#point-set-topology
1 messages · Page 196 of 1
have you thought about what this looks like for the topological space X = R^n with the euclidean (standard) topology?
it is possible to have Int A = A, that's the definition of A being open
yeah. Imagine a set like {0} in R, and reason out what Int {0} is :)
do this for a few different kinds of sets in R and you'll start to gain more of an intuition
and once you've done that try it for stuff in R^n
So interior here would be for example a closed ball minus the edge points. What I am thinking about is how a point can be in X but X not be a neighbourhood of it.
right, so the closed ball is a good example
what does it mean for S to be a neighborhood of x in R^2? Like, what's the definition?
where S is some set containing x
also if "X" is the entire topological space then X will be a neighborhood of each of its point
this follows from N2 and the fact that the collection of neighborhoods of x is nonempty
hrm, how does N1-N4 show that the collection of neighborhoods of x is nonempty
it does not
lol. It should have that
no I mean brown includes it above these axioms
they're concerning a system of nonempty sets at each point
actually snype I can give you a concrete example, instead of looking at A = a closed disk in R^2, what about A = a closed interval [0,1] in R? that example at the bottom of my screenshot tells us what the neighborhoods are in R, so you can show A is not a neighborhood of its boundary points 0,1
(also this is the book I first learned topology from!)
it is not!
this book sucks lmfao
I've never read it
¯_(ツ)_/¯
I do think groupoids are more natural though and I'll always stand by that
so in my frosh analysis course we had to write a paper in spring
like on any math thing we wanted
and this course did multivar. and complex analysis so we ended up invoking the jordan curve theorem several times
so i was like
hm, i would like to prove that
but i thought homology seemed scary and categories did not
and Topology and Groupoids proves the jordan curve theorem using seifert van kampen for groupoids
I have the paper on my website still but it's very bad http://untyped.me/groupoids.pdf
anyways i do not have a high opinion of the book on reflection
Makes sense now!
nice!
if you think about R^n a set will fail to be a neighborhood of some point if you can travel in some direction and fall outside the set
travel for arbitrarily small distances I should say
Yes I get it now. It makes sense in rn but in other spaces I suppose one just deals with it
well like
you can't really say what happens in arbitrary spaces imo
it depends on the space
like the simplest criterion is just "A is not a neighborhood of x", that's atomic
yeah the concept of a neighborhood is really atomic
literally in brown's case!
there are a ton of different ways of giving a definition of a topological space
IDK which is my favorite hrm
kuratowski closure with a single axiom
The thing is that I think I found it hard to get definition on neighbourhood in rn from the 4 axioms
for meme points
a topological space is a pair of a set $X$ and a function $\mathbf{c} : 2^X \to 2^X$ satisfying ${\displaystyle A\cup \mathbf {c} (A)\cup \mathbf {c} (\mathbf {c} (B))=\mathbf {c} (A\cup B)\setminus \mathbf {c} (\varnothing )}$ for all $A,B \subseteq X$
wdym by this?
there are multiple topologies on R^n
so there are multiple definitions of a neighborhood in R^n that are consistent with the axioms
shamroc$\overline{k}$
Yeah sorry I meant it didn't immediately follow in my head that the usual definition given in metric spaces is compatible with the axioms
ahh gotcha :)
that can be a little bit harder to verify
personally I think it's always a good idea to introduce these kinda've together
BTW do you recommend this book?
no
like the metric space or R^n definition along with the general definition for topological spaces
i anti-recommend it
as someone who learned topology from it for the first time
I do not think it is a good introduction
the groupoid stuff is vvv cool and it's worth coming back to
Ok would munkres be better?
but I think the exposition, selection of problems, and selection of topics are weird (not talking about groupoids)
I haven't read munkres but I've heard good things ¯_(ツ)_/¯
munkres is fairly dry imo
a lot of people have been recommending this book
and I have been too
but it's a newer book so it's less well-tested than classics like munkres
this looks pretty cool
my first topology book was in french and I can't remember what it was but it was super good :(
I like the selection of topics better
oh wow you're fluent in french? I didn't know that
it was pretty terse and covered it more like french style but it was good
I'm not fluent in french
I see some category Theory there that's quite appealing
oh okay
I am fluent in "throw a pdf into google translate and make do"
lmfao
I think it's a good way to introduce topological and categorical concepts at the same time
and probably builds a lot of mathematical maturity
damn where was that book when i was taking topology
back in my day we had to make do with looking everything up on the nlab
Thats nice to hear because I am also reading basic category Theory by Leinster
hot take: i don't understand how people learn from the nlab. everything is all so jumbled and circularly dependent
100%
i say this despite referencing the nlab quite a bit
yeah nlab is good for finding references when learning, not so much as a first exposure
A moduli stack of elliptic curves is a moduli stack of elliptic curves 
I use the nlab all the time for learning category stuff and as a reference
I don’t find it too circular
nlab is very hit or miss. The stuff there on classical category theory is very good, I think (it used to be a lot worse but it has got better over the years)
maybe circular is the wrong word? I was thinking about how I looked at the dold kan page the other day (which had a lot of useful info/intuition) and the 2nd paragraph jumps into infinity groupoids. this makes sense, the nlab's whole shtick is the npov, but my eyes essentially glaze over when it does this (which is on like half the articles). Part of my motivation for learning about dold-kan is to understand simplicial stuff and eventually infinity cats, but the exposition on nlab relies on already having that understanding
I'm not saying "nlab bad" but large parts of it are written as a reference for people who already know higher category theory, and so the presentation can feel p upside down
yea I think that's fair enough, there are a lot of pages that jump to this point of view too quickly
Let Y be the topological space that looks like the letter Y. Show that Conf(Y,n) is connected.
what does this mean
'Let Y be the space that looks like Y'
how can i know anything from this description
im new to topology
and?
i dont get it
whats the open setsg
XD
im sorry
slimvesus
in other words, they'll be open intervals on the three line segments, and at the intersection it's a little y shape with open ends on each "stick"
this forms a basis for the topology
Consider a complete Riemannian $4$-manifold $(M,g)$ with a nontrivial Killing field $K$ vanishing at a point $p\in M$. Then the flow of $K$ induces a one-parameter group of isometries on the tangent space $T_pM$ and this one-parameter group leaves at least one $2$-plane $V\subseteq T_pM$ invariant. If $\gamma$ is a geodesic with $\gamma(0)=p$ and $\gamma'(0)\in V$, and if $\gamma$ has a conjugate point $q\in M$, does $K$ also vanish at $q$?
gustavn64
In this situation we have a Jacobi field $J$ along $\gamma$ which vanishes at $p$ and $q$, and which is also orthogonal to $\gamma$, right?
gustavn64
can confirm the second thing is true, ya. (the second derivative of <J, γ'> vanishes by the jacobi equation, so <J, γ'> is an affine function; if it vanishes at two points it vanishes everywhere.) don't know how to answer the first immediately though, sorry
