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00:00 - 10:0010:00 - 00:00

00:44
Any last minute GRE tips?
are there any useful bounds on the Trace$(A^2)$ in terms of Trace($A)$
01:17
can't be, @Lepidop
Hi, @Ted!
((Fargle))
How're you?
doing pretty well, and how 'bout you?
I'm alright. School continues, haha.
01:18
Still too easy for you, of course
Well, it's just probability and numerical analysis. A strain on the memory, but not much else. And my numerical professor is really good at explaining stuff simply.
That's good ... Well, if you're too bored, get back to the stuff I told you to work on and work with me :P
Haha, of course. I'm actually having an attack of boredom at the moment. I may take a look at that.
Is your health good?
Also, one of my professors gave me a researchable question that I'm looking into.
Yes, I'd say so.
01:20
ok, good
ditto
Good!
Hi @TedShifrin
well, I'm happy to challenge you more, @Fargle
heya mr eyeglasses
I'm always happy to be challenged.
Hi professor
01:22
rehi @skull
anything to report of a positive nature, mr eyeglasses?
um ... so I guess not
We know that vectors in $\mathbb{C}^n$ are ordered n tuples in that $$(a,b,c)\neq (b,a,c)$$

Matrices as elements in a vector space seemed to also have some kind of ordered structure since
$$\begin{pmatrix}a & b \\ c & d\end{pmatrix}\neq\begin{pmatrix}c & d \\ a & b\end{pmatrix}\neq \begin{pmatrix}b & a \\ d & c\end{pmatrix}$$

If we don't think of matrices as made of column vectors, then how mathematically is this order structure is being introduced?
You just arbitrarily pick an order, @Secret. Say column by column or row by row.
@TedShifrin
hi @Karim
I am trying to show that $|cos(z)| \leq e$
01:29
Well, that would be very false, @Karim.
when $|z| = 1$
sorry
Maybe believable now.
$coz(z) = \frac{1}{2} * (e^{iz} + e^{-iz})$
ok, so?
so $|cos(z)| = |\frac{1}{2}e^{iz} + e^{-iz}| \leq 1/2|e^{iz}| + 1/2|e^{-iz}|$
by triangle inequality
01:31
No, you threw away too much
?
I didn't distribute the 1/2
in first line
Well, ok, that actually does it.
but second line is right
but why is $|1/2e^{iz}|$ = 1/2e ?
And what about $|e^{iz}|$?
It isn't.
Just write things out carefully, for once.
is it true that $|e^{iz}| = e^{|z|}$?
01:33
NO!
Write it out carefully, for once.
Goodnight @MikeM
$e^{iz} = e^{x + iy} = e^x(cos(y) + isin(y))$
No, @Karim.
You dropped the $i$.
Morning.
01:34
Hi Mike
I didn't
where?
hi @Karl
<--- getting annoyed by sloppiness
01:35
Some staff are digging around in the ceiling above me which is not exactly a good environment to meet a student in.
though |z|=1 iff |iz|=1
hey @Ted
But $|z|$ is irrelephant.
$e^{iz} = e^{i(x + iy)} = e^{ix - y} = e^{-y} *(cos(x) + isin(x))$
right?
Meh, not paying close enough attention to argue
OK, @Karim, but if you're going with modulus, then $|e^{ix-y}| = |e^{ix}||e^{-y}|= e^{-y}$.
01:36
yes
yes since it has modulus 1
I mean $|e^{ix}| = 1$ because $|z| = 1$
NO. $|e^{ix}|=1$ always when $x\in\Bbb R$.
You really need to pay attention to detail.
ohh I see
You should be able to finish correctly now.
Dinnertime for this bonzo.
01:42
why is it true that $\frac{1}{2}e^{-y} + \frac{1}{2}e^{y} \leq e$?
Ignores both parts
?
I am using latex
The sticky-star wore out, presumably.
@KarimMansour why do you think that's true? are you sure you've typed it correctly?
the LHS is unbounded
01:46
hm
y is bounded in this problem
what kind of y are we talking about then?
oh I see so here since we know that |z| = 1
z=x+iy and |z|=1
How do I get started learning PDE?
01:48
What's your background?
I still don't see the last step
Well, what interval must $y$ lie in?
@MikeMiller I know analysis from Folland's book and some Riemannian Geometry
it must lie in [0,1]
01:50
why we have the modulus
visualize the locus of $|z|=1$
the points will lie on a circle of radius 1
@Memeozuki: I guess I'm not comfortable saying where you should start. The standard PDE text is Evans. You should probably be comfortable with measure theory and Fourier theory (know a bit about the Fourier transform).
in the x,y-plane @Karim
01:52
Probably there is a lot more to suggest being comfortable with but these are the obvious things to me.
