#point-set-topology
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let $f:M\longrightarrow \mathbb{R}$ smooth and non-singular. Show there is a field $X\in\mathfrak{X}(M)$ such that $X(f)=1$
Necrowizard
I honestly have no idea what to do here. Any hints?
one way to do it is to pick a riemannian metric on M and consider something like the gradient of f
I haven't learned gradient in this class yet.
you could do it locally (in a coordinate chart) and then patch the vector fields together with a partition of unity
Professor told me something about it but I honestly didn't understand š¦
what didnt you get
what is the meaning of "Patching the fields together" and why do I need a partition of unity for that
But at this moment I'm guessing even my attempts to do it locally will be frustrated
if you're doing it locally then you can use the gradient on R^n
that is
you can assume that M = R^n first, prove it there, and then work on "patching them together"
as for what that means
TTerra
actually by phi_alpha X_alpha in the summand i mean the vector field on M which is equal to phi_alpha X_alpha on U_alpha and 0 outside
this is a common abuse of notation
if you've seen partitions of unity then you must have seen a similar construction
Okay, I'll work on probing it locally first then
somewhat
i should remark
the two answers i gave are basically the same
that riemannian metrics exist on M uses partitions of unity
and the proof is: cover by charts, in each chart bring over the metric on R^n, and patch together with pou
here you're covering by charts, using the metric on R^n to construct such a vector field, and patching together
thank you
Does your book give you rigorous definitions of these concepts you can work with? I would appeal to definitions here
What is meant by an "edge"
i would also advise like, coming up with a nice explicit description of the set of points in the convex hull as well as a notational system by which they can be uniquely specified
|| barycentric coordinates ||
how do u show that a topological space with an isolated point isn't a manifold
or that a topological space with a self intersection isnt a manifold
but like lets say the object in question
is the disjoint union of an isolated point and a curve
in R2, say
how do i show that that can't be a manifold
okay my object here is the set of (x,y) satisfying x^2(x-1) - y^2
in R2
i want to show that it isn't an embedded submanifold of R2
because it has an isolated point at (0,0)
but im not sure how to do that rigorously
@tight agate
again, what is your definition of a manifold
? the standard definition
hausdorff, second countable, locally euclidean
but then embedded submanifold has its own definition too
this space is hausdorff, second countable and locally euclidean
where we have to consider an embedding from one smooth mfd to another, etc
oh yeah i sort of misspoke
i meant to ask how to show this object is not an embedded submfd of R2
bc of its isolated point at (0,0)
is this more clear?
what is your definition of an embedded submanifold
an embedded submanifold is a submanifold such that the inclusion map to the ambient mfd is an embedding
an embedding between manifolds is a smooth immersion such that it's a homeomorphism onto its image
is this sufficient?
"locally euclidean" could be hiding something like "all components have the same dimension"
since sometimes people say "manifold of dimension n" and require in "locally euclidean" that the space is locally homeo to R^n, not just some euclidean space
(this is directed at pdk)
if your definition does not include the condition that all components have the same dimension, then yes
wdym by components
connected components
are my definitions just like
not clear enough or smth
bc the problem is explicitly telling me to show
that it isn't an embedded submfd of R2
if that is the case, then yes your definitions are incomplete/not clear
idk
tterra probably knows
just admit you can't solve the problem brofib
lee
all the components must have the same dimension
so your space having a point (dim 0) and a curve (dim 1) disqualifies it from being a manifold
does lee define manifolds that way?
yes, go look at the first chapter
no
the definition of a manifold
though invariance of dimension is what ensures that dimension is well-defined (at least for the components of your space) when you take the latter definition of locally euclidean i mentioned
not sure how the definition of a manifold here implies that all connected components must have the same dimensino
i see, ty
Seriously, I don't get it. It seems utterly like running in circles. If {B_i} is already a basis for M, why do I need to set the B_p,alpha's and declare it a basis that is, as far as I understand, composed of the very same elements?
I understand that there are many things in diff. manifolds that seem to be obvious although they are not. This is one of the confusing ones for me. Help...
the B_{p, alpha}'s are coordinate open sets because they're contained in coordinate opens U_alpha
(by restricting the coordinate map defined on U_alpha to B_{p, alpha})
fajitas
maybe try measuring the angle from a point not in U
That's a good idea. Maybe an inner product?

is there a precise definition for āreformulationā in math?
i read earlier that āif Y is compact then pi:XxY->Y is a closed mapā is a reformulation of the tube lemma
i understand how to prove one using the other
synonymous with "equivalent"
okay but
theyāre both just true statements
obviously theyāre equivalent
every true statement ever is equivalent
does that mean every true statement is just a reformulation of every other true statement?
?_?
the other day i asked someone whether the two parts of the FTOC were equivalent
and he said āwell theyāre both true so yesā
so i said āokay but is it okay to say that you can prove one using the other and only elementary methodsā?
and he said ādefine elementaryā and i was like )=
like am i going crazy here what am i missing
this doesn't really fit in this channel, you'll have better luck in something like #proofs-and-logic
try checking out the wikipedia page on reverse mathematics. there have been a variety of specific formal systems proposed that would constitute "elementary methods" in the context of what you're saying
yeah i moved over there sorry my bad
you may get different answers for different systems
if you want to talk about reverse mathematics ask in #foundations
thank u
I saw an exercise in John lee that says a vector field can be defined as the partial derivative with respect to an angle function. How exactly is a partial derivative a vector field?
derivations are vector fields
Maybe it's mapping a point p on the sphere to the tangent vector of the associated level set containing p
fajitas imo you have it backwards
rather than ask "how is a partial derivative a vector field" the right question to ask is like "What is a vector"
this question unfortunately doesn't have a good answer because like, generally there's no good notion of what a thing is. What is a natural number? What is a real number? We are able to give definitions of a natural number in terms of set theory and we are able to define real numbers as cauchy sequences of rationals. but that's not really saying that a real number is a cauchy sequence of rationals, we just do that because it's a technical construction that works for us, and the resulting model of the real numbers has lots of good properties we expect of the real numbers
ok so
scratch the question "what is a vector"
bad question
a more sophisticated question is "How can we precisely define a vector so that all the things we're used to doing with intuitive notions of vectors can be done with this formal model"
and that requires us to sit down and think about what we use vectors for in math. there are different things we want to use them for - for example we like to integrate vector fields along curves - but one of the most important aspects of vectors is that if you have a scalar function f and a tangent vector v, you can talk about the directional derivative of f in the direction v
and so like, for the sake of having a precise definition of a vector, you could define a vector to literally just be a differential operator defined at a point. this is commonly what is done.
so speaking literally, partial / partial x is a vector immediately by appeal to the definition of a vector
Yeah I can imagine a partial as a vector in a vector space.
John lee defines a vector field as a mapping from a manifold into its tangent bundle. I was wondering what tangent vector the partial derivative operator will map a point on a manifold to.
well
what is a tangent bundle
it's a bundle of tangent spaces
what is a tangent space
it's a vector space associated to a point
so again the answer comes back to what a vector is
you can't really define the tangent bundle afaik without explaining what the tangent space is at a point
and you can't explain what the tangent space is at a point without explaining what a tangent vector is
nvm i'm just gonna look at lee
oh wait
are you talking about Lee's topological manifolds
or his book on smooth manifolds
Smooth manifolds
ok what exercise is this
Is was example 8.4 of chapter 8.
ok. well i think if you're reading chapter 8 and you have questions about something which was introduced and systematically developed in chapter 2 you should try reading chapter 2!
I was wondering about vector fields more so than angle functions (the stuff from chapter two).
Forget about angle functions for a month, even though I brought them up.
