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01:00
@Semiclassical, we could always extend it so that it is.
and your cells consumed nutrients and oxygen
therefore
Yeah but the amount of energy you lost isn't significant
But nothing else is told to us about $g(x)$ except that it is defined on $(0,L)$.
your hand did work
no amount of energy "isn't significant"
tis still work
Then how can you infer that it's even? That's a statement beyond (0,L).
01:01
okay how about this
just near little amounts of work
You didn't do work in macroscopic level
not the microscopic level
I mean, as a very simple example: Take $g(x)=0$ for $0<x<L$ and $g(x)=1$ everywhere else.
o/
@Semiclassical I posted a question about it on the main MSE page and no answers, but a couple of guys said pretty much the same thing you did. What can we say, then?
01:01
i'll give you that one. ;)
Does anyone have any recommendations concerning representation theory of Lie algebras for undergraduates?
Well, couldn't you extend it so that it is even?
I suppose so? I could be missing a counterexample, though.
Er, what can we say about $g(x)$ that is, @Semiclassical given that $g(x)$ is defined on $(0,L)$ and that integral is zero?
But, really
01:02
@TheGreatDuck If 1=0, prove that you're the pope ;)
@Hiro that deserves a star.
If you're given $g(x)$ on (0,L), then you can always extend that to be even.
Just define $\tilde{g}(x)$ to be $g(|x|)$.
@Semiclassical this is what I said: math.stackexchange.com/questions/2032202/…
Could you take a look? I felt all confident for the like the first time ever on this assignment, and then I post just to make sure, and now I'm all muh.
In order to say anything definitive about stuff outside (0,L) you need additional assumptions.
Now, you can probably say that certain things are permissible.
I think that's what those guys on there were getting at. But, it looks here like I'm really only interested in (0,L)
01:05
But if someone just tells you "$g(x)$ behaves on (0,L) in this way"
then you can't say anything about it away from that interval.
@Hiro let the pope be denoted by 1 and everyone else as 0. I am everyone else, therefore i am the pope.
2
Do I need to though in order to answer the question?
Maybe not.
I think you could say that it's symmetric under $x\mapsto L-x$?
Though maybe that should be antisymmetric for one and symmetric for the other.
@Semiclassical would you be interested in posting an answer?
Not really.
01:07
:(
@Null Nice try, but that means that you along random people are the pope, so try to prove that you and only you are the pope.
I have a feeling nobody is going to.
basicly add 1 until we got 5=4^^
What about what the one guy said about how we need to know that $g(x)$ is even integrable on $[0,L]$?
Tbh, I don't know. This gets into the formal details of Fourier series which I don't remember.
01:09
Beautiful.
@Null the way you'd go about it would be that if 1=0, then 2=1 by adding 1 to both sides, and if the pope and I are two people, then the pope and I are one person, therefore I am the pope
The 'soft' conclusion I"d draw is that the Fourier series in the first case contains only cosines which are $[0,L]$ periodic, and the second only sines.
Because I know that you need a whole bunch of criteria - Dirichlet's conditions - in order for the series to actually converge to $g(x)$, but nobody said anything about needing that. There are lots of Fourier series that don't converge to their respective functions.
@Hiro our analysis tutorer made that joke, forgot it :(
01:11
@Semiclassical, don't know if you're a Game of Thrones fan, but that's the moment when the Hound would say "Lots of expletives".
@Null lol if you're in a logic class, the teacher will definitely bring it up
What is all of you guys' obsession with the Holy Father tonight?
@Semiclassical in any case, that's pretty much the same conclusion I came to. Unless somebody answers the question I posted, I'll stick to it, and maybe add on a bit about not being able to tell anything about the behaviour of $g(x)$ outside of the interval $(0,L)$, yadda yadda.
Hi @TedShifrin
And since TedShifrin won't answer any more of my questions since I'm cray cray :(
Do you have any opinions on good books for representation theory of Lie algebras?
01:15
He is like the god of PDEs.
@Danu Fulton and Harris is the classic right?
I have a course on exactly that at the moment
Could be!
I'm looking for something to recommend to undergrad students
(is this even feasible?!)