so if I have a topology over a set $X$
Corgwn
and $A$ is a subset of $X$ where for all elements $x$ of $A$, you can find a subset $U$ wherein $x$ is an element and $U$ is a subset of $A$
Corgwn
how would you show that $A$ is open?
Corgwn
does the opennness of these sets only specifically apply to the set of subsets paired with $X$ that we include for our topological space, $T$
Corgwn
or are all elligible sets that satisfy the openness property contained in $T$?
Corgwn
let U(x) be some choice of U for a given x \in A
then take the union of all U(x)
this is a subest of A, and contains every element of A, so it must equal A, and it is open
U has to be open for this to be true, otherwise you could just take the singleton
And that would be true for any set
oh thats right i missed that U wasn't specififed to be open
slimvesus
wdym by "that?" The definition of open set is a subset which is a member of the topology defined on the set
right, so $A$ might not necessarily be included in that topology
Corgwn
an arbitrary set A might not be open, i.e. contained in the topology, that is correct.
right
"Recall that a set Z is called countable if it is either finite or it admits a bijection f:N→A. "
is A supposed to be Z here?
if I had, say, a set [-1,1]
how would a disprove that a set that contains 1 is open on that set?
under what topology?
because a subset containing 1 may be open under the subspace topology
i think i know exactly what munkres exercise this comes from lmao
oh, I meant a set over [-1,1]
a set like [x| 1/2 < x < 1]
yes, what topology of [-1, 1]?
or let me rephrase
does this happen to be munkres section 13 problem 4?
maybe it was a 14
one of those
if it is, it's by coincidence
@placid thorn are you going to answer the question lol? You are trying to prove its not open under what topology?
I'm trying to prove that [x| 1/2 < x < 1] isn't open over [-1,1] with 1 as my counterexample
because I know it's on the "edge"
Do you know what a topology is?
its a collection of subsets of a given bigger space
so, [x| 1/2 < x < 1] might be a member of a topology over [-1,1]
wat
like (1/2,1] is open with the usual topology
or if you use the discrete topology {1} is open
I should say that the euclidian metric is being used here
ye so that's what we usually call the usual topology
well why
on the point 1, there's no "neighborhood" around 1
there's no way for me to go an arbitrary positive distance beyond 1 and have space in my set leftover
This is what we were trying to pry out of you 😂
If your space is X, then the ball of radius r around a point a is {x in X: |x-a| < r}. So you only look at points from X. So here your space is [-1, 1], so you only look at points inside that interval
So the ball of radius 1/2 around 1 is the interval (1/2, 1]
right... so what if it was [x| 1/2 < |x| < 1]?
i dont understand that notation
do you mean the set of x such that 1/2 < |x| < 1?
if so that doesnt contain 1
or does writing using closed brackets [] instead of curly brackets {} imply the closure of the set or something?
because i havent seen that before
Corgwn
well (-1, -1/2) U (1/2, 1)
but in any case its a union of open sets
so its open
and it doesnt contain 1
so i dont really understand your question
well, okay, what's an example of a set over $[-1,1]$ on the euclidian metric that isn't open?
Corgwn
I thought that a not open set was anything on the "border" of a topology
[1/2, 1) for example
is not open
singleton sets are also not open
i'd recommend you review your definition of a topology - a topology is a collection of subsets (in this case of [-1, 1]), and we call a set "open" if it is in that topology
in the euclidean topology on a set X, a subset U is open if, for all x in U and some r > 0, (x-r, x+r) intersect X is a subset of U
right
so, for (X, T) in this case
X would be [-1,1]
and T would be the euclidian norm/distance
well what does being "open" with respect to the euclidian norm mean here?
the "intersect X" is important for this specific question
btw
since it means we'll be intersecting any such intervals with [-1, 1]
when considering whether sets are open
Okay, I think I’ve bothered my brain with enough math today
I’ll leave with this question:
So, I’m trying to prove that this weirdly defined set of subsets Is a topology
And to do that I need to show that the intersection of a finite numbers of its elements is also in the topology
right, that's one thing you need to show.
so the set is specifically, for any given input set $X$
Corgwn
the set of all $U$ such that $X-U$ is countable or equal to the set itself
Corgwn
it obviously contains the null set
and obviously, a set made up of the intersection of the null set is also gonna be the null set
but what I want to show is if a set $Y$ made up of the intersections of a bunch of different sets $b$ where for $X-b$, $X-b$ isn't equal to $X$ but is countable, $X-Y$ is also countable
Corgwn
also, for uncountable $X$, is it possible that there exist $X-b = X$ for b besides the null set?
Corgwn
not if b is a subset of X.
right
which all eligible $b$ are assumed to be members of, given the whole topology thing
Corgwn
but back to my first question
for any $b$ that $Y$ is intersecting, $X-b$ might be countable, but since $Y \subseteq b$, couldn't the "uncountable" elements of $X$ that $b$ is removing in $X-b$ go away from $X-Y$?
the "root" of this is showing that X - (U cap V) is countable when X - U is and X - V is
Corgwn
hint: union of two countable sets is countable.
"It's trivial to show by induction that any finite $X - U$ intersection such and such are also countably finite"
oh
Corgwn
oh I'm big dumbus
and then the rest of the statement follows by induction yeah
In what cases could X-u be infinite?
suppose X = R, U = {x | x is irrational or x < 0}
then X - U is exactly the positive rationals and 0
i dont think theres a good, like... characterization of when X-U in this construction will be finite/infinite
I have a question about the shape operator
I know that its self adjoint, therefore, the principle curvatures are orthogonal to each other
but is there an intuitive reason why they must be self adjoint?
like, if I forcibly try to construct a local surface by defining two curves that are not orthogonal to each other, can I even do that?
I think one way is to treat the local behavior of a surface as its quadratic approximation
So for any given point on a surface, take a coordinate system where the surface is the graph of the function, and that point is the critical point (basically, the x-y plane corresponding to the tangent space)
Then, since the second derivative is full rank, it can be locally approximated by the graph of a quadratic, and the principal curves of that are always orthogonal
You could imagine defining a surface as a graph that isn’t locally quadratic
Like this ( x^3 - xy^2)
The thing is, since the second derivative at the origin is zero, the curvatures are both zero anyways, so it’s not a contradiction
Essentially, You can draw a surface where it looks like the principle curvatures aren’t orthogonal at one point, but that necessitates that the second derivative vanishes at that point, i.e the curvature is zero in all directions (i think)
People, how can I prove that the Gram-Schmidt process which maps GL(n) to O(n) is a deformation retract, in the sense that $i\circ r$ is homotopic to the identity on GL(n)? Here, r(M) is the matrix obtained applying the process on $M\in GL(n)$
pmorelli
And i is the inclusion of O(n) on GL(n)
I tried to find a explicit homotopy but it doesn’t seem to be a clever approach
Gram-Schmidt without the normalization of vectors preserves determinants, is continuous, and commutes with scalar multiplication
so you can get the desired deform retract by first scaling everything so that it has determinant 1 and then apply Gram-Schmidt
thanks