How does a partial derivative define a vector field?
sorry i meant chapter 3
not chapter 2
i think you'll be able to answer your questions if you read the chapter on the tangent bundle and tangent vectors
Thanks a lot
well in this case it converges to some integer
if you really can't find it I think you can use that x -> 10x+9 is continuous and so the limit x must satisfy x = 10x+9
I would never commit such a sin
Iām still doing AT, turns out that the cohomology ring of the n-torus is the ān-th exterior algebraā. So if the exterior algebra somehow is connected to some cross product in linear algebra then it makes me wonder if thereās some āhiddenā geometric intuition behind why the torus has that cohomology ring
derham cohomology 
I'm having trouble with exercise 16.4.O in Vakil's FOAG. It's as follows. If $X_1, X_2$ are universally closed $A$-schemes, where $A$ is a ring, then the gluing of $X_1, X_2$ along some isomorphic closed subschemes is also universally closed over $A$. Could someone please help?
Porphyrion
So the de Rham cohomology explains this?
It uses the exterior algebra š
There you work with smooth manifolds. You consider smooth functions from the manifold to the degree n part of the exterior algebra over R and these are called differential n-forms. You can integrate differential n-forms over an n-manifold. You can also differentiate a differential n form to get a differential n+1 form (this operation is called exterior derivative). Differential n-forms form a vector space over R and along with the exterior derivatives this forms a cochain complex and you can take cohomologies and the dimension of the nth cohomology tells you the number of n dimensional holes in the manifold
There's a theorem that says that this counts the same holes as the singular stuff
Aleph 0 has a really cool video on this
On some intuition
Oh man
Thatās some good stuff
Ye okay I see, I will need to look up more of this later lmao this seems really cool. Thank you so much! 
You can watch aleph 0's video
no prereqs
Oof yeee I can
I was recommended Gelfand Manin by Brofibration and Weibel by Clerk š
I am reading Gelfand Manin but haven't gotten to that part yet
You can go straight to ch3 in Gelfand Manin
The book is called Methods of Homological Algebra
Weibel I haven't looked at at all so idk
Brofib also gave me some exercises to figure out myself before looking at the book
Maybe you should try too
I'll link it wait
here
okay thanks
also thanks to brofibration
And completely unrelated
But there seem to be many papers
What isā¦
Is there any good way to find these
Googling for what is⦠math
Does not give the result
And another question related to the original question
Hmm nevermind Iāll read more first
Can you try using the valuative criterion for universal closedness?
I havenāt ever done this before but that would be my first attempt
Well, those types of criteria require finite-typeness of morphisms... I don't think it would work generally.
It only requires quasi-compactness of the morphism
But I think this might be a hiccup in the setup when you consider arbitrary schemes
:/
I think one thing to maybe consider
Is it true that the disjoint union is still universally closed?
If so, I think that the disjoint union of X1 and X2 surjects onto the gluing of X1 and X2 along their closed subscheme
Then this should hopefully give you a map over A
Once you base change the universal closedness of X1 disjoint union X2 should give you closedness
Namely, you take a closed set S in the gluing of X1 and X2
Pull this back to X1 disjoint union X2
Then when you push this into X1 glue X2 you recover S because the map is surjective (surjectivity is preserved under base change)
Then pushing S into A is the same as pushing the preimage of S inside X1 disjoint union X2 into A via your universally closed map
So you know the image of S is closed
is there a nice āprogramā for drawing spectral sequences
spooky xymatrix maybe
i would recommend chapter 5 of weibel
Spectral sequences are hard
study the "Blackboxed" examples in the first section carefully to get as much intuition as you can without diving into the technical details. i really like the stuff about the serre spectral sequence
Don't study convergence conditions or necessary or sufficient conditions for convergence at first, you can push them way off.
Learn the spectral sequence associated to a filtered chain complex and the spectral sequence associated to a double complex / bicomplex. Then stop. Don't learn any more kinds of spectral sequences after that, most examples I know of are examples of these two kinds
Make your life simpler. Assume that all filtrations start at 0 and their union is the whole complex. Assume all chain complexes are concentrated in nonnegative degree.
Weibel gives two proofs of the theorem that Tor and Ext are "Balanced". One is in chapter 2 before spectral sequences are introduced, and the other is in chapter 5 using spectral sequences. These two proofs have essentially the same mathematical content so it might be helpful to look at those intuition.
The place i got really familiar with spectral sequences was Godement's book on sheaf cohomology. it's in french and i read it with lots of help from a dictionary and google translate. but it's a great book!
I would look online to see if you can find youtube videos. spectral sequences are a very dynamic and interactive thing, like a lot of diagram chasing related things you either have to do it yourself or watch someone else do it, it's very difficult to understand by reading it
a good exercise is to use spectral sequences to prove that a Cartan-Eilenberg resolution of a complex (regarded as a total complex) has the same homology groups as the original complex, i.e. the augmentation is a quasi-isomorphism
another cool exercise: let X be a cw complex, and let C(X) be its chain complex of singular simplices. C(X) is naturally filtered by the subgroups C(X_n) associated to its n-skeleta. Play with the spectral sequence associated to this filtration and show that the concept of CW homology naturally pops out.
@gritty widget in latex there's a bunch of options for drawing https://tex.stackexchange.com/questions/1085/what-is-the-best-way-to-typeset-spectral-sequences
I think another book that develops spectral sequences in some depth is bott-tu. spectral sequences are a very natural tool for comparing two cohomology theories to show they give the same results. I think bott-tu gives what they call a "tic-tac-toe" argument to prove that Cech cohomology and de Rham cohomology agree for manifolds, which is a standard application of spectral sequences
nice
https://q.uiver.app/ and for simple diagrams this is a fun little website, might extend to some smol spectral sequences
A modern commutative diagram editor with support for tikz-cd.
also i coincidentally wrote a little blurb as well to somebody on where to learn spectral sequences, just this week
i'll just copypaste it: "Chapter 8 in "Hilton, Stammbach - A Course in Homological Algebra" gives a very rigorous way of defining what spectral sequences generally are, where they come from and what they're good for, but in very high level of abstractness; if you're not very well-versed in the basics of homological algebra & category theory, it's easy to get lost ;
There's also this paper: https://arxiv.org/pdf/1702.00666.pdf which is very down to earth and the rigor only comes at the very end, but, in my opinion, it might be simplifying things a bit too much.
And then there's the famous "User's Guide to Spectral Sequences", here https://people.math.rochester.edu/faculty/doug/otherpapers/McCleary-UGSS.pdf which is somewhere in between the two other sources. It's somehow approachable, and somewhat rigorous, too. Didn't really click with me, but it might be nice"
thanks to both of you!
i'll think about this and get back to youi
but i am prety slow so it might be a while
np!
I have a compact hausdorff space X and a closed continuous map $f: X \rightarrow X$
I have a sequence of nested, non-empty, closed and compact sets
$C_1 = X; C_2 = f(X); C_3 = f(f(X)); ...$
I want to show $f\left( \bigcap_{n=1}^\infty C_n \right) = \bigcap_{n=1}^\infty C_n$.
I have shown one inclusion namely that the left-hand side is a subset of the right-hand side.
To show the other inclusion: I take $y \in \cap C_n $. That implies there is a sequence
$(x_n)$ such that $x_n \in C_n$ for each $n$ and furthermore $y = f(x_n)$.
So we have a set $A = {x_n | n \in \mathbb{N}}$.
If this set is finite then there is a constant subsequence $(t,t,t,...)$ in $(x_n)$, so $y = f(t)$ for some $t \in \cap C_n$.
But if A is infinite, then there is a limit point x of A in X.
I have managed to show $x \in \cap C_n$, but don't see how to show $y = f(x)$.
I have also only seen filtration types in the wild and double complexes in books (just realized this message was pretty old when I replied, sorry, not deleting because I already pinged
)
hardisc
Is Godement's book still good if you mostly want to do arithmetic geometry ?
I'm asking because the book was written before the invention of schemes
Sequential characterization of continuity?
@orchid forge I know x is a limit point but I dont know if X is a first countable space. Is it still possible to construct a sequence converging to the limit point?
