so its an inner product field
a smooth inner product field basically
isn't every smooth manifold riemann-metric compatible?
i thought it is
like you can establish a riemann metric on any smooth mfd
ye,makes sense
aren't all second-countable manifolds metrizable by urysohn
true
i think so ultraproduct
regularity is local (or can be stated as a local thing) so you just say "locally euclidean" to finish the proof lol
(not really, but i think that you can do it this way without using any fancy topology theorems)
depends on their definition of a manifold i guess
hausdorff lets you have things like flows of vector fields
i was assuming that "manifold" meant "second countable hausdorff locally euclidean space" so there mightve been some confusion there ultraproduct
mb
prophetx's definition of a manifold (i checked the notes they are reading) does not include hausdorffness it seems
just locally euclidean
I apologize if this is inappropriate to share our own work like this, but reading the conversation about the inclusion of the Hausdorff condition in the definition of a manifold made me want to share this paragraph I wrote as a part of a document describing/motivating each component of the definition of a smooth manifold.
I don't pretend to be very knowledgable about these things, but this kind of summarizes what I found when I was looking into the same question
nice text
ok so I got an answer:it is different,because if you want to impose a metric as tensor field, you have to make each fibre of the tangent bundle( the tangent spaces) into metric spaces. they rae just vector spaces. if you impose a metric on each of the tangent spaces and require it to be invariant under change of charts you will get the tensor-field point of view
so the tensor-field point of view is more than simply a metric on a space
that's why they do not coincide
however constructing the tensor field structure you need to use the classic metric defintion on each tangent space
assume this is in R^2. how can U be open to A but not to the metric space R^2?
i'm reading POMA and it's not clicking for me; remark 2.29 is just totally not doing it for me
I'm guessing the dark green boundary is contained by A
baby rudin
Ah good okay
open -> there is a minimum upper bound r on d(p, q) for any p, q in the open set such that d(p, q) < r
this is where he is doing so
i'm struggling with it
Rudin says that a set is open if every point in it is interior
And says that a point is interior if there's a neighborhood of the point contained in the set
indeed
was trying to find that again, i'm picking up where i got stuck yesterday
i'll stare at this for a while and see if i can get it to click
mmh, that's what my friend was saying
is the idea here that, say, for example, i can take a half ball and go to the "closed" (better word needed) boundary somewhere near the arc and say like
Rudin is terse haha
there's no like
max distance i can go away from this point on the boundary
and still be in the half ball
because all points aren't interior
but then, isn't U just the same relative to A?
ah i see
balls around points in U which are not interior points do not contain anything in A that isnt in U
so that's what's being looked at
We care about the metric space that A creates now. Some point on the boundary is still interior, because all points that are a "distance" r away are in A.
I say "distance" because "distance" in A is different from "distance" in R²
why is distance in A not like distance in R^2?
ah yes
well
actually i think it should be
If I looked at a neighborhood on A's boundary, with reference to R², the neighborhood would leave A.
Instead, with reference to A itself, the neighborhood can't leave as that doesn't make sense
neighborhoods around points in the boundary of the closure of U do not contain anything in A that isn't in U
wait
there's a lot of stuff going on at once in this construction and it's hard to really pinpoint one specific thing to focus on
OH
YES!
that's what i needed to hear
thank you
i notice that a lot of the proofs in rudin use notions of n-balls and k-cells and whatnot; in point-set topology it seems like a lot of the time illustrations will use these really uniform set shapes and it makes me wonder: do i lose anything in doing this to visualize and work through proofs? doesn't this, working with open/closed disks and rectangles and connected regions of the real line lead to some failure to deduce some property about non-connected, not-simple sets?
is that something that will be addressed later on once i've covered the simple topics like compactness and connectedness?
can i safely use these visualizations to "cement" my intuition for these ideas, or do i need to think about sets which are not connected when i read over these basic concepts
and then later on, when we deal with disconnected sets, be able to apply that intuition from before to successfully understand what's going on
or do i need to fully memorize the theorems and corollaries symbolically in order to generalize to such cases?
i suppose not; i should just read, read, read and not fret too much about oddities until i come across one
I don't know if the answer to your question can be a calming yes, but what I have to point out is that the all-important Zariski-topology in algebraic geometry is non-Hausdorff and not induced by a metric so I suppose from its properties it's quite different.
zariski topology isnt topology tho
yes use these visualizations
you dont need to remember anything ‘symbollically’ ever really
but you should know the details that make your intuition precise
I don't know if the answer to your question can be a calming yes, but what I have to point out is that the all-important Zariski-topology in algebraic geometry is non-Hausdorff and not induced by a metric so I suppose from its properties it's quite different.