@Danu Fulton and Harris is probably very hard for undergrad students
At least, in my experience with the book
@Krijn Yeah, way too hard probably. I'm definitely not looking for that, it seems :P
@Danu: I am a baby when it comes to representation theory. I love to recommend Curtis's introductory Springer book on Lie groups, but that doesn't fit your bill.
01:20
@TedShifrin I was looking at Stillwell's "Naive Lie Theory".
Representation theory of Lie algebras is mostly (reasonably advanced) linear algebra. I would start by looking at Jim Humphreys's book.
Is this a baby like when Balarka says that he's a baby in Algebraic Topology, or a proper baby?
Not really about representations though.
But, still, it's probably graduate level.
@TedShifrin This is way too hard for my kids :\
01:21
ROFL @Krijn
I remember struggling with it myself 2 years ago
Why should kids be doing representation theory?
@Krijn No :P
@TedShifrin I just want some really basics
Because it's very useful in particle physics, to make sense out of the zoo of particles in the standard model.
I do not know an appropriate resource.
And to inspire them a bit when they encounter the $\mathfrak{su}(2)$ algebra generated by angular momentum operators
01:22
But this still requires a comfort level with linear transformations that many undergraduates do not have.
What does?
What you just said.
Meh, physicists do a good job giving some intuition without any formal knowledge :D
The concept of operators acting on a space of states (Hilbert space) is very natural for physics students, so the basic idea of a representation comes rather naturally.
Take a look at this.
You paraphrased some really negative comments in a positive daylight there.
01:25
@TedShiftin Re: "Why should kids be doing representation theory?" Well, it's better than doing drugs, isn't it? ;P
Unless it drives them to same, @Jessy :)
@TedShifrin Oh, neat!
@TedShifrin hahahaha
DESPAIR
@TedShifrin yes!
And, just for your information, @Jessy, I took one graduate course in PDE approximately 40 years ago. I am far from an expert. Even the course I taught that covered Fourier series and PDE was 30 years ago.
@TedShifrin okay so I exaggerated. You still know more than me.
01:28
"physicists don’t write the sum sign, but remember that one should sum
over indices that repeat twice - once as an upper index and once as lower. This convention is called the Einstein summation, and it also stipulates that if an index appears once, then there is no summation over it, while no index is supposed to appear more than once as an upper index or more than once as a lower index."
Yes, that's true. :) No insult intended.
What the hell
Einstein convention has been around for 100 years, @Krijn, although I tend to draw the summation symbol "irregardless."
I've heard of it but never looked into it
Think of it like this. If you wanted to write down the matrix multiplication $ABCD$ explicitly, you'd write $\sum_{klm}A_{ik}B_{kl}C_{lm}D_{mj}$
01:30
The notion that upper and lower indices need to combine and get summed to get something that is well-defined is actually quite powerful.
@Krijn This is super handy.
No, @Semiclassic, you need one upper one lower for a linear transformation.
Eh, I'm not worrying about contra/covariant at the moment.
Einstein summation convention demands (appropriately) one upper against one lower.
I am.
In any case, I'm getting back to work. TTFN.
01:31
@TedShifrin Lower them with the metric in Euclidean space and nobody cares. Only once you write Greek letters, it becomes important (duh!)
^the physics way (i'm just joking)
Bull**** @Danu.
hahahha
So triggered :D
Is this just invented to irritate people like me?
waits to be banned from chat
The thing that's funny to me
01:31
@TedShifrin Oh, physics and math
No, @Krijn, it actually works out well with Hermann Weyl's theorems on invariant theory, etc.
What a strange marriage
But what beautiful children.
I'm sure Trump will do away with that, too.
Don't tell me about it :(
@TedShifrin O. Well then, proceed
01:32
LOL
I really don't see much use of Einstein convention in quantum mechanics
Just a question, does an altitude bisect a side in a triangle?
It's essential only in relativistic theories
But in quantum mechanics, you have the whole bra-ket thing.
Noooo @Hiro, very rarely.
01:33
oh...
Only when you're dropping an altitude from a vertex with two sides of the same length coming in to it.