Don't forget boundary value problems :-)
@MikeMiller
Are there any tips for getting better at digesting really technical information. A lot of times I read estimate arguments and I just can't pierce through them.
I am not sure @KarlKronenfeld
No one is... OH right, the |cos(z)| question. What aren't you sure about?
This is something that comes with practice. (I know the feeling.) Most of these technical arguments have a main thrust - some "real idea", where the rest of it was standard manipulations. Try to find this real idea in everything you read, @Memeozuki, whether it be analysis or otherwise.
4
(This is true for most theorems in textbook mathematics. When you start reading papers things are a bit less polished and it's often harder to find this central thrust.)
01:59
if we look at the x,y plane we see that the points that have modulus 1 will be exactly the points that lie on the circle of radius 1
so
it means
One thing is that for a lot of estimates they look so ugly to me I'm not sure how somebody could ever guess for it to look like that. Is that something that's picked up over time?
it is either in
[0,1]
or
[0,-1]
right ?
uh huh, so just [-1,1]
@Memeozuki: Yes, very much so. Stick with it. (Make sure to do lots of exercises so you're doing these ugly estimates yourself.)
02:01
This is true again for every field of math. Lots of things that seem very unnatural become "the obvious idea" to someone who's been embroiled in it for a while.
well let us look at the negative part
ok ok
I get it
thanks alot @KarlKronenfeld
Ok, thanks a lot. I'll stick with it.
@KarlKronenfeld sorry I have one quick question
about something else in complex analysis
ok, if I can't answer it, surely somebody else can
02:04
Hello!
Hi @SanicHodgeheg
consider the following integral $\int_{\tau}cos(cos(sin(z))) dz$, where $\tau$ is given by $\tau(t) = e^{it}$, for $0 \leq t \leq \pi$ and by $\tau(t) = e^{-it}$ for $\pi \leq t \leq 2\pi$
@Memeozuki: I know the frustration; I used to feel the same way. Now I study a part of math which is very firmly analytic (before first thinking I was going to be an algebraist because I couldn't deal with all these inequalities :P )
so the first one is a circle that goes counter clockwise
from 0 to pi
the second one is a clock wise curve that goes from $2\pi$ to $\pi$
I was thinking to use cauchy integral formula
but its not a closed path
since we don't return to our initial point right ?
02:07
@MikeMiller That's very encouraging. I really want to learn about geometric analysis and PDE.
actually no
we do right ?
can you explain in words what the path is Karim?
ok so for first path its easy to describe
we go trace a curve from $0$ to $\pi$ that goes counterclockwise
right ?
@Memeozuki Very cool. (I study gauge theory, which is related to geometric analysis. Lots of the PDE involved is more classical though, much of it being elliptic PDE. I stay mostly in that realm, though some people do gauge theory with some parabolic PDEs.)
do you agree ?
02:09
yes
well, from 1 to -1 on the unit circle is what you mean
Ah, awesome. It seems like the geometric evolution equations that I've seen are parabolic but I'll learn more about what I want to do as I learn more PDE things.
now for the second path we go from $2\pi$ to $\pi$ but instead of going counter clockwise we go clockwise
since we added the negative
I am sorry
I meant to say
For the second path we start at $\pi$ and then we go back to $2\pi$ and we go clockwise, so we do indeed go to our initial spot, so we can use cauchy integral theorem.
correct @anon?
pi and 2pi are not points on the circle. refer to points on the circle.
oh ok
yesss
02:12
@Memeozuki: I think pretty much all modern study is on parabolic and hyperbolic PDE. The elliptic equations are the easy stuff.
I guess one way to do it is to directly compute stuff
I gotta go for now. Good luck!
$\tau(2\pi) = cos(2\pi) - isin(2\pi) = 1$, while $\tau(0) = 1$
so it is indeed a closed path
here is what I was looking for: tau goes from +1 to -1 around the unit circle counterclockwise, then goes back from -1 to +1 around the unit circle clockwise.