Nevermind that, but actually I'm not sure exactly what sequence you're talking about.
godement's book is not really about algebraic geometry. it's more general than that. it does talk about algebraic varieties but also about like, paracompact hausdorff spaces, etc. as examples it deals with de Rham cohomology, etc. It develops spectral sequences relating various cohomology theories.
Ultimately tho, everything it says about Cech cohomology and flasque sheaf cohomology is applicable to schemes. It does contain some results on the relation between ordinary dimension of an algebraic variety and cohomological dimension.
Also the first 100-150 pages in the book are a general introduction to homological algebra. which is probably valuable for anyone.
For arithmetic geometry i suspect you'll have to learn etale cohomology which is definitely not covered in Godement's book. I don't know anything about etale cohomology so I can't comment much beyond that. but certainly for everything you would see in Chapter 3 of Hartshorne, the stuff in Godement is applicable. there's a lot of overlap.
@orchid forge
Well $x$ is a limit point of $A = {x_n | n \in \mathbb{N}$. Here $x_n \in C_n$ for each $n$, and $y = f(x_n)$ for each $n$.
From here I would like to show $y = f(x)$.
The space X is hausdorff but I unfortunately don't necessarily have first countability.
Otherwise I could have constructed a subsequence of $(x_n)$ converging to $x$.
FWIW Godement's flasque sheaf cohomology computes the same theory as grothendieck's sheaf cohomology with injective resolutions.
hardisc
Alright, thanks for the detailled answer !
I'll need to learn about homological algebra anyway
If X is finite, isn't the resulting set just the empty set? Or are finite sets also considered countable?
yeah I see why it has to be true for the above to be a topology
but
finite sets can't be put into 1-1 correspondence with N
isn't that kinda bad
oh I thought it was the standard one
I guess not
I skipped the first chapter
yeah
I still like the "at most countable" terminology better
but I should get use to this
Sorry, I'm not sure if it's my fault but I have no idea how this sequence is well defined. If x is in C_n, then f(x) is in every C_(n+1) = f(C_n), and f^(-1)(x) is a closed set contained in C_(n-1) (taking C_0 = X). So if x is in each C_n, then it is the image of something contained in each C_(n-1)
@orchid forge
Hmm, well how I defined the sequence is I take $y \in \cap_{n=1}^\infty C_n = \cap_{n=1}^\infty C_{n+1} = \cap_{n=1}^\infty f(C_n)$.
So there is an $x_n \in C_n$ such that $f(x_n) = y$. This gives us the sequence.
hardisc
$\cap_{n=1}^\infty C_n = \cap_{n=1}^\infty C_{n+1}$ holds owing to the nested property of the sets $C_n$
hardisc
Back to this same question, yesterda @gritty widget helped me with some hints and I'm still lost. I (kinda) understood the part of patching solutions together but I still don't exactly know how to prove that the solution exists locally.
If I write $X(f) = X^{i}\frac{\partial{f}}{\partial{x^i}}=1$, can I just isolate the $X^i$s?
The function f is non-singular, but that doesn't imply it's derivative can't be zero.
Necrowizard
you can try choosing some X^i's that make this true
as a hint, try computing (grad f)f when M = R^n
Isnt' the gradient of f like $\nabla f = \frac{\partial{f}}{\partial{x^i}}\cdot \hat{e}_{i}$ ?
yes
Necrowizard
$(\nabla f)f = (\frac{\partial{f}}{\partial{x^i}}\cdot \hat{e}_{i})f = (\frac{\partial{f}}{\partial{x^i}}\cdot \frac{\partial{f}}{\partial{x^i}})f = (\frac{\partial{f}}{\partial{x^i}})^{2}$ ??
please write in the sums
Necrowizard
oh, I was using Einstein summation notation
sorry
ah, I can't. the indexes are not up and down
yeah lol
anyways i know what you mean
the end result is |grad f|^2
this is non-zero since we assumed f is non singular
so if you divide both sides by that you have your X
Oh I see. Then it's simple to conclude, {y} is closed since X is hausdorff, f^(-1)(y) is a closed set, and x_n is contained in f^(-1)(y), so its limit point x is too
ok, let me try that
got that, thanks
@orchid forge oh lord it was that simple, how did I not see that. big big thanks mate
I heard something like this
does anyone know what the precise statement is
If a space X can be covered by n contratible open sets
the homology groups of X cannot have more than n generators
Hmmm, sounds like some Cech homology fun; the statement that I'm more familiar with and that is easy to prove is that "If a space $X$ has a good cover, i.e. an open cover $\mathcal{U}$ with $n$ elements so that all nonempty intersections of elements in $\mathcal{U}$ are contractible, then $H^k(X) = 0$ for $k > n$"
Lartomato
I haven't heard of a statement like yours, but it sounds interesting
Yeah I'm more familiar with the second statement as well, I would guess it is a relatively simple consequence of the lebesgue covering theorem but I'm not sure
there's a very similar exercise in hartshorne
oh nvm it was about cohomological dimension
but the idea is the same
Larto is right though, the k-th cech cochain group is the free group on nCk <= n generators (one for each k-fold intersection of your n sets), so the cohomology is going to be a quotient of that
The precise statement would then be whatever you need to say your cohomology theory is equivalent to Cech
At least, that would be a sufficient condition
Actually sorry, this isn't the cech cohomology if your cover isn't a "good cover"
ah this is it
It's just a cohomology that's associated to that cover
if X is covered by n contractible open sents
n-fold cup products are zero
its this generaliseation of suspension destroying cup products
I'm calculating pi_m(O) and struggling to see why pi_1(O) is not zero
so like
the action O(k - 1) -> O(k) -> S^{2k - 1} gives you a fibration sequence
wait
I retract my statements
wait no I don't
and in particular in this fibration sequence we have
pi_2(S^{2k - 1}) -> pi_1(O(k - 1)) -> pi_1(O(k)) -> pi_1(S^{2k - 1})
if k >= 2 then 2k - 1 > 2
so this gives an iso
but then pi_1(O(1)) = 0
and we must cry
someone explain to me why I'm dumb :)
does it have to do with O(k) having two path components?
can anyone direct me to a source that will tell me what a homotopy equivalence of kan complexes is
Now I have 5 of the 8 groups. Pi1,pi2,pi3 to go
"Simplicial objects in algebraic topology" Peter may, more combinatorial definitions
"Simplicial homotopy theory" Goerss, Jardine, more categorical/abstract definitions
The union of two closed discs in R^2 is obviously disconnected. But what two disjoint non-empty open sets comprise this union?
open (in the subspace topology)
since connectedness is a property of a topological space, not of a "space, subspace" pair
does that help?
Yes it does, thank you so much!
is there a really really really cool definition/generalization of a manifold that isn't like saying glue copies of R^n a bunch of times? Definitions of manifolds and schemes are weird... they feel like a very-simple-minded generalization of R^n and Spec A.
Can you define a manifold purely in terms of functors the way you can a scheme?
You can define a scheme as special types of functors from CRing to Set
maybe nestruev's book has what you're looking for
i know there's a funky definition of manifold in there
haven't checked all the details... but this feels a lot like the sheaf-theory definition. a locally ringed space which is locally isomorphic to the locally ringed space of R^n with smooth functions.
Hey, if I remove a point from the unit circle in R^2 I still get an open set in R^2 right?
if by circle you mean the filled-in open disk, i.e. {x in R^2 with |x| < 1}, then yes
Okay so I know that the cohomology ring help us distinguish spaces with the same (co)homology groups, for example the torus and S^1 v S^1 v S^2. But how does this work geometrically? From my perspective it almost seems like a coincidence that the cohomology ring has this "property", you first define the cup product and it just turns out that induced maps are ring homomorphisms that "respect" the cup product, but how would I guess before the theorem that induced maps are ring homomorphisms that the cohomomology ring would have this "property"? Like what does the cohomology ring/the cup product measure? I kind of understand that the cup product counts the number of intersections with each simplex if you triangulate your space, but what does this geometrically mean in terms of the torus and S^1 v S^1 v S^2?
