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00:00 - 18:0018:00 - 23:00

18:03
@MikeMiller Ok cool. It's somewhere in Hatcher I suppose?
@MikeMiller and thanks for the illustration!
Chapter 4 in Hatcher
Ok thanks
18:25
How do I prove that $e^{\frac{\pi i}{b}}$ is a simple pole of $\frac{1}{1 + z^b}$? I was thinking of using the geometric series expansion, but that won't work because we need $|z| < 1$.
Note $b > 1$
I have a question about metrics. $ds^2=dx^2+dy^2$ is the usual Euclidean metric. What is $ds^2=dxdy?$
What do you mean, what is it? It's a Lorentz metric.
@user193319 Think about zero rather than pole.
oh okay that's what I thought, I just always see it written like this $ds^2=dy^2-dx^2$ lol
@TedShifrin So show that it is a simple zero of $1+z^b$? Is that easy even if $b$ is not an integer?
how do you go about computing the order of a zero
18:40
Well, for polynomials that's "easy", but I don't know how to do it in general.
can you relate the order of a singularity to the coefficients of the Laurent expansion at that singularity?
Yes, I think that's originally what I was going to try, but Ted told me to think about zeros of $1 + z^b$ instead of singularities of $\frac{1}{1+z^b}$ (although they end up being related).
@geocalc Think about how you can rotate coordinates and turn $xy=c$ into $x^2-y^2=c$.
yeah, the order of zero $e^{\pi i/b}$ of $1+z^b$ is the negative of the order of the pole $e^{\pi i/b}$ of $1/(1+z^b)$
it generally holds that $\operatorname{ord}(f/g,a)=\operatorname{ord}(f,a)-\operatorname{ord}(g,a)$ when $g$ isn't zero, this is a good exercise
Clearly $e^{i \pi/b}$ is a zero.
If $z_0 = e^{i \pi/b}$ were of greater order than $1$, we'd have $1+z^b = (z-z_0)^kh(z)$ for some $k \ge 2$ and some analytic $h$ with $h(z_0) \neq 0$.
18:44
anyhow, if you know how to relate the order of a singularity to the coefficients of the Laurent expansion, you're good, because I claim that you know a very easy way to compute the coefficients of a power series expansion of a holomorphic function (and that's all you need at a zero)
Oh, so compute the power series expansion of $1+z^b$ at $z_0$?
If $a_1 \neq 0$, does this mean it is of order $1$?
That is, a simple zero?
@TedShifrin yep got it. So I think I know how to generalize this metric to $n$ dimensions
no to the former, yes to the latter
$ds^2=dxdydz\cdot\cdot\cdot dn$
I'm telling you there's an easy way to get these coefficients without computing the power series
well, of course, if you have the coefficients, you have the series, but you only need one of the coefficients, namely $a_1$
18:47
actually that may be wrong...
@geocalc Nope.
Metrics are quadratic forms/bilinear forms.
it's gonna be so complicated.....
@Thorgott Oh, isn't it a certain integral $\frac{1}{1+z^b}$ around the boundary of a circle enclosing $z_0$?
too complicated
forget the complex stuff
this is a fact about power series
how do you get the coefficients of a power series if you know the function it defines
Oh, it's $\frac{f^{(n)}(z_0)}{n!}$ for the $n$-th coefficient.
18:51
correct
@TedShifrin okay I can generalize $ds^2=dx^2-dy^2.$ to n dimensions, but I'm having a problem with the other one
now the rest is easy
Okay, so this shows that $a_1 \neq 0$, and therefore $z_0$ is a simple root of $1 + z^b$ and hence a simple pole of $\frac{1}{1+z^b}$. Is this the correct line of reasoning?
You have to add a positive definite metric in $n-2$ dimensions.
it's a correct line of reasoning
It's possible to compute the Laurent expansion of $1/(1+z^b)$, but I believe the computation would be a lot uglier than this
18:58
so the final metric in say 3 dim. would be of the form $ds^2=(dxdydz)A$ where $A$ is a positive definite matrix?
19:12
What? Reread everything we’ve discussed.
@Thorgott You really need this to do the beginning of the Laurent expansion.
what do you mean?