bunch of stable homotopy theory nonsense but there are background chapters at the bottom of the table of contents that do homological algebra up through singular homology and cohomology and then basic algebraic topology up through fundamental groups
neat!
"Let $T_\infty$ be the collection of all subsets $U$ of an arbitrary set $X$ such that $X-U$ is infinite, empty, or all of $X$"
Corgwn
is $T_\infty$ not a topology? I feel like that's the case
Corgwn
since you could have a bunch of $U$ where, individually, $X-U$ is infinite
Corgwn
but when you put all of them together, $X-U'$ becomes countably finite
Corgwn
so...could a union of infinite finite sets become uncountable?
right...
and for any infinite set, you can just say without explaining yourself that there exists a set $U$ such that $X-U$ is finite
Corgwn
by just defining $U$ as something like
Corgwn
"Everything in X except for these, three elements"
how do you make a continuous function from a circle to a square?
ya
you would know, approximately circle 
hm...
how could I transform an arbitrary circle $(x-a)^2 + (y-b)^2 = r^2$ to the unit circle $x^2+y^2 = 1$
Corgwn
translate and scale
in that order?
up to you
good catch in that you usually have to be careful about that
but here it shouldn't matter, if you do it right
i'd translate it to the origin, and then scale, since then the scaling should have a particularly simple form



