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19:00
And of course $A_2$ will also just contain the identity permutation
How's it going @Alessandro?
I have to study differential geometry :/ @Dami
hey guys
did my message about induction go through? this machine is awful, I'm on a public machine
it'
it's running Linux and the browser is called Tor and i dont understand the buttons
therefore its bad
19:17
Maybe try the alternative browser, Ext?
well whatever I can handle it for an hour, did my induction question go through
Dami were you around when I was asking for help creating a disjoint collection of sets that union to a collection of not-necessarily-disjoint sets
was it you who helped me
My "hey everyone!" message was the first one I posted today
it was 2 days ago I think
anyway
let $\{E_k\}_{\mathbb N}$ be a countable collection of sets not necessarily disjoint
then I make a sequence
$\displaystyle F_k = \bigcap_{j \mathop = 0}^{k \mathop - 1} \left({E_k \setminus E_j}\right)$
and want to argue that the disjoint union of all $F_k$ equals the union of all $E_k$
what type of induction do I need, if any
well-founded?
it doesnt need to be induction in name I just want to be able to pass the union to a limit of sets
Is there anyone who can help me with clarifying big omega notation?
there's a way you can find out if anyone can help you here
19:23
@GFauxPas But if all the $E_i$ are equal, then the unions will not be the same
I'd be more inclined to phrase it in terms of well ordering of $\mathbb{N}$ than induction actually
countably infinite I mean
If I have x \leq \bigg(2^{-\frac{n}{2}+11} \bigg) can I conclude x \leq 2^{-\Omega(n)}?
if there's only one set it's a singleton
yeah that's what Im thinking Daminark, it's equivalent ofc
So the way I'd argue this would be to say alright, let $x\in \bigcup_{k} E_k$. Then there exists some $n$ such that $x\in E_n$, so choose the smallest such $n$. Then $x\in F_n$
19:26
I'm unhappy with your notation Max but I think I know what you mean, you're saying you want to replace the index with a function of that order?
I can re-write the notation, what part of it makes you unhappy
can I replace 2^{-\frac{n}{2}+11} with omega notation? That is replace 2^{-\frac{n}{2}+11} with 2^{-\Omega(n)}
$\Omega(n)$ is a set of functions, not a function of $n$, but I think I know what you're saying
well to start with you can factor out $2^{11}$ and ignore it, as a positive scalar multiple doesn't change asymptotic growth in this context
isnt it asymptotic decay?
12 of one, 1/dozen of the other, same thing
I see, so I can conclude that by bounding x like that with omega notation, correct?
19:30
I'm saying you can make the question simpler, I didnt answer anything
I'm just saying you can ignore the 11 part
I understand
Thank you very much!
sure, so, now you want to know
if you can replace $-n/2$ with a function in $-\Omega(n)$
yeah
and the answer is, $2^x$ and $\log_2 x$ are strictly monotonic so you can just look at the powers, youre welcome
I see
19:33
if it's for an assignment you'd want to write out the inequalities involved to show your work but my point is you can take $\log_2$ of both sides of an inequality of positive numbers
It's not an assignment, it's for my research
I'm looking into omega notation
and you are using the lim sup definition, correct?
well, if my argument convinced you, you're good. if you're still unsure, write down some inequalities :)
awesome, thank you so much
I dont remember all the exact definitions of $\Omega$ but I'm thinking of asymptotic comparison of sequences
back to Dami
I like what you're saying Dami
choose the smallest $n$ by well ordering then $x \in F_n$ because
well it's obvious but I have to say why it's obvious
because the set difference removed a set not containing $x$
because otherwise that would contract $n$ being smallest
right?
no problem Max
19:42
it remains to show that $F_n$ are disjoint
also obvious :P
why is it obvious tho
well $x \in F_m \implies x \in E_m$
and for $n > m$
Assume $x\in F_i \cap F_j$
Okay yeah
You got it I think, continue
I'm not sure how to say it rigorously
If $n>m$ then $x \in F_n$ and $x \not \in F_m$
but that's assuming the $F$s are disjoint that's circular
So assume $x\in F_n$ and $n > m$
Then $x\notin E_m$
So $x\notin F_m$
ah, I like it Dami. Well ordered sets are cool
If only we could impose a well order on every arbitrary set, wouldn't that be nice
OH WAIT\
meme of head full of stars exploding with light
Did you know Zermelo created the axiom of choice to prove the well-ordering theorem because he intuitively knew the WOT was true but needed an axiom to prove it
not the other way around
he made the AOC to be stronger than WOT, he didn't know it was also weaker
Yeah, I heard
19:55
thanks for the help Dami
are you a student?
Yup
You?