Well, when you write e.g. H^2 = R + R, you're forgetting what the generators are and any geometric/algebraic properties they have. The cup product just recovers a bit of that. Geometrically I don't have much intuition besides knowing that cup products are poincare dual to intersections. Maybe it would help to explicitly figure out what generates the cohomology in both spaces you wrote down, and see if you can interpret what the cup product is doing
(remember the cup product is defined at the level of cocycles so it's not necessarily misleading to pick representatives of cohomology classes here)
How seriously should I take the statement
Chain complexes are generalizations of abelian groups
My goal is to understand how
Spectra are mutual generalizations of spaces and abelian groups/chain complexes
The category of chain complexes over a module is an abelian category for which the prototype is the category of abelian groups
But I feel like there is probably interesting stuff already at this level that I donāt know
I don't know if that counts as a generalization though
When you say
AbGrps are the prototype category for abelian categories
Aside from being the main first example
Are you also hinting that we can make some statement like
Abelian categories are enriched over abelian groups?
lol I was just saying this
Oh
Cause I know
Sets are kind of the prototypical category
And categories are enriched over sets
Modulo
Being precise
And in the infinity category case
The infinity category of spaces, which is the infinity category of Kan complexes
Is the pro typical example
And in a way infinite categories are enriched over Kan complexes
I know maybe this should go in abstract algebra or category theory
But top x geom gang just gives the best answers
happy smiley dog ftw 
Oh shit
Abelian categories are enriched over Abelian groups
Yessss
We getting an intuition
š
ye okay I see. So it's all about the generators and the properties they have? So if two spaces have different generators that have different properties in some sense then the cup product captures that and so the cohomology rings will be different?
yeah, the cup product structure tells you how n+m forms are built out of n- and m-forms
One thing I find helpful is
still do the example though, i think it will be helpful
Arbitrary top spaces can be as bad as you like
ye I will think about those later 
Working at the cochain leave is very hard
what are m forms?
uhh elements of H^m is all i meant
oh okay
I don't really get it tbh
okay sure, working at the cochain level might be hard, but does the cup product help with it? Is that what you mean?
Oh sorry I forgot to finish that thought
If you want a āgeometricā intuition
Look up stuff like
What does the cup product look like for manifolds
Kogasa mentioned about the cup product being related to poincare duals of intersection forms
Getting a good understanding of the cup product in this situation can help
ooh okay I see I see. Thank you both so much! 
I think I need help
So I want pushforward of transsition map
But the problem is idk how to do it
maybe im being a baby nvm
i hve been struggling with this problem for longer than necessary
yeah i don't think there's much that anyone can help with, you have to just write down the definitions and go through the calculation carefully
ok
so ive done jt
and its cancer
so much cancer I might cry
ill write up my proof and show in around 3 hrs
which field has worst notation?
im guessing geometry
the computations are bad but at the end it should be a pretty simple formula
there's just a lot of indices
this is "a thing" but i don't remember the details. maybe a really categorical book on diff geo would have the answer. something like "Natural operations in differential geometry"
yeah this is because hatcher's definition of the cup product is shit lmao
this is what i was complaining about the other day
but there are much more natural ways to motivate the cup product
one is in de rham cohomology where it's just the wedge product of differential forms, which is a very basic operation.
another is using stuff from diff top, the intersection of transversal submanifolds is somehow related to the cup product (please forgive me if that sentence isn't grammatically correct, i don't know any diff top)
even in singular theory there are better ways to motivate it than just giving that bullshit formula hatcher gives
i was going to write something up on this the other day, sorry i never got around to this
but like, speaking simply
the geometric intuition i have for this stuff
and i have like, most of the formal details worked out, but not all
but
there's a binary operation called the join on topological spaces $X\ast Y$. The join is defined as $(X\amalg X\times I\times Y\amalg Y)$ modded out by the equivalence relation $\sim$ defined by requiring that $x\sim (x,0,y)$ and $(x,1,y)\sim y$ for all $x,y$. basically this is the operation that takes two spaces $X, Y$ and creates a new space out of them by freely drawing lines from each point in $X$ to each point in $Y$.
diligentClerk
this binary operation on spaces $\ast$ is functorial, in that given maps $f : X\to X', g: Y\to Y'$ there's an induced map $f\ast g: X\ast Y\to X'\ast Y'$
diligentClerk
Hatcher defines the join in Chapter 0 if you want to see a reference for this stuff
anyway this is a very natural operation for simplicial stuff because $\Delta^p\ast \Delta^q\cong \Delta^{p+q+1}$
diligentClerk
this is easy to work out
more generally if $X,Y$ are two simplicial complexes (or for you, delta complexes, because you're studying hatcher) the join of $X\ast Y$ is again a simplicial complex (delta complex) in a natural way. no subdivision etc is required like for the cartesian product, it's just a corollary of the fact that the join of two simplices is again a simplex.
diligentClerk
moreover, and this is pretty cool, if $X, Y$ are delta complexes, and $C(X), C(Y)$ denote their associated chain complexes (derived from the triangulation, then the chain complex $C(X\otimes Y)$ of the join is easy to calculate using the complexes $C(X)$ and $C(Y)$ - it's exactly the total tensor product $C(X)\otimes C(Y)$, up to a dimension shift (which i'm going to be a bit handwavy about here because the details are pretty complicated)
diligentClerk
here by the total tensor product I mean $(C(X)\otimes C(Y))n = \bigoplus{p+q=n}C(X)_p\otimes C(Y)_q$
diligentClerk
with the usual differential
Ok. So, topologically, there's a natural map $X\times Y\to (X\ast Y)^I$. It's easy to describe what this is: it sends the pair $(x,y)$ to the canonical path from $x$ to $y$ in $X\ast Y$, remember $X\ast Y$ is constructed exactly by freely drawing lines from points in $X$ to points in $Y$.
diligentClerk
And then of course $(X\ast Y)^I$ is naturally homotopy equivalent to $X\ast Y$, although not by a unique choice of natural homotopy equivalence. You have a map $(X\ast Y)^I\to X\ast Y$ given by "evaluate the path at $0$" and $X\ast Y\to (X\ast Y)^I$ given by "send $p$ to the constant path at $p$" and these two are naturally homotopy equivalent, so $X\ast Y$ is a deformation retract of $(X\ast Y)^I$.
diligentClerk
In the strong sense, I guess.
Grr. I'm worried on the edge of saying something nonsensical so i'm trying to be careful.
Here's an exercise you can do that will hopefully give you a sense of the point i'm trying to make
Let's work in the category of pointed topological spaces. If $(X,x_0)$ and $(Y,y_0)$ are given, i assume you know what is meant by the wedge product $\land$ and the reduced suspension $S$. I define the reduced join of $(X,x_0)$ and $(Y,y_0)$ as the join $X\ast Y$ modded out by the equivalence relation given by asking that $(x,t,y_0)\sim y_0$ for all $x,t$, and $x_0\sim (x_0,t,y)$ for all $t,y$.
You can prove that $S(X\land Y)\cong X\ast Y$ where all operations are interpreted in the reduced sense. This shows that the join and smash product are kind of the same up to a degree shift, a dimension shift, because we interpret the suspension operation as shifting all the 'holes' in the space up by one degree. conversely the smash product is like a downshift of the join
diligentClerk
a 'delooping'
ok. so there's some nice relationship between the cartesian product (or in the pointed case the smash product) and the join, in that they agree up to a dimension shift.