@granite copper I still visualize stuff in Zariski topology, but I just draw big open circles to draw open covers and stuff, and to think through some normal point set topology stuff. Just as long as you let go of any sort of distance-based geometric intuition it works for me
Every topological space that is the inverse limit of finite T_0 spaces is homeomorphic to a Spec R for some ring R
Or equivalently a quasicompact space with a basis that is stable under intersections and that is sober
for the above problem, if it is about metric spaces, just notice the definition of open ball in A is different than R^2
thank you, moxwell
@meager python Can you say that in a more basic way again?
how can a metric space be a closed subset of itself?
i'm reading rudin's theorem 2.33 in baby rudin
How are you defining closed here
@marsh forge
is it rigorous enough to just say 'it contains all its limit points'
Sure
ok that's straightforward
Do you see it then?
np

I cannot make sense of the scheme-theoretic image of a scheme
how do you define it when f isn't qcqs?
I'm reading through Francis Su's "Topology Through Inquiry", and came across the following theorem:
Theorem 6.8. Let A be a closed subspace of a compact space. Then A is compact.
I'm a little confused why this was chosen as a theorem. Isn't any subspace of a compact space compact?
No
It's stated as is because it's false if A is note closed
take the interval [0,1] which is compact in R, then consider the subspace (0,1), then an open cover of (0,1) by the sets (0, 1 - 1/n)
No finite subcovering will still cover (0,1)
Aaaa I see. I'll have to think about it a little more but I think it's starting to make sense. Thanks!
does the push forward map only push forward tangent vectors from a manifold to the other, or you can push forward whole fields by it? do you need additional structure to do that?
You'd want the map to be a diffeo, otherwise you get two issues:
- Not all points in the codomain will be in the image of the map, so how would you assign a tangent vector to these points?
- Some points in the codomain will be hit by the map several times, this gives us multiple choices for tangent vectors at these points, and no natural way to single one out. @cursive flume
how can you 'push forward' whole fields?
which object does it,and how is it defined?
if the map F:M->N is a diffeo, and V is a vector field on M, you can define the pushforward F_*(V) to be the vector field on N that takes a point F(p) on N and spits out DF(p)(V_p)
I.e. you just pushforward each vector comprising the vector field on M
so if i say the map is a diffeo,then this def works,right?
this doesn't contain that the map is invertible and inverse is smooth
and also says that only VECTOR FIELDS can be pushed forward, and only covector fields can be pulled back. if the map is invertible/diffeo then one can pull back vectors and push forward covectors too
is this wrong?
it's a little subtle, read: https://en.wikipedia.org/wiki/Pushforward_(differential)#Pushforward_of_vector_fields
The subtlety comes about from the injectivity/surjectivity issue I mentioned above, and is only relevant for talking about fields. For individual vectors you can push them forward and covectors you can pull back always, and if the differential is invertible then you can pushforward and pullback both.
but if i make the map to be invertibe and the inverse be smooth, everything works for fields just as fine as it does for vectors,right?
yep, because the obvious way of pushing forward each individual tangent vector works.
thank you! 😄
no worries 🙂
does anyone know papers/books discussing the hawking-penrose singularity theorems from a mathematically rigorous PoV?
if an affine transformation doesn't involve translation, is it always an isomorphism?
does it hold for the connection coefficient functions,if you multiply the symmetric part by the antisymmetric part,then it is 0?
since they are not tensors
Consider a Riemannian 2-manifold with boundary $M$, and assume that $M$ is non-compact and simply connected (and therefore orientable). Furthermore, assume that we have a harmonic function $f:M\to\mathbb{R}$ which vanishes on the boundary, and is positive on the interior. We can view the interior of $M$ as a Riemann surface, and by the uniformization theorem it is conformally equivalent to either $\mathbb{C}$ or the upper half-plane $H={z\in\mathbb{C}\mid \mathrm{Im}(z)>0}$. The former case can't happen, since the complex plane has no non-constant positive harmonic functions, so $\mathrm{int}(M)$ must be conformally equivalent to $H$. Sounds correct?
gustavn64:
Can someone help me find a clear definition of "(non-)singular curve"?