20:16
hi chat
i know it may sound a bit presumptous, because i'm pretty sure i don't have enough breakground to understand why, but I was wondering why $\sigma_s(\nu_2(\mathbb{P}^n)$ does not have the expected dimension for any $n>2$,$s<n$
(recalling $\sigma_s$ to be the $s$-secant variety and $\nu_d$ the $d$- Veronese embedding)
20:28
Yo @Mathein, what's up?
20:48
Analysis question: Suppose for $f: \mathbb{R} \rightarrow \mathbb{R}$, the fundamental theorem of calculus can be used to evaluate $\int_a^b f(x)dx$ for all $a,b \in \mathbb{R}$. Does that necessarily imply that $f$ is continuous?
I.e. can the fundamental theorem ever hold for a discontinuous function?
@konoa: In some sense it's because those varieties have a ton of symmetry. There's a beautiful paper of Griffiths & Harris that does all sorts of projective differential geometry relating to this.
Hi demonic @Alessandro.
Can I bug you with a couple of diffgeo questions?
@Sir: We already said it holds for some discontinuous functions the other day.
sure, @Alessandro.
Wait am I losing it
So what are the necessary conditions for FTC to hold?
20:50
All my manifolds are smooth. $X$ is a manifold, $TX$ and $T^*X$ are diffeomorphic, right?
We didn't answer that, and I'm not sure I know a general answer, but it definitely can hold for discontinuous functions.
Sure, @Alessandro.
Huh, interesting. I like to explore the important differences between antiderivatives and integrals, which most people shrug off as being "essentially the same"
You need to work lots of examples from a good analysis book like Spivak's Calculus or something else.
Ok, I was pretty sure of that, thanks! So we keep them distinct because they're conceptually different, just like $V$ and $V*$ for (finite dimensional) vector spaces
Well, they're dual vector bundles, @Alessandro. So, if you're not in the smooth category, but in an analytic category, they're not generally isomorphic as bundles.
20:53
Hey @Ted, @Sir
@Daminark Howdy :)
@TedShifrin whoa what
@Alessandro I guess you weren't joking about DG :P
Hmm I don't know what the dual of a bundle means
Guess they needn't be even in the smooth category, come to think of it. Even if they're diffeomorphic manifolds. Duh.
Hi Demonark.
20:53
@Daminark nah we mostly did curves and surfaces in $\Bbb R^3$ and looked at some general stuff in the last few lectures
Sure you do, @Alessandro. The fibers are the dual spaces of the other fibers :P
Just another question, if anyone is willing to answer: math.stackexchange.com/questions/2755711/…
@TedShifrin ah, makes sense
@Sir: First, without loss of generality, you can assume the intervals are the same. Now if the images are disjoint, you can certainly find an $\vec F$ where the integrals will be different. You should be able to generalize to see if the images are different on a closed subinterval.
@Alessandro: So what were your questions?
@TedShifrin Wait, so there are no disjoint paths for which the integrals are always equal (besides sign)?
20:59
Nope.
Would you happen to have a proof?
Make $\vec F$ that's totally $\vec 0$ on one and has positive work along the other.
You can use bump functions to glue to make a global smooth vector field.
Well I wonder how curvature is defined for an $n$-dimensional Riemannian manifold, but I guess that's better answered by a textbook than a discusson in chat!
That's sorta involved, @Alessandro. If you read my moving frames section in Chapter 3 I can tell you quickly how it generalizes.
So on to the next question, I have a 2-dimensional smooth manifold. When does it admit a Riemannian metric such that its curvature is constantly 0? (We saw the flat torus in class and it's hurting my brain)
21:01
Compact without boundary?
The flat torus shouldn't hurt your brain ;)
@TedShifrin Well, the paths having the same image doesn't necessarily mean the path integrals will be equal, e.g. if one isn't injective
@TedShifrin I think I should stick to the syllabus for the moment and come back to the interesting stuff after the exam :D so I'll ask you about that at some point in the future
Gauss-Bonnet gives necessary and sufficient conditions in the orientable case. You need $\chi(M)=0$.
I'm wondering what the necessary conditions are for the integrals to be equal, besides the sign
@TedShifrin is that needed? I'm pretty sure the flat torus does hurt my mind :/
21:03
@Sir: Even if it's not injective, they can still agree.
@TedShifrin Sometimes, but not necessarily, right?
@Alessandro: The interesting result is that $K=0$ iff the surface is locally isometric to the plane.
Right, Sir.
Yep, I'm wondering the necessary conditions tho
@TedShifrin o i c why this is fails if u live in complex land now
You could overlap in a back-and-forth way but still make one net trip from beginning to end.
21:04
@TedShifrin the theorema egregium gives one direction, I'm not sure about the other
It's harder, @Alessandro. Shall I refer you to one of my exercises?
