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3:06 PM
On a partially related note, for a given function $f:\Bbb C\rightarrow\Bbb C$, one can define several $F$ such that $F^\prime(z)=f(z)$, correct?
 
@LegionMammal978 Do you know what the derivative of a constant is? :)
 
Upto a constant (like Danu is telling you) it is, however, unique.
 
hi there, would someone be willing to help me with a quick math query?
 
@LegionMammal978 I assume that simplifies to $\sqrt{x^2}$?
without going through it
where $x^2$ is rendered as $\exp(2\log(x))$ and $\sqrt x$ is rendered as $\exp(\log(x)/2)$
and where division ($x/y$) is rendered as $\exp(\log(x)-\log(y))$, etc. etc.
@MeowMix What's the problem?
 
3:24 PM
Given three points in the plane, find the point which minimizes the sum of the distance from each point to that point
 
I need to find a sequence such that $a_{n}$ converges, $b_{n}$ is bounded, and $a_{n}b_{n}$ diverges. I chose $a_{n}=\frac{1}{n}$ and $b_{n}=(-1)^n\cdot n$. Is that correct?
 
By the way, In $\Bbb R^3$, the set of points such that that sum is fixed would make an ellipsoid, right?
 
@mrnovice Your $b_n$ doesn't look bounded to me
 
I don't think so. Ellipsoid is set of points with fixed total distance from two points, right?
Foci.
 
Oh, I tried to generalize it wrong-ly
 
3:26 PM
@BalarkaSen That would specifically be an ellipsoid of revolution, though, wouldn't it?
 
I think in general it's gonna be a cubic.
 
What would 3 points make then? 1 point makes a circle, 2 makes an ellipse
 
@Akiva Weinberger I thought it was bounded since $|b_{n}| =1$?
 
It would have rotational symmetry around the line through the points.
 
line?
 
3:26 PM
@AkivaWeinberger Don't remember what that is.
Yeah, I suppose.
 
@mrnovice $|b_n|=|(-1)^n\cdot n|=|(-1)^n|\cdot|n|=1\cdot|n|=|n|$
@BalarkaSen I just meant an ellipsoid that's also a solid of revolution.
 
@MeowMix Line through the foci.
 
@AkivaWeinberger Ah yes my mistake, thanks
 
@Akiva Sure. Didn't remember things other than that were called an ellipsoid too.
 
@AkivaWeinberger Here's my analysis question, also
 
3:28 PM
But of course cross sections can be ellipse with varying eccentricity
 
$(x/a)^2+(y/b)^2+(z/c)^2=1$
 
Assume you know $f(x)$ is continuous, but you're only given it on some interval, minus finitely many singletons
 
except in this case, two of $a,b,c$ are equal
 
Gotcha.
 
Can you find out the function?
Similarly, say you're given the function on $[0,1] \setminus \{1, 1/2, 1/3, \dots \}$
Can you uniquely determine it on $[0,1]$?
 
3:30 PM
It need not extend to a continuous function on $[0, 1]$. Are you assuming it does?
 
I was just asking.
Like, it seems if say, you're given $f(x)=x^2$ on $[-1,1]$ except at $x=0$
 
? I am asking you what your hypothesis is. $f$ is continuous on $[0, 1] - S$ where $S$ is a bunch of points. Is $f$ also continuous on $[0, 1]$?
Otherwise it won't extend!
 
Oh, sorry. Yes.
 
If it extends, it extends uniquely, if that's what you're asking
 
Right.
 
3:31 PM
But what about the case listed above?
 
Still true.
 
Does it still hold?
Is there some criterion that needs to hold here?
 
Extend it on each $\{1, 1/2, \cdots, 1/n\}$ uniquely, for all $n$.
 
As long as the set of points where you don't know it has "empty interior" (each point is the limit of things outside of the set), you can extend it
 
Criterion for the set we're removing, I mean.
Oh, empty interior, that's right.
 
3:33 PM
So, like, $S=\{1,1/2,1/3,\dots\}$ has empty interior in $[0,1]$, Since each point in $S$ can be approached by things in $[0,1]\setminus S$.
Same for $T:=S\cup\{0\}$.
 
So like, every point in our set has to be a limit point in $R - S$?
Or am I interpreting this wrong.
 