02:17
in real variable calculus, do you know the relationship between $\int_a^b f(x)dx$ and $\int_b^a f(x) dx$? One goes on a path from $a$ to $b$, the other on a path from $b$ to $a$.
it is the negative
going from a to b is the negative of going from b to a
so what do you think will happen with your integral if you split it into two parts, each integral over the same path but in opposite directions?
they will evaluate to zero
try it and see what happens
02:34
yeah
it evaluates to zero
is it true that $|\int_{\tau}f(z)| \leq \int_{\tau}|f(z)|$?
yes
well, you have to write it correctly
$\int_\tau |f(z)|dz$ needn't even be a real number
one should write $\int_\tau |f(z)dz|$ (can you interpret that?)
ohh I see
coz I am using the problem I solved before to show that $|\int_{\tau} cos(z) /z dz| \leq 2\pi*e$
$|\int_\gamma f(z)dz|$ is bounded by ${\rm len}(\gamma)\cdot \sup_\gamma |f(z)|$
$|\int_{\tau} \frac{cos(z)}{z} dz| \leq \int_{\tau} |\frac{cos(z)}{z}dz| $
$\leq \int_{\tau} \frac{e}{|z|}|dz| \leq e * 2\pi$
right ?
@anon ?
no wait I think that last line is wrong
 
3 hours later…
Huy
Huy
05:27
@KarimMansour: are you in $\mathbb{R}$ or $\mathbb{C}$?
Huy
Huy
@KarimMansour: how do you get $\cos(z) \leq e$?
(or was your idea something different from the first to the second line?)
$|cos(z)| \leq e$
@Huy I made a mistake
Huy
Huy
@KarimMansour: for which $z$?
for |z| = 1
Huy
Huy
05:30
ah
05:52
someone will discuss functional analysis things with me?
Weak convergence of $A_n\rightharpoonup A$ means $\forall x\in X, \forall f\in X^*, f(A_nx)\to f(Ax)$
06:30
why does people call the norm a function? isn't it a functional since it maps from the linear space to the scalar field?
again this one is just like one before "expanding a non-periodic" function (even and odd) , Can anyone help me to confirm my solution(?) :
0
Q: Expanding Fourier Series of $f(x)=x^2$ where $0<x<1$ (even and odd)

sajjadI tried to solve Fourier series (which appeared on title) and ended up to below solution : on even state : $ \phi(x)= \begin{cases} x^2 & 0<x<1 \\ x^2 & -1<x<0 \end{cases} $ $a_{0}=\dfrac{2}{3}$ and also $a_{n}=\dfrac{4(-1)^n}{n^2\pi^2}$ on odd state I reached below answer : $ \phi(x)= \be...

06:53
Figured the topology problem I gave you, @JulianRachman?
07:34
Sorry haven't had time @BalarkaSen can yoi give me a jist because I am really busy right at this moment
07:47
@JulianRachman What do you mean by "gist"?
The problem was to show that $\Bbb R$ and $\Bbb R^2$ are not homeomorphic, both given the standard topology.
user61230
08:02
Anyone here have a moment to help with a hopefully straightforward covariant derivative question?
Sorry autocorrect. @Balarka
user61230
I'm trying to show that, supposing $W$ has $||W||=C$ (constant), then $(\forall V)(\nabla_VW\perp W)$.
@JulianRachman Then what did you mean?
user61230
I have a vague intuitive understanding of why this should be, but I'm not sure how to approach proving it. I've started with $(\nabla_VW)\cdot W=\sum V[w_i]w_iU_i$, but I'm not sure how to show this quantity is zero (or even if this is the right approach).
08:06
Yeah, I guessed, but gist of what?
@Emrakul Take the inner product of $W$ with itself and differentiate
The solution
user61230
...that is glaringly obvious in retrospect. Thank you, @Tobias!
@Emrakul I only knew how to do it because I happened to have done a similar exercise (like 10 years ago)
@JulianRachman Are you sure? It has a one-line solution.
There is a trick involved, but I guess you need to do some thinking for that.
08:09
@BalarkaSen And the trick involved is one that it useful for a large number of exercises on showing spaces not to be homeomorphic
Right.
(especially subspaces of the reals and the plane)
I just need time to do everything wnat first
user61230
Glorious. That's a nifty little proof.
@TobiasKildetoft I gave it to Julian because essentially the solution comes from looking at $\pi_0$. This generalizes to $\Bbb R^m$ and $\Bbb R^n$ where one looks at $\pi_k$ for higher $k$'s instead.
So it's a neat introduction to the concepts of algebraic topology, I think.
One can explain why $\pi_1$ is interesting/relevant by looking at the case $m = 1$, $n = 2$.
That provides some motivation.
08:15
Ya well Ted has been telling me to focus on the basics and not care about other stuff yet
He's quite right.
And is Munkres the best text for Algebraic Topology?
"best" of course not. It's good as an introduction, in my opinion.
and how about your situation? Arent you the same age as me?
Yes. What about my situation?
08:17
then what is the strongest base introduction and what is the best structure book to completely read out of
Well you are like so good and trail right behind you... gg
@JulianRachman What do you mean by "strongest base introduction" and "best structure book"?