We have already said that if $C(X)$ and $C(Y)$ are the chain complexes associated to delta complexes $X$ and $Y$, then the chain complex of their join $C(X\ast Y)$ is just the total tensor product $C(X)\otimes C(Y)$ shifted up by one. Or to say this another way, $C(X)\otimes C(Y)$ is a kind of "delooping" or downshifting in the category of chain complexes which is given by taking the "join" of the two chain complexes and shifting everything down by one dimension.
diligentClerk
On the other hand, how should the operation of forming these chain complexes play with the cartesian product? In the singular case at least, the singular $n$ simplices $\Delta^n\to X\times Y$ are in bijection with the set of ordered pairs $(\sigma, \tau)$ where $\sigma : \Delta^n\to X$ is a singular $n$ simplex in $X$ and $\tau$ is a singular $n$ simplex in $Y$. This follows from the universal property of the Cartesian product of spaces. So if $C(X)$ is the chain complex of singular simplices in $X$ and $C(Y)$ is the chain complex of singular simplices in $Y$, so that $C(X)_n$ is free on $n$ simplices in $X$ and $C(Y)_n$ is free on singular $n$ simplices in $Y$, then $C(X\times Y)_n \cong C(X)_n\cong C(Y)_n$. (There's a theorem about abelian groups which says that the free abelian group on the cartesian product $A\times B$ is isomorphic to the tensor product of the free Abelian groups on $A,B$ respectively. this isn't hard to show.)
diligentClerk
I'll denote the chain complex $C(X)_n\otimes C(Y)_n$ by $C(X)\times C(Y)$. of course it's not really the categorical product in the category of chain complexes, which could be confusing, but normally we'd use the direct sum notation for that, and i don't need to talk about the direct sum here anyway. We view $C(X)\times C(Y)$ as algebraically representing the cartesian product of the two spaces.
diligentClerk
So, from the homeomorphism $S(X\land Y)\cong X\ast Y$ that we talked about earlier, we might hope that in the category of chain complexes we can get the "Cartesian product" $C(X)\times C(Y)$ to agree with the "delooping of the join" $C(X)\otimes C(Y)$. Indeed this is the case. These two complexes are naturally homotopy equivalent! This is called the Eilenberg-Zilber theorem.
diligentClerk
It's a great theorem. the actual formulas are a bit of a combinatorial nightmare but it is possible to get geometric intuition for what they say, I promise!
i won't go into that right now. But the point is, this Eilenberg-Zilber theorem $C(X)\times C(Y)\simeq C(X)\otimes C(Y)$ is really really fundamental. It's the basis for all the product structures in singular homology and it comes from this subtle relationship between the Cartesian product and the join.
diligentClerk
Now, one of the important things about the homology functor from chain complexes to graded groups (i.e. sending $C_\bullet$ to $H_\bullet(C) =\bigoplus_n H_n(C)$ is that it actually plays nicely with the total tensor product in that there's a natural transformation $H_\bullet(C) \otimes H_\bullet(C')\to H_\bullet(C \otimes C')$. A pretentious way of saying this is that the homology functor is 'lax monoidal'. The famous Kunneth theorem gives necessary and conditions for this map to be an isomorphism using homological algebra to describe the quotient. similarly in cohomology, say with coefficients in modules $G,G'$, there is a natural map $H^\bullet(C,G)\otimes H^\bullet(C',G')\to H^\bullet(C\otimes C',G\otimes G')$.
diligentClerk
It's not hard to work out what these natural transformations are on your own. Take an educated guess!
Now. If we combine the Eilenberg-Zilber theorem i described a minute ago with this natural transformation, what do we get? Let $X,Y$ be spaces, we'll look at singular homology.
We have natural maps
$H_\bullet(C(X))\otimes H_\bullet(C(Y))\to H_{\bullet}(C(X)\otimes C(Y))$.
But of course $H_\bullet(C(X))$ is just $H_\bullet(X)$, and $H_\bullet(C(Y)=H_\bullet(Y)$. And by the eilenberg-zilber theorem there is a natural homotopy equivalence $C(X)\otimes C(Y)\cong C(X\times Y)$, so $H_\bullet(C(X)\otimes C(Y))\cong H_\bullet(X\times Y).$ Thus we get a natural map
$H_\bullet(X)\otimes H_\bullet(Y)\to H_\bullet(X\times Y)$.
diligentClerk
This map is called the cross product in homology.
It is the most fundamental product structure in singular homology.
There is also a cross product in cohomology
$H^\bullet(X;G)\otimes H^\bullet(Y;G')\to H^\bullet(X\times Y;G\otimes G')$.
We can derive this almost exactly the same way as the other one, with minor changes, so i won't explain that in detail.
diligentClerk
The most important case of the cross product is when we take $G =G'=R$ for some ring, $R$. Then we can use the multiplication map $R\otimes R\to R$ to give a map $H^\bullet(X\times Y;R\otimes R)\to H^\bullet(X\times Y;R)$. It's obvious how to do this i think.
diligentClerk
Thus combining these two we get a map $H^{\bullet}(X;R)\otimes H^{\bullet}(Y;R)\to H^\bullet(X\times Y;R)$. This i think is also sometimes called the cross product map in cohomology.
diligentClerk
Ok. So now we arrive at the cup product, at the very end. Set $X=Y$ and look at the diagonal map $\delta : X\to X\times X$. Then because cohomology is a contravariant functor, there's an induced map $\delta^{\ast} : H^\bullet(X\times X;R)\to H^\bullet(X;R)$.
diligentClerk
If we combine this with the cross product from earlier we get a map $H^\bullet(X;R)\otimes H^\bullet(X;R)\to H^\bullet(X;R)$.
diligentClerk
That's the cup product.
So I think we should understand the cup product in terms of the cross product and not the other way around, as hatcher does.
seems a bit bizarre to me honestly.
This is the exposition Spanier gives in his book and this was kind of a revelation to me after Spanier's attempt
he doesn't give much geometric intuition but at least the order of development makes more sense
Anyway i'll stop there but talk to me another time about if you want some more intuition for the formulas in the eilenberg-zilber map and where they come from
we also have the alexander whitney map
i've been working pretty hard on my own to try and get these formulas to just fall out of the sky naturally by appeal to general categorical principles
i've gotten some of them
ok.
done there
peace
š„¤āļø
i didn't see it as i'm on dark background.
thanks for pointing it out.
:pettheclerk:
I think he wants you to talk about the categorical properties of the topological space "cup with a straw" and how it relates to this cartesian product map
oh i'm an idiot
(i don't actually think that)
oh true that is what that is
tteppa now that it's like 24 hours later what do you have to say about warner's book on smooth manifolds and lie groups
i never had a moment to look at it or read the original question i got pinged for
that night i went and got wasted with my friends
and i spent today hiking
nice
Wikipedia says the homology of spheres can be computed just from the axioms. That seems interesting - is there a simple characterization of such spaces? And am I right in thinking they are precisely the ones whose homology can be computed without reasoning about what the maps that show up between homology groups do?
Also, if a space is assigned the same homology groups by every homology theory, can we compute them from the axioms?
(By the "axioms" I meant Eilenberg-Steenrod axioms with the dimension axiom)
the axioms are enough to give you the Mayer-Vietoris sequence, which you can use to do a bunch of simple examples
i dunno if there is an exact characterization of spaces whose (co)homology is determined by the axioms though
is mater vietoris sequence the LES made with relative homology?
like LES of (Sn,dSn)
or am i thinking something not it
yea thats not it nvm
re: this, I think you can relatively easily show that the axioms are sufficient for a space with a sufficiently nice cover
because of this fact
I think even then we need to reason about maps somehow?
well yes
inclusion maps in particular
but inclusion maps are mentioned in the axioms, so you can still say some stuff
intuitively it should be possible for any space that is built in a nice way out of other spaces whose homology is computable from the axioms
Reasonable
if you don't include the dimension axiom though
it might get weird
you still have MV but one fewer building block, in this analogy
We wouldn't know the homology of, say, D^n?
yeah I don't think so
I think this should follow from the completeness theorem in logic, but sadly I don't even know its precise statement. If it is true, then maybe we can use the result that the axioms determine the simplicial homology for all triangulable spaces, or something, and in this case my question is kinda trivial because a whole theory is "built" from the axioms.
if you replace the homotopy axiom with weak homotopy then the question definitely does become trivial
What does it say?
if weak homotopy equivalences induce isomorphisms in homology then, since any space is weakly homotopy equivalent to a CW complex, we can just compute the cellular homology of that, which i think is the unique homology theory satisfying the axioms for cw complexes
Aha
So the axioms are "too" strong in this sense
i'm not sure
Most "identities" in specific groups cannot be deduced from group theory axioms
I mean there are many groups but only one homology (when we restrict to nice spaces)
there is a paper by Milnor that shows that there is (up to isomorphism) only one additive (co)homology theory on the category of pairs (X,A) where both X and A have the homotopy type of a CW complex
still using the dimension axiom though
Do we get a consistent theory by picking an arbitrary sequence of groups, and saying these are the homology groups of the one-point space?