You get to use differential forms :P
We just defined today what's a 1-form, I guess I should really learn what they are eventually!
Yes, you must.
I'll add that to the things I shall learn after the exams then
Basically, it reduces to the fact that on a disk a $1$-form is closed iff it's exact. (No cohomology.)
In general, this is a PDE fact in all dimensions (curvature = 0 iff locally isometric to Euclidean space in the usual metric).
WE have to keep you busy learning interesting stuff so you don't have time to run over us innocent people.
21:07
oO
@TedShifrin hmmm cohomology (and homology) are also on that famous list :P
I guess I'll be busy during the summer
But you should read section 3.3 and see how beautiful differential forms make some of that ugly surface theory you learned ... :)
Are you coming to visit?
@TedShifrin id call this an ODE fact moreso
Ok, I'll read it then!
Well, my proof uses Frobenius, which is PDE for sure. And closed = exact is PDE, not ODE.
21:13
When you write up something in Latex and it involves nested proofs, is it best to write \begin{proof} again or is it confusing for the reader? What is the general consensus for when writing a general proof, you'll need to prove something else inside it.
@TedShifrin It's not sure yet
but you can do it w jacobi
I'm sitting here being very stoopid and confused, @EricSilva.
Ah @Alessandro.
I think I'm out of diffgeo questions for now, thanks a lot for your help! @Ted
@Maximus: Nested proofs is not good style.
21:14
^
Happy to continue later this summer, @Alessandro. If something else comes up whilst you're reviewing for the final, let me know.
Have: If $W$ subspace of $V$, then $\dim V = \dim W + \dim V/W$. Problem: If $\varphi : V \to W$ is a linear transformation, then $\dim V = \dim \varphi (V) + \dim \ker \varphi$. I've tried applying what I have to solve the problem, but I just don't see it. It's clear that the problem I am working on implies what I have, but that isn't helpful...
@TedShifrin Thank you, then how would you recommend writing?
I could use a hint.
Move the nested proofs outside as lemmas and invoke them in the bigger proof
@TedShifrin sure, thanks
21:15
@AlessandroCodenotti What if the nested lemmas are connected with the main proof? Do you re-write all the pre-requisites in the lemma?
(Not really related but I never understood "while" vs "whilst" in English)
Sometimes it's preferable to prove the lemmas (or some of them) before, sometimes after.
"Whilst" is old/poetic.
@user193319: $V/\ker\phi \cong \phi(V)$.
I see, so I can say "See proof of Lemma x.x"
as a reference
Frobenius is like an ODE result masquerading as a PDE result
No, it's the result of the lemma, not the proof, that you refer to, @Maximus.
21:17
or prove it before and refer to it, correct? @TedShifrin
yes
that's what i meant, sorry
Yes, @Maximus, or even after.
@AlessandroCodenotti true anglos say whilest
yousay x=y (as proved in Lemma x.x)
yeah, @Maximus.
@TedShifrin Thank you so much!
@AlessandroCodenotti And thank you as well!
21:18
@EricSilva seems legit
Index is 2 hard imo
@EricSilva: I'm having a total mental collapse. How can two real vector bundles be isomorphic and have different euler characteristics? Did I switch orientations with the isomorphism?
Oh good, @MikeM is here to show me how I'm stooopid.
@TedShifrin I tried showing that, but I couldn't figure out the isomorphism.
It's the first isomorphism theorem
@TedShifrin Not seeing what you've written above, but Euler class of an oriented vector bundle negates under orientation-reversal, so that must be what happened.
21:20
@user193319: Have you done group theory? It's just like that. But here the proof is just with bases.
@MikeM: I was commenting earlier that for smooth bundles, $E\cong E^*$.
Isa
Isa
If I have the solution $u(x,y)=\sum A_n e D_n \sin(x)$ of a PDE where I used separation of variables i.e. $u(x,y)=X(x)Y(y),$ and $X(x)=D \sin(x)$ then I'm able to know the explicit coefficient $D_n$ If I use the sine Fourier expansion, am I right?
(Whereas not true in the holomorphic category.)
The trick being that when you reverse orientation on M, e(TM) = -e(-TM), but to get the Euler characteristic, you integrate, which uses the ambient orientation of the manifold, so we get chi(M) = chi(-M).
@TedShifrin Ah, yeah, that breaks the orientation.
You guys, when someone asks questions here, do you actually read the latex? or do you somehow translate it?
I think.
21:22
@TedShifrin Yes, I have. I tried the canonical projection $\pi : V \to V/\ker \varphi$, but this doesn't seem to work.
See "LaTeX in chat" up there >>>>>^^^^^^ @Maximus
@Isa Are you thinking of Fourier's trick?
No, @user193319: Start with a basis for $\ker \phi$ and extend to a basis for $V$.