I have read algebraic topology from 2 book - Munkres and Hatcher. Hatcher is just too hard for beginners.
Ok that is all I need
@JulianRachman Well, I'm studying the basics too.
I could read and understand algebraic topology because (I think) I have a firm background on some algebra and topology. But I am lacking on analysis.
So, e.g., if I want to read about differential topology, I'm going to have to learn multivariable calc. That's what I am doing right now.
08:20
I am learning multivariable next year as a formal class
in college classroom
Cool. :)
so that is covered
and I think you also have more background on real analysis than me?
I think I going to read munkres part 2 right after I finish homework then do a few problems from my problem set
ya I technically do
I studied it for a year before topology
If you want. But do this $\Bbb R$ and $\Bbb R^2$ problem first.
08:22
Ok
@JulianRachman Yeah, I thought so. You know measure theory?
Because I don't know anything about it.
Not familiar with it however it was mentioned in my text for real analysis
I attended a lecture in ergodic theory but came out confused. They're applying so much real analysis to prove completely number theoretic things.
Oh my.
that must suck because you sit there not knowing what or how to do anything
well, not completely. I understood what the statement and the theorems are. I just don't have enough background to understand the proofs.
The point of being in lectures is to get an idea of which branch you would want to study, really :P
08:25
@JulianRachman That is the default state of about half the audience at most seminars
Ah I see. Honestly so far for me I just love category theory. I want find that gap in the spectrum where category theory could change it all
lol I want to attend some seminars
I think I might try some at UCLA
@JulianRachman Then do so, they are usually open
I don't see the point of studying category theory for the sake of it, as I had said earlier.
do you guys take notes
?
In the seminars I mean
08:27
In lectures? Yes.
@JulianRachman Sometimes, though not that often
I am not learning it just for the sake of it. I want to apply it to some other mathematics discipline
Most of the time, things go the other way around. You learn some branch where some ideas of category theory are introduced, and you pick them up along the way.
and ya. I would figure that it would be pretty hard to take notes during a seminar that like 3/5 of you don't understand
That's how I learnt the category theory I know, from studying algebraic topology.
08:29
ok
Well it is also a huge part of algebra, then like homology theory, homotopy theory, etc.
@JulianRachman But if you have the notes with you, then you can come back to it later on to see which things you need to study to do understand it.
ok i see
@JulianRachman It's not a part of any three of the things you mention. In homology theory, one studies homological algebra - this might be categorical, but is a far-reaching branch of math. I don't know what kind of algebra you have in mind when you say that.
@BalarkaSen homological algebra is best understood in the language of category theory
In homotopy theory (something I don't know much), they do have an abstract setting, or so I have heard. But that has concrete applications, like computing homotopy groups of spheres.
08:31
Aluffi's categorical algebra
Then there are all the applications of $2$-categories and their $2$-representations that are starting to become apparent in some areas of representation theory
Yeah, n-categories are useful in bordism theory. But that's all I know about them, haha.
@BalarkaSen I never go beyond $2$. Plenty of stuff to do there
@JulianRachman You mean Aluffi chapter 0? Bleh. That unnecessarily complicates simple, concrete topics in algebra.
Well Idk I like it so far
08:35
How much have you read it?
Half way through groups
OK. Then you haven't started on the concrete stuff yet, I guess.
I guess so
So why do you say that category theory is not something to learn?
There are categories involved in the group theory stuff in Aluffi?
I have never said it's not something to learn.
@TobiasKildetoft You know, wrapping everything in a fancy language.
08:39
@BalarkaSen I agree that using categories there is going too far
(not that there are not things in group theory one can use categories for, it just comes later)
@JulianRachman I'm just saying you're better off learning concrete things (have a look at Artin) and pick up categorical stuff as you go ahead. The real application of categories come way later.
So should I keep with all aluffi or just stop where I am and go artin
I am unclear what representations of G \wreath S_n has to do with classification of simple modules, although I admit I don't know much about this stuff.
@JulianRachman Have a go at Artin. It's a beautiful book.
Ok. Then a hat should I do with category theory?
@BalarkaSen representation = module
@Julian Learn bits of it in your leisure if you want. But I'd say you'd find algebra much better than category theory when you really learn it.
Oh and @Balarka isn't since \mathbb{R} is compact that means that it is not homeopathic to \mathbb{R}^2 which is not compact?
08:45
Both are noncompact.
Why would $\Bbb R$ be compact?
Ugh I don't want to give up on category theory because that is where lots of the big research is
@JulianRachman Category theory is a lot easier to learn once you have learned all the stuff that motivated it in the first place
The big research is on applying category theory to prove concrete stuff, last time I heard.