Can you clarify?
I hope this helps but I'm specifically talking about algebraic curves
Does it suffice to just say "every point has a tangent line"?
Also I'm not sure whether this is equivalent to just having a self-intersection or not but I suspect so
Thanks
Over what field though?
I think over an algebraically closed field derivative 0 means self intersection... but I miiiiiiiight be wrong
well I ended up finding a clear definition after getting to the exercises lol
so gabe u got it xd
Question
In 3-dimensional space, if you take an object and two perpendicular axis of rotation relative to the object, you can achieve any rotation you want.
You don’t actually need the third axis is my point
Does this generalize to higher dimensions? Does an n-dimensional object always require n-1 axis of rotation to be able to trace out all possible rotations, or is there a “cheaper” way?
Actually, do objects in higher dimensions even have “axis” of rotation?
Or is rotation a 2-dimensional phenomenon, meaning an n-dimensional object has an (n-2)-dimensional object it rotates around?
Are there transformations that correspond to higher dimensional versions of rotation?
I remember people talking about this
And I want to quality that my memory isn’t great and I’m not an expert
But you have to specify what you mean by rotate
But I think the definition I heard that’s the right one (someone correct me if I’m wrong) is that you fix a 1-dimensional sub space
Which is the axis of rotation so to speak
But I definitely might be wrong here so take that with a grain of salt
axis of rotation is a 3D thing, rotations really happen in a 2D plane
arent some elements of the euclidean group rotations around hyperplanes?
I think those are called axes too, right?
the hairy ball 
oh hey my manifolds class is also doing a sort of project
Let's say we have a smooth 2-manifold (surface) with boundary, $\Sigma$, assume that $\mathrm{int}(\Sigma)$ is endowed with a complex structure (which a priori does not extend to the boundary). Now let $f=u+iv$ be a smooth complex-valued function on all of $\Sigma$, which is holomorphic on $\mathrm{int}(\Sigma)$. Assume that $u>0$ in $\mathrm{int}(\Sigma)$ and $u=0$ on $\partial\Sigma$. Can we say anything about the directional derivative of $u$ at the boundary, the derivative being taken along an outward-pointing direction? For instance, is it necessarily non-zero? Can we say anything about that same derivative of $v$ at the boundary?
gustavn64:
I think what the first question boils down to is really: We are given a smooth surface with boundary, equipped with a Riemannian metric defined only on its interior, and given a function which is positive and harmonic on the interior, and vanishes identically on the boundary. Is the normal derivative of that function non-zero?
The Hopf lemma seems to say that the answer is yes, under the extra assumption that the metric is defined on the boundary too, but does this still hold when the metric is not defined on the boundary?
I HAVE SINCE SOLVED THIS
Given a quasi-coherent sheaf $\mathcal{I}$ associated to a scheme $X$, I tried to define the closed subscheme asssociated to it as $(\text{Supp}(\mathcal{O}_X/\mathcal{I}),\iota^{-1}\mathcal{O}_X/\mathcal{I})$, where $\iota$ is the inclusion of Supp$(\mathcal{O}_X/\mathcal{I})$ into $X$. I've shown that for an affine neighborhood Spec $A \subseteq X$ that the open set Spec $A\cap\text{Supp}(\mathcal{O}_X/\mathcal{I}))$ of Supp$(\mathcal{O}_X/\mathcal{I})$ is equal to $V(\mathcal{I}(\text{Spec }A))$, which is splendid, the only issue I'm having is showing that this scheme restricted to $V(\mathcal{O}_X/\mathcal{I}(\text{Spec }A))$ is actually affine, presumably it's supposed to look like Spec $A/\mathcal{I}(\text{Spec }A)$, or really the image of the closed subscheme of Spec $A$ associated to this scheme, but I can't for the life of me compute what happens to the sheaf because of this annoying $\iota^{-1}$.