The only way I know how to compute the Laurent expansion is to use the Taylor expansion of the denominator (around the relevant point, of course).
well yeah, but it's, in general, an ugly computation
19:30
I like doing those Laurent series computations even for residues. I always drilled my students on those (as oppose to various higher-order derivative computations). But the latter aren't good if you want the actual Laurent series for a few terms.
what is the geometry induced by the metric $ds^2=\log(dx)\log(dy)$?
That makes zero sense.
which part?
The expression.
you can't take the log of dx?
19:34
Not if you want to make mathematical sense.
can you explain better I'm confused
$dx$ is a one-form; you can't do random functions with those.
Remember that a metric needs to be a bilinear form on tangent vectors.
@TedShifrin the problem is that I derived that $\log(x)\log(y)=1$ is a preserved metric of a transformation
sorry, I mean that $\log(x)\log(y)=1$ is a preserved metric of $(x,y)\mapsto (x',y') = \left(x^{\exp(\Delta b)}, y^{\exp(-\Delta b)}\right)$
trying to get the metric from this
 
1 hour later…
21:06
Hello everyone!
Hey there
Guys, should I worry if I hate doing epsilon-delta proofs? It's not fun at all.
why do you hate it?
It's much more interesting to prove more general statements, not applying formal definitions to explicit functions.
I mean, I prefer proving that the inverse function of a continuous function that has a compact domain is continuous than proving sqrt(x) is continuous for the domain [0,\infty)
Is this nonsense?
Oh Gosh another topological man
21:30
Hahah I'm just starting to get a taste for all of these things, but it does seems more laborious than it should to do epsilon-delta proofs
And I'm not saying that I prefer another definition of continuity, for example, but it's just that when working with specific functions (such as a simple sqrt(x)), the proof is very specific and usually involves intense algebraic manipulation or some trick
But I might be wrong, as I said, I'm really new to all of this
You are right, it can be tricky somehow if you do not manipulate correctly
A lot of mathematics depends on estimates (not algebra, but analysis, numerical analysis, differential equations, geometric analysis ... and the list goes on), so that's what you're starting to learn to do.
Nothing is fun until you learn to get better at it.
I never found manipulating symbols in abstract algebra at all fun.
I still don't, but now I understand that there's a lot of beautiful concepts going on in that algebra.
@TedShifrin That is probably true, as these tricks don't come easy at me, so I get lost quickly and that's obviously not fun.
I guess the way to get better is keep trying and doing exercises?
There are some standard methods to learn, and yes, as with everything in mathematics, you have to practice a lot.
I wrote a handout for my Calculus with Theory students some years ago on basic $\delta$-$\epsilon$ proofs. If you want to email me, I'll forward it to you.
Sure! May I email you at your UGA email?
21:39
Yes, absolutely.
@TedShifrin Sent you! Thanks!
Lots more exercises to practice, if nothing else :P
Sent.
Received! Thank you!
learning to use $\varepsilon-\delta$ in actual proofs is important and pops up everywhere in analysis, but proving that a specific function is continuous using $\varepsilon-\delta$ is most often just an extremely ungrateful exercise
Well, it's surprising how many calculus books (and even analysis books) make a hash of it all.
I still remember when I first encountered this stuff reading Thomas's Calculus book in high school, he had ad hoc garbage with cube roots of $\epsilon$. I would never allow my students to do that nonsense.
21:49
I don't believe anyone has ever generated as much as an ounce of insight out of proving that some random degree $3$ polynomial is continuous via $\varepsilon-\delta$, but I used to see a lot of questions in that vein on main
Once you know how to do a quadratic, I agree you're not learning too much, but doing it once is good. The key thing to learn is what I always called the "stipulate" game, and then of course you'll have to know how to divide your cubic by $x-a$.
But if you can do synthetic/long division, it really doesn't matter what the degree of the polynomial is if you do this right.
In case of finite measure spaces $L^p$ sits inside $L^q$ if $p > q$. Not true in eg $(1, \infty)$ anymore. What's a unifying way to say these stuff?
it feels very redundant to prove anything polynomial is continuous using $\varepsilon-\delta$ when it's sequentially obvious. Students should learn about both continuity in terms of sequences and in terms of $\varepsilon-\delta$ in a course and why they are equivalent.