I mean replacing the dimension axiom
I was wondering the same thing, there's all kinds of generalized homology theories but I dunno what you can get by fixing the homology of a point
the first derived things you meet are derived functors in the form of Tor and Ext
and the as far as i understand
these are best thought of as obstructions to tensor and him being exact
i assume we can do something similar for any other functor possibly modulo small conditions like being a functor in abelian categories
can someone tell me
what the big picture of derived algebraic geometry is
why do you do it
feel free to use terms i wonāt understand
i am more so lookin for an answer that i can stew on and eventually learn where thins are going
I'm a bit confused as for what to do here. I'm on 1c and I don't think I really understand vanishing lines very well.
This is what I have so far.
nonorientable Riemann surface
Yo omg I didnāt even see that you wrote all of that! I will need to take a careful read through it later on because this is good stuff. Thank you so much!

I donāt claim to know all of derived algebraic geometry but the āwhy do you do itā is the same reason as you listed above; if for example you are considering an intersection theory, there are cases of intersection multiplicities being less than you want because of Tor groups which are āinvisibleā unless you take the entire derived tensor product into account
I also just very quickly want to ask if $\alpha \smile \beta[v_0, \cdots, v_n] = \alpha \smile \beta [v_{\sigma(0)}, \cdots, v_{\sigma(n)}]$ where $\sigma \in S_n$, so is the cup product independent of how I choose to "represent" my simplex? Because I know that if you permute some $v_i$'s in $[v_0, \cdots v_n]$ then the orientation might change, so does the cup product respect that? If this holds up to sign change, then how do I know how I'm supposed to "label" a simplex when I'm calculating the cup product?
Tokidoki ā
so let's say that I have this torus and I want to look at $\cup: H^1 \times H^1 \to H^2$. I know that $H^1(T^2; \mathbb{Z}) = \text{Hom}(H_1(T^2), \mathbb{Z})$. The boundary of the sum of the simplicies in the picture above is zero so I want to look at that. $a$ and $b$ are the generators of $H_1(T^2)$ and so the dual basis for $\text{Hom}(H_1(T^1), \mathbb{Z})$ is $\alpha$ that sends $a$ to 1 and everything else to 0 and the same goes for $\beta$. Let $\alpha$ be a representative of $\alpha$ in $H^1(T^2)$ and the same for $\beta$. I want to have $\alpha \partial = \beta \partial = 0$ and this is true since I have drawn the $\alpha$ and $\beta$ with orientations (which looking at it now, does it really matter what orientation $\alpha$ and $\beta$ has? It seems like no matter what I choose, $\alpha \partial$ will always be zero). Now the thing is that I have $\alpha \smile \beta [1, 3, 0] = 1$ but $\alpha \smile \beta[0, 3, 1] = 0$ even though $[1, 3, 0]$ is the "same simplex" as $[0, 3, 1]$. So how do I know which one to pick?
Tokidoki ā
i dont need any hints, i just dont understand what is being asked
what does it mean for A-tilde, p to be the covering space corresponding to the kernel of that map
proving that A tilde is a covering space isnt difficult
iāve heard this example before of bezouts theorem and trying to find the right way to count multiplicity
i suppose i more so want to know
what objects do we derive
Is it possible that in some metric space, we can never attain the minimum length among all the curves connecting two points so only the infimum of the length is obtained?
weilam06
Oops it's arbitrary metric space
My bad
I think it's correct by considering R^2 with origin removed
My concern is that if we pick (-1,0) and (1,0), let says, then yeah; but what if I take two points on R^2 which its shortest line segment does not pass through the origin?
so you want this to be true for all points?
Yeap
Ideally we derive schemes and stacks. Derived tensor product of rings becomes derived fiber product of schemes (apparently this still not a fully developed theory though)
All of the stuff like spectral schemes are basically attempts to make a rigorous theory of that
Tfw serre intersection formula 

It's talking about the galois correspondence between covering spaces and subgroups of pi_1
okay thanks
I think I'm slowly realizing how shitty Hatcher's examples of the cup product are
My definition of a variety is a ringed space $(X,\mathcal{O}_X)$ such that there is an open cover $U_i$ of $X$ such that each $(U_i,\mathcal{O}_X|_U)$ is isomorphic to a closed subset of affine space. I want to show that if $f$ does not vanish on some open set $U$ then $f$ is a unit in $\mathcal{O}_X|_U$
lime_soup
this is obvious if U is an affine open set
yoo you lost the light blue name
but dont' see how to do this for an arbitrary open set
Cover U by affine sets, then for each V_i in the cover we have a local inverse g_i now notice that g_i and g_j have to be equal on any intersection because on V_i \cap V_j fg_i=1=fg_j. So that means that the g_i satisfies the sheaf condition so there exists g on U st g restricted to V_i=g_i and g is the inverse
Maybe take R^2 - (Q x Q)
Ohh then the denseness of Q in R showing that the shortest path is not attainable right
No problem, also this should hold in general for locally ringed spaces, because the germ of f at each point x is not in the maximal ideal of the stalk so it has an inverse in that ring so it will have an inverse on some open set containing x, now we can use the logic I gave to finish off
thanks!
If you have only learned cup product from hatcher, i strongly recommend you look into the de Rham formulation for geometric intuition
ye I really need to do that
read (the beginning of) bott & tu maybe
there's so many details in these examples that Hatcher skips
it's an awesome book to read
He just claims a bunch of stuff like "oh it's an easy calculation that blablabla" when in reality you can't even compute that thing because that thing is dependent on how you label the vertices and he hasn't done that
okay roger that! Thank you so much!
I'm trying to under the segre embedding
sorry i keep accidentally hitting enter ill type this all and then post it
Hi! I have the following question: prove that if F -> E -> B is a locally trivial fibration, where the base space B is contractible, comapact and T2, then this is a trivial fibration, that is E = B x F. Can you give me some hint regarding the solution?
I could be wrong but I don't think there's a particular trick here. Lifting a nullhomotopy of $B$ lets you identify all these copies of $F$ in the local trivialization: given $(b,v) \in B \times F$, the nullhomotopy gives a path $b \to b_0$, which lifts to a path $U \times F \cong p^{-1}(b) \to p^{-1}(b_0) \cong V \times F$, and you associate $(b,v)$ with the other endpoint of the path ending at $(b_0, v)$
Kogasa
err those should be $b \times F$ and $b_0 \times F$, not $U \times F$ and $V \times F$
Kogasa
does this make sense at all? i can draw a picture if not
maybe a simpler way to say it would be, if B collapses onto b then you can collapse a local trivialization U x F onto b x F in a unique, continuous way (by some lift). Each e in E lies in a fiber over p(e), and collapses onto (b,v) for some v in F, and we identify e ~ (p(e), v)
then you can either prove this is an isomorphism directly or use the universal property of cartesian products
i'm trying to compute the derivative of the curvature of a curve and i keep getting the following (in terms of the unit tangent vector T in the frenet frame)
geometroid
geometroid
How exactly are you chain ruling the sucker
,,\kappa' = \frac{d|T'|}{dT'} T''
Oh I see
why is it 0?
geometroid
Its zero because the curve is unit speed
oh that is true
but that seems weird, why would the curvature derivative be zero?
implies curvature is constant
unit speed =/=> constant curvature
But not T' dot T''
Yeah I always screw that up lol
that resolves my problem, thx u
Cause T itself is the derivative of a thing
this is still not true
it is
It is if |T|^2 is constant.