@MeowMix Yeah
 
Cool :P
In $\Bbb C$ I'm pretty sure the requirement of holomorphicity is really strict
 
Although, here's a question: Suppose $f$ is continuous and defined on $[0,1]\cup\{2\}$.
 
Yes, it is.
 
3:35 PM
And we only know its values on $[0,1]$.
 
Can't you like define it (Assuming it's holomorphic on a disk) on the boundary of a disk and get it defined for the whole disk?
 
Can we uniquely recover the original function?
 
I'm pretty sure not.
 
Oh, wait.
Yeah
You can't
 
3:36 PM
The function will be continuous no matter what you define $f(2)$ to be
This means that $\{2\}$ (which has empty interior in, say, $\Bbb R$) doesn't have empty interior in $[0,1]\cup\{2\}$.
So we care what the surrounding space is.
 
@MeowMix Again, is that what you meant to ask? $f$ can be holomorphic inside the disk and still have singularities on the boundary of the disk.
 
By holomorphic on, I mean, the whole closed disk
 
$1/(z - 1)$, and the disk is the interior of the unit disk.
 
Like, the disk is closed.
 
@MeowMix That doesn't make sense, sorry. Holomorphicity is defined only on the interior.
 
3:39 PM
Oh, you're right.
 
But you probably mean it doesn't have singularities on the boundary?
 
Yeah
 
Holomorphic on the interior and defined/nonsingular on the closure
You can use Cauchy's formula to recover the values on the interior if you only know the values on the boundary, right?
assuming it's holomorphic
 
For sure.
 
Yeah, that was the question I asked as well.
 
3:41 PM
I think if you're defined on the boundary you can analytically continue it on a bigger disk containing the closed disk.
 
This doesn't mean that every continuous function defined on $S^1$ can be extended to a homolorphic function on $D^2$
 
Kind of like analytic continuation, because analytic and holomorphic are the same thing in $\Bbb C$ right?
 
@AkivaWeinberger Not true. $\bar{z}$.
 
I said it doesn't mean it can be extended
 
@AkivaWeinberger $S^1$ is the unit circle and $D^2$ is the unit disk right?
 
3:42 PM
Yeah
 
By the way, isn't $\bar{z}$ not holomorphic or sommething?
 
@Akiva You originally started with "Doesn't", which was a bit confusing. I agree.
 
@MeowMix Right
 
However, you can give a pretty strong condition on your function on $S^1$ (harmonic) and the extension problem is a deep problem in analysis. Also known as the Laplace boundary value problem.
 
Why?
 
3:43 PM
Cauchy-Riemann
 
Try differentiating it with the definition
(or that^^)
 
Aren't you just flipping the plane over the real axis?
 
You know how "differentiable" on $\Bbb R$ means "if you zoom in, it'll look like a line"?
On $\Bbb C$, it's essentially the same thing; "if you zoom in, it'll look like a linear function"
Linear functions are like $z\mapsto az+b$.
There's no place on $\bar z$ where you can zoom in and have it look like something of the form $az+b$.
 
@MeowMix Yes, but that means the derivative (at 0, say) along the imaginary axis is negative and the derivative along the real axis is positive.
 
It "flips orientation" in a way that $az+b$ does not, if that makes sense.
 
3:45 PM
Whereas holomorphicity means you have to have all derivatives from all directions the same.
 
That's extremely weird...
I mean, it makes sense.
 
It's a strong condition. (x, y) mapsto (x, -y) is differentiable as a multivariable function, but is not holomorphic.
You essentially want everything to be "like" polynomials like Akiva said
That's why complex analysis is so rigid
 
Oh, and that's related to analytic-ness?
 
You can say that
 
On the other hand, if I have this right, things that are differentiable as multivariable functions will look like something like $az+b\bar z+c$ when you zoom in.
Which is more general.
 
3:49 PM
Nice perspective. It's right, of course.
 
And this is related to the concept of Wirtinger derivatives, which are written like $\dfrac\partial{\partial z}$ and $\dfrac\partial{\partial\bar z}$.
Which I assume would give you $a$ and $b$, respectively (from the $az+b\bar z+c$ thing).
 