Chmonkey:
When asking for help, do not insist on getting just the answer; we are here to help you learn, not cheat. Likewise, if you are providing help to others, try your best to explain and elaborate instead of simply giving away the answer.
Stick to one channel and don't post the same question in multiple channels. Please don't ask for help in other channels if no one is responding in the one you have posted your question in.
and this is not even topology
its geometry lol
unless something was deleted and you're not referring to magician's message
Let's say I have a given set of points in an arbitrary known shape(8 verticies), and I want to convert this arbitrary shape to a cube (n dimensional) via minimizing the amount distances between points are changed (nonlinearity ok). Is there a "canonical" way to do this?
In addition, this arbitrary shape is infinitely repeating, with some verticies connecting. In the case of a cube, it's an infinite amount of cubes with each cube having another cube touching all faces.
So distances to "outside" shapes need to to be considered.
It is very unclear what you mean
You have 8 points in what space? R^n?
You want an n-cube with 8 points?
What do you mean here by n-cube?
A cube in n dimensions. 8 verticies for the arbitrary shape. N points. Arbitrary shape lies in R3
All arbitrary shapes have the same points inside of them. I want to convert this arbitrary shape to a cube, while changing the distances between the points (a point to all other points, including all neighboring shapes) the least.
Naively, I could just "stretch" the 8 verticies to a cube in R3, but I don't think that's the ideal solution.
I want to keep distortion to a minimum, so if I need to project to a higher dimension that's fine.
You cant use 8 points to create an arbitrary n cube
A cube in R3 has 4 verticies
Im really not following
Can you explain in a longer message and make sure to define your terms
Ie what does distortion mean
In r3, since cubes have 8, and my arbitrary shape had 8, I can naively stretch space to convert the arbitrary shape to a cube.
But you're right. I can't do that for n-Cubes.
I'll type up something more detailed. Give me second.
Here's an example in R2
there is an infinite amount of these shapes, each with their own points inside of them.
In this case, lets say I want to convert this arbitrary shape to a square.
the resulting transformation might look something like this
we can look at the ratio of the side length and the distance between points
and see that this isn't a perfect transformation (im pretty sure)
my question is primarily:
Given an arbitrary shape with 8 verticies in R^3, how can I create the most perfect cubic representation in R^N?
A representation is perfect if forall points, the distance from one point all others expressed in terms of side lengths is as close to the original as possible.
All arbitrary shapes in R^3 are rhombohedrons
I'm not sure if my criteria for "best" is correct, but it's roughly there.
does anyone know what it's on about with the dot products thing?
I can show that it's closed by considering all the convergent sequences, but I don't know how to use this hint
hint: continuous preimages of closed sets are closed
do I sum up all the dot products in a matrix or something? The dot product on its own wouldnt map a matrix to a number
tbh the easiest way to see this is to note that a matrix A is orthogonal iff AA^T = I
and that A \mapsto AA^T is continuous
yeah I did that with a sequence $A_n\to A$
but I do want to understand this hint
i mean, you can define some map from R^(n^2) to R
like, sum up all the dot products <v_i, v_j> for all (i, j)
then the matrix is orthogonal iff it gets mapped to n
ah yeah, and so that will map to {n} which is closed in R
ye
but as i said the easier thing is a map R^(n^2) -> R^(n^2), A \mapsto AA^T
and then its preimage of {I}
but it's the same thing i guess 🤷
oh yeah nice thinking
the thing I was doing before was considering any convergent sequence $A_n\to A$, then the limit of $A_nA_n^T$ is $I$, so the limit $A$ is orthogonal
but I think your way is nicer
yeah, when i want to show that some space is closed/open, the first thing i try to do is show its the preimage of some "nicer" space
I also have a scuffed proof that I feel is wrong but I don't know how to fix, if anyone wants to check
actually maybe it isnt terribly wrong
excuse the "clopen"
You should be careful as Int(A) isn't necessarily the same as the interior of the closure of A
You also shouldn't be able to prove that B is connected given only A is connected with Int(A) = Int(B). Consider for example
A = (- infinity, 0)
B = A union {1}
Inside of the reals R
hmm good points @unkempt bolt I will throw the proof out and try a different approach
when is int(A) not equal to int(clos(A))?