divide the coordinates by r, not sqrt r
it's a circle of radius r
and you wanna go to one of radius 1
like (x, y) -> (x/r, y/r)
hm...
ya it's good
but then how would you make the translation happen?
would it just be... subtracting every point's x coords by a^2?
the center of the circle given by (x - a)^2 + (y - b)^2 = r^2 is (a, b); how do you send that to the origin with a translation?
((x-a)/r, (y-b)/r)
how would I prove that two sets aren't isomorphic over the euclidian metric?
find for any bijective function between them $f$, there's one point $x,y$ where the euclidian distance between $x$ and $y$ isn't equal to $f(x),f(y)$'s euclidian distance, right?
what do you mean by isomorphic? isometric?
Corgwn
i see what you're getting at (negate the definition of "isometric" for metric spaces), but one maybe easier thing you can try is to find isometry invariants of the space that aren't the same for your two spaces
by "isometry invariants" i mean properties of the spaces that are preserved by isometries, like boundedness, diameter, completeness (cauchy sequences converge), etc.
so like a sphere of radius 2 wouldn't be isometric to a sphere of radius 3, both with the euclidean metric, since as metric spaces they have a different diameter (even though they are homeomorphic)
a general tip: if you know your spaces are homeomorphic, the property you find should be defined in terms of the metric
find for any bijective function between them $f$, there's one point $x,y$ where the euclidian distance between $x$ and $y$ isn't equal to $f(x),f(y)$'s euclidian distance, right?
@placid thorn that’s less of a strategy and more of a restatement 🙂
(A correct restatement, if that was the question)
Invariants good. Definitions bad
so the way I did it for R and (0,1) was
"let x be arbitrary and let y = x +50"
so there's a euclidian distance of 50 between x and y
but since f(x) and f(y) need to map to (0,1), the maximum distance between f(x) and f(y) is 1
well, that's the upper bound
and so since 1 \le 50, the euclidian distance between f(x) and f(y) isn't 50, and so regardless of if a valid f exists for R and (0,1), it's never isometric"
that's one way to do it
you can essentially rephrase this as a 1-liner though
||one of 'em is unbounded, other isn't||
usually when we wanna prove two spaces aren't homemorphic/diffeomorphic/isometric/whatever, we do it like that, showing that one space has a property that the other doesn't that would usually be preserved if they were actually homemorphic/...
as cohomo says, definitions bad, invariants good

really
I don't think we've learned that bound equivalence is cause for isometry in the course I'm in yet
is (0,\infty) technically "bounded"?
yes of course it is
but I don't want to use that one liner to show that R and (0, infty) aren't isometric
yea
because there's a value, 0, such that all elements within that set are greater than it
well I figured out (0,1)
now I'm trying to figure out (0,\infty)
Corgwn
Compile Error! Click the
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euclidianistically
or maybe showing that for every x and y = -x pair, assuming that the distance between $f(x)$ and $f(-x)$ is equal to $2x$ leads to contradictions
Corgwn
answer, using an isometry invariant: ||(0, \infty) is not a complete metric space, whereas R is||
but we're talking about $(0,\infty)$ here
Corgwn
fixed
we haven't talked about complete metric spaces in the course though
sadistic prof lol
so I feel like using that here is cheating
so you're saying, suppose we have an isometry f: R -> (0, \infty), then for any x in R, |x - (-x)| = 2|x|, so |f(x) - f(-x)| = 2|x| as well, then you want to derive a contradiction?
hmm
well then f(x) - f(-x) = 2|x| or f(x) - f(-x) = -2|x|
and f > 0
i don't immediately see it, but you can try playing with that a bit
just noticing that f will always be positive might be enough to pull out a contradiction
you could try rephrasing the complete metric space bs in terms of actual cauchy sequences and use that to get your contradiction
like, ||1/n is cauchy, its image in R under an isometry f: (0, \infty) -> R is also cauchy, so its image converges in R, but...||
tbh i don't really see how to do this without just nuking it using completeness
oh shit I know!!!!
👀
we just proved that R and (0,1) aren't isometric
could we show that (0,1) and (0,\infty)...
no, we couldn't
😔
well wait, if the argument works for (0,1), it will work for (0,a) right?
and if we make a arbitrarily large...isn't that the same as showing that (0,\infty) isn't isometric with R?
you mean like your earlier argument will apply to show non-isometry of (0, a) and R? it should, yeah
but i'd be very wary about taking a large like that
yeah it feels too easy
because now you're asking about the (non)isometry of metric spaces that depend on a and whether that is preserved as a gets large
seems hard
yea
i got to go but good luck on the question, hopefully you find an answer that isn't a completeness nuke
yeah me too
" In order to disprove isometry, given the euclidean norm, we must find $x$ and $y$ contained in the real numbers such that $x - y \not= f(x) - f(y)$. Suppose we fixed $y$ as 0, here, obtaining that $x = f(x) - f(0)$, or that $x - f(0) = f(x)$. Consider that $f(0)$ is a strictly positive value, since $f$'s output is over all positive reals, so suppose we then set $x$'s value as $-f(0)$, valid, since $x$ is over all the reals, including the negatives. Thus, our expression would expand to $-2f(0) = f(f(0))$, or that $f(0) = f(f(0))/-2$. This is plainly absurd, however, as it implies that there exists an $x$, $f(0)$, such that $-f(x)/2$ is equal to a positive value, and therefore that $f(x)$ returns a negative output. Thus, we must conclude that $x - y \not= f(x) - f(y)$, when setting $x$ to $f(0)$, and $y$ to $0$.
"
@gritty widget
Corgwn
how would you show that a triangle and a square in R2 aren't isometric?
leveraging the fact that one only has 3 vertices whereas the other has 4?
so, for the metric space ([-1,1], euclidean), {x | 1/2 < |x| < 1} is an open set, yea?
@placid thorn are you still stuck on any of these?
yes for the last one. Proving that is just a matter of showing that for each x in the set, you can find a sufficiently small open ball containing x contained in the set.
Right, where the ball (or line, in this case) is just a “set slider” of sorts.
That brushes up against a bunch of points
Hm...so for ([-1,1], euclidean), {x | 1/2 < |x| /ge 1} isn’t open, because we can’t make a ball that catches 1, right?
Or can we? We could just set our ball’s center at .99 with a radius of .1, right?
you have the wrong idea here. An open ball in [-1, 1] is the intersection of an open ball in R with [-1, 1]
We could just set our ball’s center at .99 with a radius of .1, right?
think about the definition of open ball. This open ball would not contain 1.
well I'm not quite sure what an open ball means here, I'm still having trouble wrapping my head around this.
is it like...a circle and everything in the circle?
or is it just the boundary of a circle?
an open ball in $\bR^n$ would be something like $B_r(a) = {x \in \bR^n : |x| < r}$. Like a filled in sphere w/o its boundary.
kxrider
right, okay
the relevant fact is that an open set in euclidean space is a union of these guys
so let's just take this open ball, and make it's radius .2. Now it contains 1 and 1.05
or did I violate some rule by trying to do that?
closer to the right idea. The space we are working in is [-1, 1]. An open ball in [-1, 1] will never contain the point 1.05. But there is an open ball of radius .2 centered at .99
for example, the open ball centered at .99 of radius .2 would just be the set (.97, 1]
for this particular metric space
yea. btw typo from earlier, $B_r(a) = {x \in \bR^n : |x - a| < r}$ oops
kxrider
right. So we don't need to worry about the fact that 1 is on the "edge" of this particular subset of the big set this metric space is over
yup
and since 1 U the set from earlier is just this set, and we know all the other points from the earlier set are open, we're good here, yea?
all the other points from the earlier set are open
i assume you mean that there are open balls containing each point contained in the set. You're right that each point of the old set is an interior point of the new set for the same reason they were interior points of the old set, and that you only have to check that 1 is in the interior of the new set to show that the whole thing is open.
right, so then what about ([-1,1], euclidean), {x | 1/2 /ge |x| /ge 1}?
I heard from someone that this set isn't open, but I'm not sure why
what about the $/ge$ being after the 1/2 would cause this set to stop being open?
Corgwn
the idea is to show that 1/2 is not in the interior of that set (i.e. that there is no open ball containing 1/2 contained in the set).
right..., well, why not the ball centered at .51 with radius .1?
wouldn't it go to the left of our number line and snatch 1/2?
the distance from .51 to .5 is .01, which is less than .1
because that ball is not contained in {x | 1/2 /ge |x| /ge 1}.
you have that .41 is in the ball of radius .1 centered at .51 while .41 is not in {x | 1/2 /ge |x| /ge 1}.
okay, fine, why not a ball centered there with radius .01?
...that wouldn't contain 1/2 itself, because 1/2 would be just on the border
and if bump up our radius of the ball even a teensy but such that it's now able to capture 1/2, it'll also be containing stuff outside of {x | 1/2 /ge |x| /ge 1} as well.
is that right?
yep
so hold the phone
why were we able to get that to work for ([-1,1], euclidean), {x | 1/2 < |x| /ge 1}?
shouldn't the same argument apply to any ball that's trying to-
no
it doesn't!
because the ball doesn't intersect with anything outside of that set!
since we're restricted to [-1,1]
okay, I think that's where my confusion with this definition was
so, by that, (R, euclidean), {x | 1/2 < |x| /ge 1} isn't open
right, {x | 1/2 < |x| /ge 1} is open in [-1, 1] but not in R under their usual metrics
okay
then I want clarity with one last set...
{x | 0 < |x| < 1 and 1/x \not\in NN}
I think this is open
what is NN?
because even though those restrictions against x where 1/x is natural numbers is a bit of a minefield here for the positive members of x,
natural numbers
so, x couldn't be 1/2, 1/3, 1/4
any member of the harmonic series
as long as you aren't a member of the harmonic series itself, you're gonna have a finite distance between yourself and the next harmonic down, right?
so you can just make your bubble big enough to avoid the next harmonic down
or the next harmonic up
but you'll always have a buffer of points between either
at least I think so
right, this set is open in $\bR$. You have that an open interval is open in $\bR$, and the union of open sets is open. So this set can just be written as $$ \bigcup_{n=1}^\infty (1/(n+1), 1/n)$$
kxrider
oops forgot about the absolute values
Yea
And that set also fits everything in [-1,1] right?
I don’t see why it wouldn’t
It seems like shrinking the set that spawns the topology or whatever is better here
sure, its also open in [-1, 1] for basically the same reason.
It seems like shrinking the set that spawns the topology or whatever is better here
there isn't really a convention about this, but i think i know what you mean. You can right this set as a union of open sets in R which are small enough to be open sets in [-1, 1] on their own
Are there any techniques people know of to determine a maximal polytope containment? I.e., given two d-polytopes, and have the second one fixed, determine whether the first polytope is contained within the fixed polytope given some rotations and/or translations
are normal spaces
like hausdorff spaces but for closed sets?
and is tietzes important?
yes
i've seen it applied in functional analysis like once. I don't think the proof is important. it's nice to be aware it exists
so like
point set topology is of limited importance
there are basic things you gotta know
you gotta know the language
it's very helpful in that way
but pure point set topology theorems are not very helpful
nobody studies this stuff
these notes are the best way to learn point set in my opinion
they're good, and only focused on things people actually use
people studied pure point set a little bit in the 40s-60s, but everything interesting quickly got solved
and what's left is actually set theory/logic
so unless you're interested in that, i wouldn't spend a lot of effort on things outside the doc i linked
you can always learn a random point set theorem when you need it
I was googling and i came across this which explains it really well
From Moschovakis's Notes on Set Theory:
General (pointset) topology is to set theory like parsley to Greek food: some of it gets in almost every dish, but there are no great “parsley recipes” that the good Greek cook needs to know.
the thing is, when more point set comes up beyond that, the book you're reading usually explains it
or gives you enough info to get going
like if i've got the name of the theorem and the buzz words involved, i can probably look it up
and make sense of it
ah i see
that's annoying
you definitely hit diminishing returns after the stuff in hatcher's notes. I don't disagree that knowing these slightly more general theorems exist is worth
basically i agree with you lol
The person who says this scares me
Based
Ultra 5 years ago
That sounds like a lot of fun actually
A computability theorists point set topology course would just be a semester on the baire category theorem
I wonder if anyone's ever given a course exclusively on applications of BCT
in a topological space, How do you show that boundary of boundary is equal boundary
Let A be a subset of a topological space, then ∂(∂A)=∂A
is that true?
I could be wrong but I think they're sticking with the same ambient space instead of putting subset topology on the boundary
Oh by $\partial A$ do you mean $A-int(A)$?
doja max
Closure\interior I think
Ah right.
[REDACTED] 
yes
ok R is the boundary of Q so I take back most of what i said
if empty interior, boundary of boundary is boundary
by defn
But boundary = boundary isn’t true. Take Q in R, the boundary is R, boundary of that is empty
what we should take away from this is that the notion of boundary transcends mathematics and enters the field of sociology
one might say that the notion of boundary is at the boundary of mathematics
if A is closed then interior of the boundary of A is empty set
my guess is that for super nice subsets like submanifolds, it's true
ok, thanks
like ∂S^n = S^n I think
it's funny we were talking tietze today, because I think i can use it to solve a problem my (likely) advisor gave me
are you in grad school?
yeah
🤷♂️
still a baby grad student tho
idk i feel like i'm crushing a fly with a hammer here, i'm going to post the problem and my solution in #advanced-analysis to see if anyone has any better ways to do what i did
probably: chain maps preserve B's so the construction of the map B_n'' into B_{n-1}', which is killed in the quotient
also this is more appropriate for #groups-rings-fields, it's a homological algebra question
here's a real answer: if $z$ were in $B_n''$ we could write $z = \partial'' x$ for $x \in S''{n+1}$. then surjectivity of the map $p : S \to S''$ implies that we can lift $x$ to $y \in S{n+1}$. we can then choose $s_n = \partial y$ since $p(\partial y) = \partial''(p y) = \partial'' x = z$, as $p$ is a chain map. then $\partial s_n = \partial(\partial y) = 0$, so $s'_{n-1} = 0$
shamroc$\overline{k}$
and then the class of that in homology is zero too
@gritty widget sphere quiz
What are the n such that the tangent bundle of S^n can be given a complex structure

Ie we can make every tangent space into a complex vector space compatible with the existing real vector space structure
,w What are the n such that the tangent bundle of S^n can be given a complex structure
Wolfram Alpha doesn't understand your query!
Perhaps try rephrasing your question?
Click here to refine your query online
they're all even dimensional so all of them 
Hmm

X

are you saying all S^n or all S^(2n)?
all the tangent bundles are even dimensional
X
isnt this an open problem?
for n=6
it is not
you're n = 6
the answer I was looking for is n = 2, n = 6
n = even prime
what do you mean by an almost complex structure?
an endomorphism that squares to -1
That is what I mean by a complex structure

That's what a complex structure on a vector bundle is defined as in this book
there's an integrability condition for it to be complex
shhhhhhhhhhhhhhhhhhhhh
yeah, if you want the underlying manifold to a complex manifold then you have an integrability conditiom
yeah, what, did he smash some fucking particles together and find one?
But what I said above was just a complex multiplication on the tangent spaces
yellow chat 

Rip brofibration
brofibration for honorable?
simply mute brofibration
Piss color?
Then we have yellow chat

therapist moment
huh
it actually seems pretty easy to rule out a lot of the spheres
by just using Hirzebruch Riemann Roch
Hi everyone,
I was wondering if a parametric surface in 3D $p(s,t): D \subset \mathbb R^2 \rightarrow I \subset \mathbb R$ can have a one-to-many mapping between its domain and image?
avneesh
Surface is smooth and non-intersecting
By one-to-many I meant that multiple elements from the domain map to a single element in the image
@gritty widget I am sorry I am very new to the subject. It might imply injectivity. I just wanted to confirm
@marsh forge Oh yes. I meant one element from domain to many in image
@marsh forge Okay. Thanks for clarifying
wait
one element in the domain can never go to multiple in the image
as long as you are working w functions
@marsh forge but doesn't that apply to only functions? Or does it apply to parameteric curves/surfaces too? Again, I am sorry if my questions are trivial
all of this stuff is normally defined as functions
it's possible that you might be wrong about what the domain is, however
@gritty widget yes but a circle cannot be a graph of a function (because it has one to many relationships). But it's representated as a parameteric curve
a circle is a function
take [0,2pi] under e^ix
the image is (homeomorphic to) a circle
Okay. Thanks
A slightly dumb question
I am trying to proof that the gauss map is invariant under reparameterisation
But I got stuck
I swear I knew how to do it 9 hours ago
I probably even wrote it somewhere underneath the heap of paper I unceremoniously decide to throw on the floor
Now it’s lost in the sea of scribbles
And my brain is kinda fried
Someone help
<@&286206848099549185>
pretty hyped for my first class in manifolds/DG today
thanks 
what's the syllabus 
basic knowledge about smooth manifolds,including the basic concepts, tensors and differential forms, de Rham cohomology, vectorbundles and covariant derivatives, and (possibly) Riemannian metrics.

hot
a question of my own- do you think classical diff geo (like do carmo's diff geo of curves and surfaces) is a prerequisite for abstract diffgeo?
is there much harm done in doing lee's trilogy first
abstract diffgeo as in what kxrider just posted? nah
maybe for riemannian though, yeah
tbh
i just went through a smooth manifolds course and a riemannian geometry course without knowing the classical theory
it was a little bumpy in the RG class, but not knowing the classic stuff didn't hold me back too much
also like, i think lee goes over the classic stuff here and there
not as a focus, but as a motivation, or series of examples
you're reading hubbard and hubbard's vector calc book, yeah? that should be enough to jump into lee
Great! I gave do carmo a peek and i was bored out of my mind lmao
glad I don't need to go through that
ty!
do carmo has an RG book that does a lot of the things he does in his curves and surfaces book but in more generality 
but do carmo's rg book is also...
ye probs won't touch it on my own
Old books suck 
was traumatized by rudin and i don't want to go through that again
it's not a bad book, it's just rather confusing to read through imo
garbage notation
but the last few chapters of do carmo's rg are great in my opinion 
lee on the other hand is very kind and doesn't write confusing things
yeah I read some of LTM and like the first bits of LSM, and they were super nicely written
is a shame that there are no published solutions to exercises tho:(
just read my exercise solutions 
By the way
Can someone check my solution?
I’m not really used to frechet derivatives
wait how're you defining gauss map? Isn't it a map from S--> S^2? by defn it doesn't care about the parametrization you use
Yeah
That’s why I wanna proof that it’s invariant under reparameterisation
It’s just 1 line in my notes
Like so
It’s not a question, I just wanna make sure I get the chain rule right
And I feel kinda dumb for not being able to this quickly tbh
I learnt my entire course but I still mess up with trivial stuff...
what is sigma_u and sigma_v?
Partial derivative
ah the coordinate vectors given by the parametrization
ok let me think about it for a moment
Thanks man
n(p) is one of the unit normals to the surface at p, and i guess you would want to show that that is independent of parametrization, up to a sign
ok so
i am having a brain fart
chain rule hard

what should happen if $\tilde{\sigma} = \sigma \circ \varphi$ is in $$\frac{\tilde{\sigma}_u \times \tilde{\sigma}_v}{|\tilde{\sigma}_u \times \tilde{\sigma}_v|},$$ the numerator will pick up a scalar involving $\det D\varphi$ and the denominator the same scalar with absolute values, so then the above thing is $$\pm \frac{\sigma_u \times \sigma_v}{|\sigma_u \times \sigma_v|}$$
TTerra
now let me take a careful look at yours
ugh i hate cross products
i'm not sure what happened here
and then if you compute cross products, hopefully things cancel
TTerra
and then that becomes plus or minus 1, which verifies what you wrote
actually, it should be pretty easy to show that, just using the properties of the cross product
@desert bloom
sorry that took so long
Np
what do u think S^1
I ws just wondering why this is a thing that needs to be proved
cuz like, the gauss map definitely isn't unique, there are two normal vector fields for each connected component of S (if it's orientable at all)
maybe if i phrased it as "prove that the unit normal is, up to a sign, independent of chart" it would make a bit more sense
since that's essentially what this is
Intuitively, it makes sense, I need it to make sense mathematically too
Plus practise
(at least, that's what i'm thinking)
Yeah, that makes sense
makes sense, ig I'm just used to thinking of vector fields as inherently chart independent
TTerra
and there you have it
the entire thing is a bit disjointed but it's just a computation, so it might be good to rewrite it all together and make sure it makes sense
too much of DG is checking that things are chart independent 
for example
here's an excerpt from my manifolds course notes
mamma mia
wait so why's this necessary? we know that dx^i is a 1-form, and da_i is a differential which we know is well defined and is a 1-form, so the wedge should automatically be a well defined form, right?
wanna make sure it's equal in the overlap
since it's defined wrt coordinates
then you can extend to all of M
like, it's well-defined in the coordinate chart, yes, but we want something on all of M
spooky
I'm not particularly sure why this^ fails though
that's absolutely true, it's just not the point
let me post the full thing
choice of representative <-> choice of coordinate chart, in this case
if we're comparing w algebra
I meant form as in like the exterior derivative takes the same form in each chart, accidental crash of terminology lol
I wish I knew algebra tho
miss me with that category shit
I like magma

based
the only reason I post sully at partials
is I don't like them and I can't do those computations
this will hopefully change since I'm doin analysis on manifolds this seeester
so invariably we will be doing these kinds of proofs
and I will be sad
let the total derivative into your heart
it will warm you when you are cold and bring you peace when you are troubled
computations are good 🤤
anyways, I gotta use gram schmidt to get an orthonormal basis in stereographic coordinates for my homework 🙃
🤢
ttterrrra please help me with bundles



Heya
Can I ask if anyone have a more qualitative way of thinking about the second fundamental form?
Like I understand the first fundamental form as the dot product on the tangent space
But the only way I understand the second fundamental form is through the shape operator
It seems to be the dot product of something on the tangent plane of the gauss map and the tangent plane
A smooth surface is locally the graph of a smooth function. If you write this function using adapted coordinates (pulling down the surface and rotating it so that the derivative vanishes at the point you're looking at), then the second fundamental form is the quadratic terms in the taylor polynomial of the function
Ah
"the rate of change of the tangent planes taken in various directions within the surface" is cool
well now it depends on what you mean by second fundamental form 
in the single week that i studied this in RG, i learned that the second fundamental form is uh... many different things 
Top bit highlighted in green
How can I interpret a dot product?
For now, I interpret it as some sort of preservation of angles
that's how I see it in the first fundamental form I suppose
Yeah thanks
shamroc don't you sully at me
the geometric and scalar projection things actually make sense
I think I kind of got it now
I am a little dumb, so if its purely mathematical, I will get a little bit swamped
I hope that some day I could understand what -S^1 said
kai I was sullying you because it seemed like Marco was looking for geometric intuition more specific to this scenario
then taylor expand the surface locally
oh lol my sully was justified then
Yeah haha that was my thinking
I don't know this classical diff geo stuff very well, otherwise I would try to help
Sorry
np
I only know this stuff in the general riemannian setting
I tried thinking through it myself
I basically tried using Euler's theorem and parameterise the tangent plane so that it coincides with the directions of curvature
Okay ttera's reaction is fair, I don't really know it in that setting either
But I'm supposed to know it
that wasn't a "not like you know it there either" reaction lol
Lol
it was a
don't know anything about that
hubbard will explain it better than I did I guess, let me grab a screenshot


I'm taking an intro to topology next semester
Exciting!
Are you guys all masters and post grads?
LOL
lmao
nope, I'm a 3rd year undergrad
same
I think ttttteeeerrrrrraaaa is too
ya, im third year
I'm a lowly freshman
you shouldn't compare yourself to others, especially in something like math
^^
well then terry tao would make everyone feel bad 
Its more like I know I need to work a bit more on it
And plus, I want mathematics to be more like a hobby, so I would wanna do it in my free time as well
as of now, I procrastinate too much!
It's more important to decide if it's something you want to work for tbh
Its more like, when I do marathons like this and try and understand my course, I can see glimpses to how fun it could be
I do enjoy it
I wanna enjoy it more though
but your maths courses sounds intense
Mine is just real analysis and differential geometry
I wanna throw in group theory as well tbh
but I do have to choose physics modules as well
physics good
giving you about a minute before people come in here to yell at you for liking something with even an inkling of physics in it

nooo noooo noooooooooooo it's not pure enough nooooooo

The more I do physics, the more I like maths
ritually disembowel yourself
So can I unshoot myself into the sun?

best thing do do is both 


My course is literally called maths and physics
fuck yeah
@shut moat high five
What?
someone solve this system of odes for me
No
?
just do it numerically 4head
this is inappropriate for this channel

Please post in #multivariable-calculus
they're geodesic equations
thank you
lee problem 5-4 
hmm I don't remember computing geodesics
but im just typing it up for completeness
one of the parts is to show that meridians are geodesics
so naturally
i try to write geodesic eqns
yeah but you don't need to find all geodesics for that


... is it even possible to solve by hand?
this question was nice
probably not lol
if you write out the connection, it turns out it is ||the standard euclidean connection plus the cross product||
Huh I don't recognize that one
I'm curious what it is
It's obviously not symmetric lol
unless we work in char 2...

glad to know the real numbers have char 2
Suppse a covector field $\alpha$ is given by
$$
\alpha=a_{i} d x^{i}
$$
Then if we hare a smooth vector field $X=X^{j} \frac{\partial}{\partial x^{j}},$ why do we get
$\left(a_{i} d x^{i}\right)\left(X^{j} \frac{\partial}{\partial x^{j}}\right)=a_{i} x^{i}$
I'm aware that $d x^{i} \frac{\partial}{\partial x^{j}}=\delta_{j}^{i}$
distribute the sums out
snypehype46