4:20 PM
Let $E=\{(x,y,z\in\mathbb R^3:x>0,y>0,z>0\}$ and $f\colon E\to\mathbb R$ given by $f(x,y,z)=x^yy^zz^x$. Compute the partial derivatives of $f$.
It suffices to compute only the first derivative of $f$. I started as follows:
\begin{align}D_1f(\vec x)&=\lim_{h\to0}\frac{f(\vec x-h\vec e_1)-f(\vec x)}{h}\\
&=\lim_{h\to0}\frac{((x-h)^y,y^z,z^{x-h})-(x^y,y^z,z^x)}{h}\\
&=\lim_{h\to0}\left(\frac{(x-h)^y-x^y}{h},0,\frac{z^{x-h}-z^x}{h}\right).\end{align}
However, I don't know if I can continue from here on. Is there anything elke I could do?
Or should I maybe not use the definition and work with "regular" differentiation?
oh wait, I see I messed up badly too
I should have written:
\begin{align}
D_1f(\vec x)&=\lim_{h\to0}\frac{f(\vec x-h\vec e_1)-f(\vec x)}{h}\\
&=\lim_{h\to0}\frac{(x-h)^yy^zx^{x-h}-x^yy^zz^x}{h}.
\end{align}
I'm guessing the answer is this:
$$D_1f(\vec x)=\frac{\partial f(\vec x)}{\partial x}=yx^{y-1}y^zz^x+x^yy^zz^x\ln x.$$
 
4:46 PM
hi @arctictern do you know a good book along with Gelfand homological algebra as reference ?
for homological algebra ?
 
5:01 PM
Everything is easier with matrices
 
@Secret Isn't that mixed derivatives (of a multivariable function), rather than Taylor series?
 
You use them for multivariable Taylor series
 
Well, that matrix just makes it easier to keep track of what derivatives I have computed for the taylor series
I tend to miscount things when they are presented horizontally
This is why I don't like polynomial expansion
 
5:17 PM
@MikeMiller I was wondering can we define homology theory in terms of non-abelian groups ?
 
You can define $H_1(X;G)$ when $G$ is non-abelian. You can't do $H_k$ for $k>1$.
Can you? I guess I know you can define $H^1(X;G)$.
 
why can't we do it for higher homologies ?
 
What happens if you try?
 
oh I see we get this issue with it not being necessarily a group
hm is there some variation for homology theory for non-commutative things ?
It seems that a non-commutative homology theory would be very useful
 
5:36 PM
I remember you guys telling me once that it had to be an abelian category
(not that I fully know what those are)
 
it's essentially a category where you can take derived functors. you should read the construction of Ext and Tor in Hatcher
chapter 3
 
@AkivaWeinberger Abelian category you can think of it as generalization of abelian objects modules,abelian groups,etc
@AkivaWeinberger I don't recommend hatcher
Try Methods of homological Algebra by YU.I.Manin
 
he doesn't need to learn all of homological algebra to understand abelian categories, assuming he's not going to get to technicalities in the first dip
"generalization of abelian modules, abelian groups" is also a rather uninspiring description
 
no there is section on abelian category on that book which is short
It covers it better than Hatcher
 
Hatcher doesn't cover abelian category....
i just told him to learn the defn of Ext and Tor from Hatcher.
 
5:43 PM
oh okay
 
@Danu Sorry, the question I had in mind was: How would one determine a specific value of the antiderivative (ignoring the constant of integration for now) on the complex plane? It can be done easily enough on the real line with $F(x)=\int_a^xf(x)\,\mathrm dx$, etc. but I can't figure out any of this contour craziness.
 
@LegionMammal978 It's the same idea in complex analysis. If $f$ is holomorphic on a neighborhood of $0$, you write $F(a) = \int_\gamma f(z) dz$ where $\gamma$ is an oriented path going from $0$ to $a$ given by moving from $0$ to $\Re[a]$ along the real axis, and then moving from $\Re[a]$ to $a$ along the imaginary axis.
You can prove $F'(z) = f(z)$ by using the Goursat's theorem (integral of hol. function along triangles are zero) - which is a version of Cauchy's theorem.
 
@BalarkaSen "Holomorphic on a neighborhood of $0$?" Sorry, never been real good with this terminology
 
Look in Stein-Shakarchi for details.
@LegionMammal978 Holomorphic on a open disk containing $0$. Just assume holomorphic on $\Bbb C$ if you want
 
Also, what are you denoting by $\Re[a]$?
 
5:52 PM
Real part....
 
Oh, okay :P
 
I have to go for now. See ya
 
Oh, okay, "holomorphic" basically means "differentiable"
 
But be careful
Like @Balarka said, it's much stronger of a condition than, say, multivariable differentiability
 
As in...?
 
5:57 PM
@Adeek When you write down $\partial^2$ and your coefficients are nonabelian, $\partial^2 \neq 0$. So you're screwed.
 
Huh, it also ensures that it's analytic
Will only really be taking these for elementary (or, more accurately, Liouvillian) functions anyway in my use case
 
yeah I see @MikeMiller
 
i have a function $f:\mathbb{R}_+\rightarrow \mathbb{R}_+$ increasing such that $f(0)=0$ and for all $s,t\in\mathbb{R)_+, f(s+t)\leq f(s)+f(t)$ please if $f(x)=0$ can we deduce that $x=0$ ?
 
@Vrouvrou Isn't $0\not\in\Bbb R_+$?
 
$\mathbb{R}_+=[0,+\infty[$ and $\mathbb{R}_+^*=]0,+\infty[$
 
6:06 PM
ah, okay
Is $f$ strictly increasing, or no?
 
no just increasing
 
In that case, wouldn't $f(x)=0$ for all $x$ be a simple counterexample?
 
yes
 
So no, we cannot in general deduce that $x=0$
 
there is a question suppose that there existe $s>0$ such that $f(s)=0$ how to schow that $f$ vanish on $\mathbb{R}_+$
@LegionMammal978 please if we suppose that $f$ does not vanish if f(x)=0 can we deduce that x=0 ?
someone here ?
?????
@AlessandroCodenotti hello
 
6:29 PM
Hello everyone
this is something I have been stuck with for a while
I want to calculate the covariance
not in advance, but as the data is coming in...
So if at T1 x1 enters the system cov1 should be calculated
at T2 x2 cov2 should be calculated (without having to save in memory x1!)
some sort of moving covariance
Any suggestions?
 
Hmm
I figured out an O(1) moving standard deviation once
You just have to save the sum of the elements and the sum of their squares
 
@MikeMiller have you read homological algebra by Gelfand before ?
Methods of homological algebra *
 
@LegionMammal978 yes but I only have 1 element at a time
and need to have a covariance immediately
 
@trilolil O(0) isn't necessarily possible
 
Sorry?
 
6:39 PM
As in, you can't calculate anything "immediately"
 
6:50 PM
@Adeek Nope.
 
hello, can someone help me on my question ?
 
7:05 PM
vrom vrom
 
7:28 PM
immediately as in atomicly?
 
what?
 
Hi @Meow
 
Hi @Balarka
 
yawn I give up trying to numerically approximate values of the complex antiderivative
Nothing I'm doing is working
 
hello
 
7:46 PM
hi balarka
hi meow
 
@BalarkaSen Did you see the drawing of homer simpson using Fourier Series?
And they showed it as like circles rotating around circles rotating around circles rotating around ...
 
Hi anyone familiar with spinor bundles?
 
what's homer simpson
 
Meow Mix are you really middle school student
 
7:49 PM
Yes.
 
impressive
 
@MeowMix neat
i guess
 
@BalarkaSen I might try creating one of those lol
All I'd have to do is just draw it out as one continuous curve, create functions for the x and y then approximate them with fourier series?
 
something like that
 
Is there a theorem analogous to Weierstrass Approximation for Fourier Series?
Like, fourier series are dense in the set of continuous functions on some interval?
 
7:55 PM
Yes. Sufficiently nice periodic functions are approximated (in some appropriate norm) by partial sums of their Fourier series.
It's a subtle topic, so I don't know much about it.
I think it's analogous to the proof of Weierstrass using approximate identities for C^1 functions on the circle with uniform norm.
 
Interesting.
 
@MeowMix There's a chapter in Ted's notes, and a whole lecture he devotes to them, where he described this as a sort of orthogonal projection thing on towers of subspaces spanned by $1,\sin(kx), \cos(kx)$ (n = 1, 2, ..., N), in the vector space of C^1 functions on [0, 1] say.
It explains the intuition behind why it "should" happen nicely.
 
Every function in $L^2(-\pi,\pi)$ has a converging Fourier series
 
@Alessandro There are C^0 counterexamples, IIRC?
 

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