08:47
i.e. pretty much all other math
Like I was even thinking to other day on how we can prove the ABC conjecture using category theory instead of the original 500 page proof
So you need to know the concrete stuff.
@JulianRachman ABC conjecture is still not proven
Oh. Wait didn't take a Crack at it and the paper was wrong?
To be frank, I think it's silly to hope ABC conjecture can be proved using category theory.
@JulianRachman Mochizuki has claimed he has proved it. But nobody bothered to check it because it's so badly written.
08:49
Ok well ill go artin
and p2 munkres
09:03
I have decided to finish the basic categorical part of Aluffi then jump into Artin and Munkres Part 2
@TobiasKildetoft So, what have you been thinking about lately?
@BalarkaSen still trying to understand the Kazhdan-Lusztig cells in type $B$
though I have also been trying to understand the implications of a new description of so-called special representations, which allows the concept to be extended to a much broader generality
Must be fun. I have no idea about the kind of math you do :)
@BalarkaSen The Kazhdan-Lusztig cell stuff is really just combinatorics (since someone has worked out previously how it should be). It just happens to not be described very well, in a paper that is not very well written.
09:18
Can you give me a rough idea of what it is?
I'm curious.
@BalarkaSen Are you familiar with Weyl or Coxeter groups?
I know the definition of a Coxeter group.
actually, let's just take the "easy" case of type $A_{n-1}$, which is just the symmetric group $S_n$
The KL cells come from three different partial preorders on the group, the left-, right- and two-sided preorders
let's just focus on the left for now (the right is just the same with inverses and the two-sided is generated by the other two)
09:22
okay.
we say that $x \to_L y$ if two things are true: There is some element in the generating set (which are the transpositions of the form $(i\ i+1)$ here) which reduces the length of $y$ when multiplied on the left, but which does not reduce the length of $x$ when multiplied on the left
OK, that makes sense.
(so for example if $x = e$ is the identity, then this part holds for any $y$
Now, the second thing is somewhat technical. It requires that the KL-polynomial $K_{x,y}$ or $K_{y,x}$ (whichever is non-zero if one of them is) has largest possible degree given the lengths of $x$ and $y$ (there is a bound for any KL polynomial in terms of these lengths)
09:26
what's a KL-polynomial?
and don't ask me why anyone would consider this condition, as I have no intuition for that
the KL-polynomials come from a distinguished basis of the Hecke algebra of the Coxeter group
ah, ok, I'll just take it as granted that there is such a thing for now, then. what do you mean by "largest possible degree"?
@BalarkaSen There is a general bound on the degree of $K_{x,y}$ in terms of the lengths of $x$ and $y$ (which I can never remember)
so largest possible means that the degree equals this bound
anyway, one extends this to a partial preorder on the group in the obvious way
09:30
the first condition can be reproduced in any group by defining length to be the Gromov metric of the element and $1$, but this condition is too technical, it seems.
@BalarkaSen yeah, the second condition is very technical
plus, those KL-polynomial things only come from Coxeter groups, you say.
ok, please continue.
@BalarkaSen Yeah, not sure if they can be defined in higher generality
anyway, ths gives of a partial preorder denoted $\leq_L$
09:31
yep.
and as with any preorder, we get an equivalence relation denoted $\sim_L$ (so $x\sim_L y$ if both $x\leq_L y$ and $y\leq_L x$)
the equivalence classes of this are called left cells
and the equivalence class is called the left cell?
ok, fair enough.
similarly, one defines $x\leq_R y$ iff $x^{-1}\leq_L y^{-1}$
09:33
ah.
and $x\leq_{LR} y$ as the union of the preorders
and these give right- and twosided cells
alright, I get it.
for $S_n$ there is a really nice description of the cells and of the two-sided order (not sure if there is a nice one for the left or right order)
why are these things of general interest?
@TobiasKildetoft oh?
Well, given a left cell, one can define a representation of the group, and the the symmetric group, one gets precisely the irreducible representations this way
plus, they turn out to encode a bunch of important stuff
09:35
How can one define a representation of the group from a left-cell?
@BalarkaSen in a technical way that I can never recall
hah, fair enough.
anyway, the nice description of the cells is via the Robinson-Schensted correspondence if you are familiar with that
no, I am not really familiar with it.
ok, the important thing is that it is easy to compute and associates to each permutation a pair of standard young tableaux of the same shape
09:38
hm, ok
elements are then in the same left cell iff they have the same left tableau and in the same twosided cell iff their tableaux have the same shape
and the twosided order (on the twosided cells) coincides with the dominance order on the corresponding partitions
though that last is a theorem from 2006, despite the rest being known since like the 80's
ok, interesting.
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