I.e. identifying Fourier coefficients
@TedShifrin I think the easiest for me to perform a sanity check is with the recollection that oriented Riemannian vbs of rank 2 == Hermitian vbs of rank 1
21:23
@Maximus Use chatjax++
So O(1)* = O(-1) tells me that this isomorphism swaps orientation
Isa
Isa
@Lozansky yes, exactly
@MikeM: I don't see how choosing a Riemannian metric on $E$ to give $E\cong E^*$ messes up orientation. I have taught this before, dammit.
@TedShifrin I am unable to find it
Isa
Isa
@Lozansky I want them to be in the final answer $u(x,y)=\sum A_n e D_n \sin(x)$ but not sure If it's correct to do so
21:24
@TedShifrin It is not obvious to me either, but it must happen. Perhaps the explicit case of O(1) over CP^1 will make the computations clear?
@TedShifrin But my book says that isn't necessary. It says that it is an immediate corollary of the one theorem I already mentioned.
Holomorphic category the bundles aren't isomorphic!!!
@TedShifrin never mind I found it
@Isa You need boundary/initial conditions to determine the coeffiecients
@SirCumference Thank you
21:24
@TedShifrin I'm just abusing notation to denote the underlying oriented real vector bundle
And in holomorphic category I believe O(1)* = O(-1) is true
Which is the "oriented statement" I think you seek
The transition function for O(1) is $z \mapsto z$ on an annulus, right? We could see how that changes using the metric trick.
I don't know, @user193319. I have no idea what your book knows and what it doesn't.
In my first post, I said I have the following: If $W$ subspace of $V$, then $\dim V = \dim W + \dim V/W$. Problem: If $\varphi : V \to W$ is a linear transformation, then $\dim V = \dim \varphi (V) + \dim \ker \varphi$...And my book says it follows immediately from this.
Of course, @MikeM, I know how connection and curvature "transform" when I go to the dual, so I could cheat that way, too. But ...
Isa
Isa
21:27
@Lozansky yeah I forgot about it.. duh
@user193319: But it does follow immediately if you've already proved what I said. I can't do math this way.
So I'm thinking, @Ted, that the identification $E \cong E^*$ restricts to the trivial bundle as the transpose, right?
I'm too slow for this right now.
Me too.
Transition functions for the dual are the inverse transpose.
@Isa Also, $u$ looks to be only a function of $x$? And I would rewrite $A_nD_n = C_n$ for simplicity
So we want $z^{-1}$ transpose, which should just be $z^{-1}$.
That's O(-1), right?
21:29
LOL ... one way or the other.
I would have said O(n) is the guy with transition function $z \mapsto z^n$.
Your point is that $z^{-1} = \bar z$ reverses orientation on the circle.
It depends on whether you're transforming frames or local sections in a trivialization.
hi @ted
hi Leaky.
@MikeM: I still don't see how if all the transition functions for $E$ are in $GL^+(k)$, then the same fails to hold for $E^*$. Grr.
@TedShifrin I think that is true. That guy is still orientatable, just with a different orientation.
21:35
But what does that even mean? Oh help and bother.
I think you swap the orientation on some basic chart, or something like that, I guess
and then the transition functions say this "new orientation" is the "new orientation" on other charts as well
I'm making this up as I go.
This is deplorable that I'm stuck on this.
That's what I should say about my research for the past two weeks as I face a deadline.
Well, ignore me and work on your own stuff. We'll sort this out.
@TedShifrin Catch up with me elsewhere sometime.
21:44
Okey dokey. The key point is that the underlying real bundles of the complex duals are not isomorphic even if the real bundles are isomorphic. ... Talk soon.
22:22
@TedShifrin are you familiar with Omega notation?
can someone explain to me intuitively what omega notation means?
Big O notation is a mathematical notation that describes the limiting behaviour of a function when the argument tends towards a particular value or infinity. It is a member of a family of notations invented by Paul Bachmann, Edmund Landau, and others, collectively called Bachmann–Landau notation or asymptotic notation. In computer science, big O notation is used to classify algorithms according to how their running time or space requirements grow as the input size grows. In analytic number theory, big O notation is often used to express a bound on the difference between an arithmetical function...
Their definition uses lim sup of some 2 functions
22:45
Let $f:\mathbb{R}^n\rightarrow \mathbb{R}$ be twice continuously differentiable and homogeneous of degree $2$.

I want to show that $f$ has its possible local extrema at its roots.

I have shown that (using Taylor expansion around the point $0$) that $f(0)=Df(0)=0$.
This means only that the function can have a local extrema at the root $0$, or not?
23:19
Or do we have to take the expansion at an arbitary point a?
23:40
Does someone have an idea?

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