(which, if 1, is what it means to be unit speed)
thanks u saved my night
I think the best way to remember this is that T' when normalized is N, the normal vector.
But then T'' is not the binormal
ok so this finally yields an expression for torsion
geometroid
in terms of just derivatives of the unit tangent vector
i needed it
to do uhh
to compute the variation of an integral over torsion

ah shit it turns out theres another difficulty hiding right after this one
turns out my night is stunted again
simply overcome it

It's giving cope
This is for my analysis class but i thought posting it here might be more appropriate
All we discussed about dense subsets is that their closures r equal to the parent set
So the image of the closure of E is equal to the image of X, any hints on what to do next?
That statement is equivalent to "f(E) closure contains f(E closure)", and you can prove this by looking at sequences converging to points in the closure (I'm assuming you're working with metric spaces)
Yes we r
f(E) closure contains all the limit points of f(E) right?
How do we relate that to f(E closure)
Take a point of the latter and show that the point must be in the former
So i said let f(x) be in f(E closure), so x is in E closure
Ultimately we want to show f(E) closure is equal to f(X) dont we?
Yes, when you take closure inside the subspace f(X)
So it suffices to show only one inclusion
As in, you have some U ā A ā B, and you want to show that U is dense in A, ie closure of U in A is A, and this is equivalent to showing that closure of U in B contains A
Because then everything in A is a limit point of U
If f(x) is in f(U), you can't be sure that x is in U
But you can start by saying
Let y ā f(E closure), then there is some x in E closure such that y = f(x)
there was a brief mention made in an algebra lecture that if X is compact and hausdorff, and if C(X) is the ring of all continuous functions from X to C, then all maximal ideals of C(X) consist of the functions that evaluate to 0 at a given particular point x of X. I can easily see that each such ideal is maximal, but I can't see why all maximal ideals have this form, and where the properties of X being compact and hausdorff come in at all
it was just meant to be a fun little cute example šš
If m is a maximal ideal such that the elements of m have a common zero, then there must be at most 1 common zero, otherwise you have a larger proper ideal containing it. Now suppose there are no common zeroes. Then for each point in X there's a function f_x in m which is non zero at x therefore in a neighborhood U_x of x. By taking powers of f_x you can assume that the real part of f_x is positive on x (hence on small enough U_x). Take a finite subcover of this cover and the sum over (the x in the finite subcover) of f_x and this is non zero everywhere hence a unit
if i just wrote $\int \alpha\otimes\mathrm{d}\beta$ where it's understood that $\otimes$ is a tensor product, is this even well-defined? you need antisymmetry in the tensor algebra to use geometric integration, aka the wedge product, so I'm puzzled at friz and hairer using this in their papers/books
teafortwo
the idea is for the regular euclidean case to collapse to lebesgue intengration of alpha wrt the induced measure of dbeta
the exterior algebra is a quotient of the tensor algebra
so it could just mean the corresponding equivalence class in the exterior algebra
so im taking this integral modulo that class?
i guess i should check that preserves representation invariance
ohhhh ok that's so nice, I assume somehow X being hausdorff was used secretly, but I didn't catch it and maybe my mind jumped assumptions. what step fails if X is non hausdorff?
I don't think hausdorff is needed for this part, it's needed to say that x ⦠m_x is injective
oh right
actually I'm not seeing why the sum over the finite subcover is nonzero everywhere
each f_x is nonzero on U_x
but when you add them
Oh you're right that doesn't work
oof yeah, this works when you have real valued functions and you take squares
you can form a function algebra generated by the finite set {f_x}, so like polynomials in those functions
but I'm forgetting what neat properties those have
like if that ring satisfies certain properties then I know it's dense in C(X)
so you could just make it close to some unit
oh yeah that could work
and therefore make it a unit
How would you show that this algebra separates points?
that's what I'm thinking of rn
If $f_x \in m$, then $\bar{f_x}$ is continuous and $|f_x|^2 = f_x \cdot \bar{f_x} \in m$ right?
Kogasa
I was thinking of saying like maybe it doesn't
but if it doesn't, then your functions must already be nice
in some way
Perfect
I was trying to work with weaker condition of being closed under multiplication šµāš«
Good evening guys, I'm kinda stuck on how to go about this problem.
So some background first.
Two metrics, d1 and d2 on the same set X are called strongly equivalent if there are constants
0 < c < C such that
c d1(x, y) ⤠d2(x, y) ⤠C d1(x, y)
for all x,y in X
Prove that the following metrics are strongly equivalent (R^k)
- Taxicab (Norm 1)
- Standard Euclidean (Norm 2)
- Max Metric (Norm inf)
I think this might actually work lol
You can change X to X/~ where ~ identifies all points that aren't separated and quotients of compact spaces are compact
So this algebra is a dense subalgebra of C(X/~)
yes yes yes
so the other points are filled in because they are defined as the ones that aren't separared
it seems silly to separate points if all we are looking for is a function with no roots š
but this is my only way of using the results I know š¤š¤
my other option would just be modifying the Weierstrass approximation theorem for a weaker condition... and no thanks
sorry!!!! I didn't see this
that's wonderful
that's wonderful
now I'm š¤¦āāļø
i was literally like "hmm if these were real we could just square them"
"too bad there's nothing like that for complex numbers" š
good work team
I don't remember sending this twice š¤š¤
appreciate if anyone has any pointers on how to get started.
Try sketching what an open ball looks like in each metric, and the equivalence condition talks about fitting scaled versions of the open balls in different metrics inside one another (after you fix an x)
You can guess what c and C would be by looking at those sketches and then formally prove the inequalities
Taxicab and standard are kinda easy
Itās basically drawing a triangle
Like, just consider points on the unit circle
Since you can just scale stuff
ohh, ok, so for 1) and 2) I see that the c = 1 and C = 2/sqrt(2) does that work?
c and C should depend only on the dimensions
i wonder what we can say about strongly equivalent metrics that are dimension-independent. can they only be scaled versions of the other?
hahahaha
right sqrt(2)
Right
For the infinity norm
Well
was it true in general that taxicab >= standard >= infinity
I think so by just
Looking at the unit circle again
So I think strongly equivalent is transitive?
Like⦠pretty easily?
Infinity balls are squares 
So I think it boils down to the infinity and standard
And for this oneā¦
I remember being presented this proof on day 1 of analysis
Freshman year

But I donāt remember the idea
Isnāt it something stupid like uhh
Oh well
Isnāt the infinity norm minimized at like
45 degree angles?
If that makes sense
ez to prove by showing two sided inequality
Itās when the two coordinates have the same absolute value

(Again on the unit circle)
Infinity balls are actually squares lol like sides parallel to the axes
Oh right
What if this isnāt R^2

Well whatever, find a point where infinity norm is minimized
you maximize the infinity norm by just moving a single coordinate
Wrt the unit ball
minimize it by making them all as close as possible
Well you wanna minimize it
Yeah
You should be able to minimize it and get a constant
bonk
Just work on the unit ball (in Euclidean, lol)
And everything else will scale out the same way
ok, I'll try
Hopefully this was actually helpful
It would have been if you didn't nitpick dimensions 

I'm just stuck on showing the inequalities. I assume it goes something like the triangle inequality proof
Iāll let moldi handle this
Oh shit the problem was in R^k
Chmonkey was right

Chmonkey wins again
It won't be ā2 in higher dimensions
Will be āk
ye
Now maybe you'll have more success 
btw @empty grove I just realized, even though we are over this, all ideals separate points, it's necessary for them to absorb multiplication.