Essentially when some limit point of A has a neighborhood consisting entirely of A and itself
There examples that aren't that bad if you want to think of one
I can give you an explicit one if you want
yea I'm struggling to imagine such a case
oh true
Cool
Unrelated but there's a really nice problem by Kuratowski about closures and interiors
If you want I can state it for you at some point
once I get these proofs done I might take a look
Yeah for sure, just wanted to mention it
$f:\mbb{R}\mapsto S^1,\ f(x)=(\sin x,\cos x)$. Am I right in thinking that $f$ is both an open and closed mapping?
It's locally a homeomorphism and thus an open mapping but I don't think it's a closed mapping
I mean if it’s locally a homeomorphism then it should be a closed mapping as well
Shouldn’t it
No
You could say its "locally a closed mapping"
Maybe by defining that to mean that given any point p there's a neighbourhood U of p so that f maps closed subsets of U (closed in the original topology, not subspace topology) get mapped to closed sets
But the given f is not a (globally) closed mapping
I'm kinda new to this btw, if I say something that's unclear or you want some hints just ask
I think you can take a discrete set in R that maps to a dense set in S^1
As a more concrete way of confirming this idea
Whoever:
The_Vman:
No problem
wo want to help me with an exercise?
I want to prove that there is a unique topology on X such that every $U_i$ is open and every $\phi_i:U_i\rightarrow V_i$ is an homeomorphism. In this topology, a subset $U\subset X$ is open $\Leftrightarrow$ the sets $\phi(U\cap U_i)$ are open for every i.
Davide:
where $X$ be any set and $\phi_i$ be a bijection onto an open subset on $\mathbb{R}^n$ and $U_i$ covering X
Davide:
You need to show that your proposed topology (is a topology) and has the property you claim
Ok
And that any topology with the property is actually exactly this one
I'm sure that is a topology but i can't prove that is unique with this proprieties
Hmm ok
show that its both finer and coarser
than any topology with this property
that will give you the result
I think you are missing one assumption actually
You probably need to assume that for any $i$ and $j$ the set $\phi_i(U_i \cap U_j)$ is open in $\mathbb{R}^n$
The_Vman:
where did R^n come from
Davide i think your problem is poorly stated, could you write it exactly as given
The_Vman:
@gentle osprey yess sorry
in particular, what is V_i
The probelm is relative to non prior topology, a way to define a smoth manifold structure to a set X without a prior topology on X
where $X$ be any set and $\phi_i$ be a bijection onto an open subset on $\mathbb{R}^n$ and $U_i$ covering X
These are the assumptions right? They seem fine
Then you prove that there is a unique topology on X compatible with the no prior topology
Thats not sufficient to make the problem well defined lol
The_Vman:
but its possible that im missing some prior info
so ill just leve it to you
i think he wants like
charts on a set X induce a topology on X and it comes with smth manifold structure for free
I'm just describing where the problem comes from
yeah the problem just doesnt make a ton of sense as written
i think i do first by showing you where the problem is coming from
http://people.dm.unipi.it/martelli/didattica/matematica/2018/Manifolds.pdf
in page 56
yeah okay that makes everything well defined
the question made no sense without that paragraph
anyway! my approach to the problem will still work
I think I am convinced of the uniqueness of the topology
I try to prove that, with this topology, a subset $U\subset X$ is open $\Leftrightarrow$ the sets $\phi(U\cap U_i)$ are open for every i
Davide:
$\phi(U\cap U_i)=\phi(U)\cap V_i$ then $\phi(U\cap U_i)$ is open iff $\phi(U)$ is open iff U is open
while, if $U $ is open, then $U=\cup_j U_j$ then $\phi(U\cap U_i)=\bigcup_j \phi(U_j\cap U_i)$ that is open
Davide:
it's right?
The_Vman:
YEs
Ok so there are still some slight errors
The_Vman:
I don't undestand
$\phi(U\cap U_i)=\phi(U)\cap V_i$ then $\phi(U\cap U_i)$ is open iff $\phi(U)$ is open iff U is open
Here you wrote $\phi(U)$
The_Vman:
I think you sort of have the right idea
The_Vman:

