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00:00
the parametrization definition is the odd one out
50 mins ago, by Balarka Sen
Like, take a loop and twiddleschloopkinfloop it to floop it all into $\Bbb R^n$ and slurpslorp
can't type
right, so we get $Df(\phi(x))D\phi(x)=0$, which we can write as $\nabla f(\phi(x))\cdot D\phi(x)$. So we see that all vectors of $D\phi(x)$ are perpendicular to the gradient of $f$ at a point of the manifold, and since they span the tangent space, we know that all those vectors are perpendicular to the gradient. Also, the inclusion goes both ways because of the dimensions
@BalarkaSen I feel like there's a 60% chance you actually had something in mind when you typed that ^
Akiva, that was us proving the fundamental group of $S^n$ is $\mathbb Z^n$
00:00
Superb, @Sha. Kudos.
I hope not, @GFaux.
@GFauxPas $\pi_1(S^n)=\Bbb Z^n$?
@GFauxPas $0$ you mean lol
that's...not good
00:01
@AkivaWeinberger I did
errr I was thinking $T^n$ sorry
sigh of relief
It was perturbing the loop a little to make it non surjective
Wait, no, relief is from topography, not topology
00:01
@BalarkaSen how u gonna do that on $S^1$
then bloop it floop
@0celo7 I wont
that's the $S^n$, $n\ge 2$ proof
not "the" but yes
The proof.
The only proof.
The proof to end all proofs
00:07
While I don't know how is power defined in "there exists to the power there exists to the power for all", googling "exponential logic" lead me to something called linear logic:
"as a refinement of classical and intuitionistic logic," immediately loses interest
LEM 4eva
00:25
Hi everyone! Can someone please explain the intuition behind the definition of the complex-valued function $g(z) = \frac{f(z) - f(a)}{z-a}$ for $z \not = a$ and $g(z) = f'(a)$ for $z = a$ where $f$ is an entire function. Bak and Newman use this function frequently throughout their text and show that the rectangle theorem (integral of a function $g(z)$ around the boundary of a rectangle $R$ and the closed curve theorem apply to $g$, later showing that if $f$ is analytic at $a$, then so is $g$).
It seems to me that as you take the limit as $z \to a$, then $g(z)$ is the definition of the complex derivative of $f$ at $a$; so are Bak and Newman using $g$ to show that the complex derivative of $f$ at any point where $f$ is analytic is also analytic and inherits all properties of the analytic functions?
What's the rectangle theorem?
Is it Cauchy's integral formula?
Bak and Newman define the rectangle theorem as if $f$ is entire and $\Gamma$ is the boundary of a rectangle $R$, then $\int_\Gamma f(z) dz = 0$.
Ah
$\Gamma$ doesn't need to be a rectangle, by the way, turns out
They'll probably prove that soon, 'cause it follows from the rectangle case
but $\Gamma$ can be any closed curve
I think they're gonna prove the Cauchy integral formula, then, assuming they haven't already
Right, I read that it can be a smooth closed curve! I guess I'm just a bit unsure of the motivation behind the definition of $g$!
Say $\gamma$ is some curve around $a$, and $f$ is analytic
00:33
pointwise smooth*
@GFauxPas We need that?
rectangle
I mean, can't it be any curve?
Co-shi's integral formula lets us define $f(a)$ in terms of an integral, which will turn out to be useful later (we can get bounds on the value of $f$ using it)
So let's say we know that $\dfrac{f(z)-f(a)}{z-a}$ is analytic
(defined to be $f'(a)$ at $a$)
well you want it to be differentiable with respect to the parameter so you can change of coordinates in the integral and therefore parameterization doesnt matter yadda yadda
Then $\displaystyle\int_\gamma\frac{f(z)-f(a)}{z-a}dz=0$
00:35
$f(\gamma)\gamma'$
But also we know the value of $\displaystyle\int_\gamma\frac1{z-a}dz$
Is $\gamma$ a clsoed curve around $a$? Then that would be $2\pi i$ right?
That's the derivative of $\ln(z-a)$, so we can try to use the Fundamental Theorem of Calculus. The natural logarithm can't be defined on the whole complex plane, but there's a way around that
and we end up with $2\pi i$ times the winding number of $\gamma$ around $a$
If it's just a counterclockwise circle then yeah it would be $2\pi i$.
Or any loop of winding number $1$.
So $\displaystyle\int_\gamma\frac{f(a)}{z-a}dz$ would be...
($f(a)$ is a constant)
$f(a)2\pi i$.
So we can take that $\displaystyle\int_\gamma\frac{f(z)-f(a)}{z-a}dz=0$ that we had earlier
and suddenly we realize we can do something to that, if we split up the fraction
$\displaystyle\int_\gamma\frac{f(z)}{z-a}dz=\int_\gamma\frac{f(a)}{z-a}dz=2\pi if(a)$
$\displaystyle\frac1{2\pi i}\int_\gamma\frac{f(z)}{z-a}dz=f(a)$
and now we have Cauchy's integral formula, a way to express $f(a)$ in terms of just the values of $f(z)$ on a loop around $a$.
Oh wow, I see the importance of the expression $\frac{f(z) - f(a)}{z-a}$ now.
It's kinda motivated by the result, tbh
00:42
Thanks Akiva!
We know $\displaystyle\int_\gamma\frac C{z-a}dz=0$ when $C$ is a constant, and we can wonder what happens when $C$ is a function
and we can make a conjecture, and then the expression helps us prove that conjecture
is kinda how I see it
Gotcha.
'Cause it turns out that $\dfrac{f(z)}{z-a}$ is just an analytic function away from something of the form $\dfrac C{z-a}$.
And so their integrals are the same.
@Poptart Here's a neat application of this
Say that $f$ is bounded
For example, let's say we know that $|f(z)|<1$ for all $z\in\Bbb C$.
Note that $\sin$ does not satisfy this!
$\sin(i)\approx1.17520$.
$\sin(iz)=i\sinh(z)$.
So, here's the question: Can we find any functions that actually do satisfy $|f(z)|<1$ for all $z$, real or complex?
Well, constant functions, for one. $f(z)=\frac12$ is a boring function, but it works. Are there any others?
We know that $\displaystyle\frac1{2\pi i}\int_\gamma\frac{f(z)}{z-a}dz=f(a)$.
$\operatorname{Arg}(z)$?
Analytic functions, I mean
00:48
;)
That's not even continuous!
And also, it goes from $-\pi/2$ to $\pi/2$...
Let me actually see if I can remember how to do this
Let $\gamma$ be a HUGE circle
omg so big circle
Let me first spell out an important consequence of this formula that I didn't mention before
$\displaystyle\frac1{2\pi i}\int_\gamma\frac{f(z)}{z-a}dz=f(a)$ means that, if we just know the values of $f$ at points on $\gamma$, we know the values of $f$ everywhere in $\gamma$
because we can just calculate them from the formula
(In fact, it will turn out that more is true, but I can't prove that now)
00:50
because holomorphic functions are ~magic~
^This is the main lesson from complex analysis
Analytic functions are magic
So, uh, say $\gamma$ is a circle of radius $R$ around $a$.
Wait
Akiva, you want to find $f'$
so differnetiate both sides wrt a
wait, is that right
you want $2 \pi i f' = \int f/(z-a)^2$ thing
I can do this another way, I think?
If I show that $f(a)-f(b)=0$ for all $a$ and $b$, I'm still good
and $\dfrac1{z-a}-\dfrac1{z-b}=\dfrac{a-b}{(z-a)(z-b)}$
And so $\displaystyle\frac1{2\pi i}\int_\gamma\frac{f(z)(a-b)}{(z-a)(z-b)}dz=f(a)-f(b)$ if $\gamma$ contains both $a$ and $b$
But this is more complicated than I originally thought it would be
I had forgotten the details
@Poptart When you see this: Sorry
Lemme finish this anyway
00:56
wikipedia/proofwiki lol
that's what I do
So $\gamma$ is a big circle around $a$ and $b$ of radius $R$
The left-hand-side, we know that the the integral of a function around a loop is at most the max value of the function times the length of the loop
If $|f|<M$ and $\ell(\gamma)=L$ then $|\int_\gamma f|\le LM$
There's a name for that, I forget it
@Daminark yo are you here?
But it's the important thing that makes Cauchy's formula useful here
@AkivaWeinberger basic L^\infinity estimate?
ncatlab.org/nlab/show/simple+object can someone give a simple counterexample to prop 2.1 when the field is not algebraically closed?
00:59
Rouche's Lemma or something?
wait no thats different
So $\displaystyle\int_\gamma\frac{f(z)(a-b)}{(z-a)(z-b)}dz\le\frac{1(a-b)}{{|z-a|}{‌​|z-b|}}\cdot2\pi R$
estimation lemma
'cause $|f(z)|\le1$ by hypothesis, and the length of $\gamma$ is $2\pi R$
and if $z$ is on the big circle, then $|z-a|\ge{}$uh, $R-|a|$ or something?
If $\gamma$ is centered around the origin, then sure, yeah
The point is, we're bounding this thing by something that's approximately $\dfrac{\rm constant}{R^2}\cdot{\rm constant}R$
which is approximately $\dfrac{\rm constant}R$
which goes to $0$ as $R$ goes to infinity
But $\displaystyle\frac1{2\pi i}\int_\gamma\frac{f(z)(a-b)}{(z-a)(z-b)}dz=f(a)-f(b)$
So as I make $\gamma$ bigger and bigger, the left-hand side goes to $0$
meaning the right-hand side, which doesn't change with $\gamma$, has to equal $0$ the whole time
which means $f$ is constant
so boom
@Daminark I have some crap complex analysis that I'm stuck on
Also, I could have started this with $|f(z)|\le M$ instead of${}\le1$
so all bounded analytic functions are constant
Why? 'Cause we can write them as an integral, and then we can show that the integral can't go big enough
I have no intuition for this fact that doesn't go through the Cauchy integral formula
So the Cauchy integral formula lets us prove magic
01:10
Are $a$ and $b$ two arbitrary points contained in the region contained in $\gamma$?
Two arbitrary points... at all
$\gamma$ is a big circle containing $a$ and $b$
We want to prove that, for any $a$ and $b$, we have $f(a)=f(b)$
Oh i see! that's a cool result!
@AkivaWeinberger thank you again :)
There's another way, where instead of trying to show $f(a)-f(b)=0$ for all $a$ and $b$, you try to show $f'(a)=0$ for all $a$. But for that you need a different result, namely $\displaystyle\frac1{2\pi i}\int_\gamma\frac{f(z)}{(z-a)^2}dz=f'(a)$.
yeah that's the way I was thinking of Akiva
Which your book will probably prove soon.
But it's probably annoying proving a second integral identity (even if it follows from the first)
You can get it by differentiating both sides of Cauchy's integral formula with respect to $a$, but I was worried about the rigor
01:15
you need to show you're allowed to do $\mathrm d \int = \int \partial$
or, alternatively, that the thing minus the other thing goes to 0 in modulus, which is probably easier
Or consider the definition of the derivative, and replace each instance of $f$ in it with a whole integral
It's doable
You actually can get a formula for $f''$, $f'''$, etc., also
In fact, it turns out you can use the integral formula to prove that those all exist
All analytic functions are infinitely differentiable
In other words, if a function in the complex plane can be differentiated once, it can be differentiated infinitely many times
which is very not true for functions on the real line
So that follows from the integral formula as well
Again, analytic functions are magic
that's just elliptic regularity theory
Also, all analytic functions have antiderivatives
Also, all holomorphic functions are analytic
meaning that theyre equal to their power series
01:20
(Well, $\frac1z$ is defined on $\Bbb C\setminus\{0\}$, and it doesn't have an antiderivative defined on $\Bbb C\setminus\{0\}$.
because it'
But if something's defined on $\Bbb C$, it has an antiderivative defined on $\Bbb C$.)
s not holomorphic on any nbhd of 0
(And that integral is analytic. So you can integrate it infinitely many times also.)
@AkivaWeinberger You mean functions defined in simply connected domains have primitives.
01:21
Right, you can strengthen it to that
Simply connected means it doesn't have holes, and primitive is a synonym for antiderivative
01:45
Hi all. I am tasked with writing $\sum_{i, \space j, \space k \space distinct} x_i^2x_j^2x_k^2$ as an elementary symmetric polynomial. Any ideas?
In other words, I want to write this thing in terms of $s_1 = \sum x_i, \space ... \space s_n = \sum x_1 \cdot \cdot \cdot x_n$
02:01
Proof that part of higher mathematics is salesmanship:
in Homotopy Theory, Apr 23 at 1:20, by Tyler Lawson
writing that out, i feel like i may have tried to make this sales job to the chatroom before
In mathematics, an ordinary differential equation of the form: y ′ + P ( x ) y = Q ( x ) y n {\displaystyle y'+P(x)y=Q(x)y^{n}\,} is called a Bernoulli differential equation where n {\displaystyle n} is any real number and n ≠ 0 {\displaystyle n\neq 0} and ...
Lol Bernoulli diff eq, i remember those days....
02:25
@NicholasRoberts If you get rid of the "distinct" bit, it becomes $(\sum_i x_i^2)^3$
So from that you have to subtract out things where two are equal
and add back some thing where all three are equal probably? Maybe with some constant in front
Ok so youre saying to start with the sum of (x_i)^2 and then try and subtract things to get the result
seems like a lot of trial and error, but i'll try
I would write it out with some example (i.e. $n=3$)
@NicholasRoberts I don't have a better idea at the moment
Ya but n = 3 its already a symmetric polynomial
its simply s_3
02:27
5, then, I guess?
This all sounds annoying
Yeah i suppose. LOL yes it is very annoying
but if you write it out neatly maybe you'll get ideas for less annoying things
02:59
I'm stumped on this geometry problem

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