The 0 ideal doesn't 
But yeah as long as the ideal doesn't vanish at a point that makes sense
Urysohn right?
urysohn what?
Wait how are you proving this
So to prove the inequality, do it based on the norm of the point wrt the euclidean one.
When you have a point on the sphere of radius r in euclidean
You just need to prove that the taxicab length is at most sqrt(k)r
You can do this by say, I think am-gm
Maybe?
If not you can use calculus⦠if you have access to that
I think I just have the definition of the metric to work with
so the metric function
What is gonna be the best way to do this then
Fix an x, prove the inequality for all y, choosing c and C to be independent of x, so that the inequality is shown for all x as well
And without loss of generality you can do this for x=0
Oh well
In my head Iāve already done this kekw
Iām just struggling to come up with a nice proof that this bound works for points on the sphere
Without calculus
I actually donāt think am-gm works?
Does it?
Let me have a think
It seems like youāre bounding the arithmetic mean by the wrong thing

draw a triangle and do induction
^ yeah
Fix M
Thinming š„ø
Write out k things in the form
x_i = M/k + epsilon_i
And uh
I guess the sum of epsilon_i = 0
So my general proof struct, give c and C. Fix arb. x,y in R^k, try and show inequality holds
Then expand out what the Euclidean norm of
(x_1,ā¦,x_k) is
Like the point is I want to show this is less than the norm of
(M/k,M/k,ā¦,M/k)
In terms of the differences epsilon_i
Or something
Lmfao
Idk if this works though lmfao
Like well
We can ignore the sqrt
So it comes down to showing that
(M/k + epsilon_1)^2 + ⦠+ (M/k + epsilon_k)^2 <= k (M/k)^2
And like on the left hand side
We get k(M/k)^2
Along with like
2M/k(sum epsilon_i)
= 0 by assumption
And then the sum of epsilon_i^2
So we need to show that sum epsilon_i^2 <= 0
When these are numbers chosen so that they sum to 0
Does this⦠work?
ĀÆ_(ć)_/ĀÆ
Wait this has to be bullshit
I messed up somewhere
These are all nonnegative cuz square
I'm just gonna do induction
for the inequality
monkey magic
Oh wait Iām dumb
Itās cuz
My inequality is supposed to be backwards
Lmfao
I want to show that
For a fixed number for the sum of the coordinates
The Euclidean norm is GREATER when the coordinates arenāt all M/k
And so it should be showing sum epsilon_i^2 >= 0
But this is⦠obvious
So it should be like this
Fix x
If the taxicab norm is M
Call the Euclidean norm uhhh
N
I swear this should work
I am just drawing a blank on order to do it hurb
Oh RIGHT
Okay sorry
So N(x) >= N((M/k,ā¦,M/k))
And note our taxicab norm is M
By assumption
So it suffices to show that for the constant C
That CN((M/k,ā¦,M/k)) >= Taxicab norm(x) = M
But also the point (M/k,ā¦,M/k) has taxicab norm M
If you have radius r, then you're trying to compare distance in standard norm (which is āk times RMS of coordinates) and distance in taxi cab (which is k times the AM of coordinates). RMS ā„ AM gives āk standard distance ā„ taxi cab distance and taxi cab distance ā„ standard should be just Pythagoras 
So we can basically just show that CN(M/k,ā¦,M/k) = CM/sqrt(k) = M
Wtf is the RMS AM inequality bruh
Lul it's root mean square
Itās mega pepega
Hurbed
It's annoying to prove RMS ā„ AM and I'm sure you're just trying to do that ultimately
But it should be fine to assume this inequality
RMS is also called QM (quadratic mean apparently)
And I think RMS ā„ AM might be just Cauchy Schwartz
Hey, does anyone know an explicit example of a homeomorphism between S1 and D2 to the torus? Like an example of a function
Do you mean from S1 x D2 to the solid torus?
Yes, the solid torus, sorry I wasn't clear on that
For me, an explicit homeomorphism would be the identity, but what is the solid torus for you?
The filled in donut?
Oh I see where I've gotten mixed up
I mean from the circle S1 and the solid disk D2 to the solid torus which is the product space of S1 and D2
what does "and" mean in "from the circle S1 and the solid disk D2"?
So I know that the solid torus is the product space of the circle and the disk. I'm asking if there is an example of f(s, d) where s is in S1 and d is in D2 and the image of f is the solid torus
But then aren't you asking for a function f: S1 x D2 -> S1 x D2?
I mean, the solid torus, as you said, is S1 x S2. And you are asking for a function that takes two inputs, namely from S1 and D2, and spits out something in S1 x D2. Why not simply take the identity?
So I guess I've been skipping a step somewhere - I have subspaces D2 and ST defined explicitly, and I'm supposed to construct a homeomorphism between D2 x S1 to ST. I thought by looking at an example or two I could have an intuition of how to do it.
$D^2 = {(x, y) \in \mathbb{R}^2: ||(x, y)|| \leq 1} \subset \mathbb{R}^2$
subspaces of what?
wOne
Do you view ST as a subset of R^3?
I can? I'm not sure if I have to
$ST = {(x, y, z) \in \mathbb{R}3: (2 - ||(x, y)||)^2 + z^2 \leq 1} \subset \mathbb{R}^3$
you just said \subset R^3 
So I was given these 2 expressions for D2 and ST, and I'm supposed to find a homeomorphism g: D2 x S1 -> ST
I did, and admittedly I was using them interchangably because I don't know of a difference between them now
difference between viewing the space ST and viewing ST as a subspace of R3
wOne
saying "space ST" doesn't tell you what the topology is, only the underlying set, unless you say that you are inducing the subspace topology from R3
I mean all you did was give ST as a set, you have to describe the topology somehow, and saying that it is a subspace is probably the easiest way to say it
otherwise you haven't given enough info
Sorry, a bit confused now - so you're saying that by me describing ST as a subspace of R3, I have given enough information to describe it?
yes because you have told us that it has the subspace topology
without that we don't know the topology
like if you want to describe the space ST separately you have to describe the topology in some other way
So I suppose this earlier definition of ST described it as a subspace of R3 then
Then in that case, is there a way to come up with a homeomorphism from my definition of D2 plus an arbitrary S1 to my definition of ST?
Plus doesn't make sense, you are asking for an isomorphism S¹ x D² ā ST
Okay, then given that you seem to know what I'm asking for, do you have an example of such an isomorphism?
I'll tell you the isomorphism going backwards. So ST has a map onto the circle, which is just "ignore the thickness of ST", and it has a map onto the disk, which you get by taking each disk cross-section of ST and mapping each point in this cross section to the corresponding point in the actual disk
This is scuffed 
But this gives you maps from ST to S¹ and to D² and put them together in a pair to get a map to the product
Like imagine S¹ x D² as a bunch of disks glued together in a circle, that's exactly what ST is
yo can I ask a quick question?
** ** 
š š
okay lmfao so what is the difference between a k-vector and a k-form?
I'm watching some video online but they don't really say the definitions
k-form in the sense of?
element of exterior product of copies of k?
Mathematically, they're dual to one another. Lemme see if I can find the bells and bongs interpretation.
oh yeah, so a k-form "measures" a k-vector right?
let me just review this before I say something wrong 
I'd say that's good.
wait what does a k-vector mean? k is a natural number and you mean k-tuples of vectors?
Misner Thorne and Wheeler's gravitation talk about it pages 115-120, I really shouldn't screenshot all of that lol.. ||You can find it online for free though, shh||
I honestly don't know, the video keeps saying "k-vectors" and "k-forms" without really defining them
but I guess that k-vectors are just vectors with k components
So a k-form is an alternating multilinear function from product of k copies of R^n to R (replace R with any field and this works)
So k-vectors aren't used that much (and I don't know if the wedge product is defined for them), but again they're ideally dual to the k-forms.
Isn't that just a k-dimensional vector? Not the same in this context, heh.
ye it is I guess but I don't really know what else this guy could be talking about lmao