Once they have that, forcing them to apply one definition when the other is much more natural just feels very counter-intuitive (there are equivalent ways of defining things everywhere in math and students should learn to actively decide which definition is best suited for their purposes and then apply that). There are still
22:05
@BalarkaSen The general phenomenon is that there is such a nesting iff $X$ does not contain sets of arbitrarily big measure iirc
@Balarka $L^q\not\subset L^p$ iff $X$ contains set of arbitrarily small measure and $L^p\not\subset L^q$ iff $X$ contains sets of arbitrarily large finite measures
wait, I mean not subset
Garbage phrasing Thorgott
@AlessandroCodenotti ya
the operator norm of the natural embedding is $\mu(X)^{1/p - 1/q}$
you can fix the phrasing yourself
measure spaces which does not contain nonempty sets of arbitrarily small measure -- lol
also known as completely garbage atomic spaces
Can't you say something with norms
I guess you can also say the finite measure space thing is a consequence of convexity of L^p spaces + $L^{\infty}\subset L^1$ iff $\mu(X)<\infty$
22:08
its a consequence of direct calculation
it's all just direct calculation
$\|f\|_{L^p} \leq \max\{\|f\|_{L^q}, \|f\|_{L^r}\}$ if $q < p < r$ is true maybe
yeah just Holder innit
something better is true
we just discussed this yesterday in here lol
20 hours ago, by Thorgott
I think I got it. Pick $\alpha$ such that $\frac{\alpha}{p}+\frac{1-\alpha}{r}=\frac{1}{q}$. Then $p/\alpha q$ and $r/(1-\alpha)q$ are conjugate and Hölder gives $\int|f|^q=\int|f|^{\alpha q}|f|^{(1-\alpha)q}\le(\int|f|^p)^{\alpha q/p}(\int|f|^r)^{(1-\alpha)q/r}$. Taking the $q$-th root gives $\lVert f\rVert_q\le\lVert f\rVert_p^{\alpha}\lVert f\rVert_r^{1-\alpha}$. Lastly, observe $x^{\alpha}y^{1-\alpha}\le\max(x,y)$ for $0\le\alpha\le1$.
22:09
@Alessandro see what exactly
well the proof is direct
i was hoping for something conceptually easier; the inequality seems like something explanatory
@Thorgott yeah
well $p,q,r$'s are switched
but yeah
up to conjugation of variable names
@Thorgott what does convexity mean
im making a list of all things banach; give me content
@BalarkaSen Look up interpolation techniques in L^p theory
22:16
I didn't mean convexity, I meant $L^q\supset L^p\cap L^r$ for $p<q<r$ (consequence of the above inequality)
time to terrytao.wordpress.com
But convexity is also a thing: $\lVert f\rVert_p^p$ is log-convex in $p$
@Thorgott Yeah OK
wait, inclusion is the wrong way round
yeah man its alright
human brain cannot understand inequalities according to Misha Gromov
22:19
give $L^p\cap L^r$ the norm "sum of $p$-norm + sum of $r$ norm", then the inclusion $L^p\cap L^r\rightarrow L^q$ is continuous
@MikeMiller Too dank, bookmarked. I'll read
I’m on mobile
you can read the chapter on $L^p$-spaces in Folland
lots of cool stuff in there
Too dank, bookmarked
Just tell me the important theorems and I'll prove them by myself
Only way to learn analysis
Yeah!^
22:25
time to learn about uniformly rotund Banach spaces
prove L^p is dual to L^q or sth
easy
already did
Yes! Banach spaces are what my professor studied
@BalarkaSen There are a lot of very cool posts there
I still have to read the one about Gromov's theorem
its hard to read because he goes off on so many tangents
analysis brain
22:28
prove Riesz-Thorin or whatever
Geocalc 🧠
No Thor
good decision
@BalarkaSen But he shows interesting connections with other stuff
lol does the proof use holomorphic functional calculus
@Alessandro its too much for my brain man i am a simple man i stick to one picture at a time
ok i have to sleep, be back tomorrow
22:32
gn
Have a good one
22:45
hi chat
Did you see my message ?
In a private room I made on this chat
I did not lol
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