Well that makes things 180 degrees more complex
i.e., an isosceles triangle.
You could get rid of the bra-ket thing and just have stuff like $\phi_i=|i\rangle$ and $\phi^i=\langle i|$
oh it bisects an isosceles triangle?
01:33
But then, how do you differentiate between the sum of $a_ix^i$ and the actual $a_ix^i$
not sure which order I like better, w/e
Draw the picture and prove it, @Hiro.
@Krijn: It gets particularly troublesome in differential geometry when coordinates have upper indices and you want to take powers of those variables.
In general, if you're doing Einstein notation you don't care about individual a_i x^i
If you do, you have to say "unsummed" IN WORDS.
01:35
But that does NOT mean exponent when you write that $i$. It means $i$th variable.
Hence why it's not convenient if you want any kind of multiplication.
Yeah, I think that's actually quite nice
It's mostly handy if you're doing contraction of tensors.
01:36
So dot product shows up as pairing a covector with a vector, and the notation works perfectly, @Krijn.
If you want a dot product of two vectors, you need the metric tensor in there: $g_{ij}x^iy^j$.
There's also the connection to diagrammatic notation, if you're Roger Penrose :)
@Krijn: There are also unitary/hermitian variants, where you put a bar over the second index and it all works out swimmingly.
@TedShifrin Ah, yeah, we use the bar for practically nothing so no chance of confusion there
Bar for complex conjugation.
Totally consistent.
Hermitian inner products are, after all, sesquelinear.
I do believe it all works out pretty nicely in the end
It's just not for my taste, I think
01:42
@Ted I found Gilmore's book "Lie Groups, Lie Algebras and Some of Their Applications".
This seems to be pretty nice
I know nothing, @Danu.
Starts by defining a set, a group, etc :D
Ends with Dynkin diagrams
Claims to have been written based on notes for a course about Lie algebras and their applications in physics
Looks perfect for physics students (that want to learn some math)
Well, give it a shot.
I'm just sending them an email with stuff I recommend
@TedShifrin Let ABC be a triangle, let a,b,c be the lengths of its sides opposite to A,B,C respectively, and let $h_A$, $h_B$, and $h_C$ be the lengths of the altitudes from A, B, and C. Suppose that $\sqrt{a+h_B} + \sqrt{b+h_C} + \sqrt{c+h_A} = \sqrt{a+h_C} + \sqrt{b+h_A} + \sqrt{c+h_B}$. Show that $(a+h_B)(b+h_C)(c+h_A)=(a+h_C)(b+h_A)(c+h_B)$
01:45
I guess nobody will even look at it
but it's worth a shot to try 'n' inspire them
Ugh @Hiro.
Even though I'm geometric, things like this make me go "ick."
lol
@TedShifrin it's not that bad xD
Plane geometry is the worst geometry
01:47
What the hell is the meaning of something like $\sqrt{a+h_B}$?
There, I said it
There can be beautiful things, @Danu.
@TedShifrin is the point that we can't?
can, maybe. Nobody showed me much cool stuff.
We can't what, @DHMO?
I can sometime, @Danu.
01:47
I think that's not necessarily as complicated as it seems, though. If you write it as $\alpha_1+\alpha_2+\alpha_3=\beta_1+\beta_2+\beta_3$, then the implication is $\alpha_1^2\alpha_2^2 \alpha_3^2=\beta_1^2\beta_2^2\beta_3^2$
Yes, @Semiclassic. I saw that much.
@TedShifrin Would love to hear about it.
That doesn't feel geometric to me at all.
and, ignoring the squares, those terms show up if you cube both sides
01:48
Gauss thought his 17-gon was pretty spectacular and he's not a bad mathematician, I think
hmm?
"Ignoring the squares"?
I am not arguing at all, @Krijn.
No no
01:49
$\alpha_1\alpha_2\alpha_3=\beta_1\beta_2\beta_3$
@Danu was
Yeah, but what about all the rest of the junk, @Semiclassic. Surely there's some geometry in there somewhere?
from where did you come up with that expression? @Semiclassical
Oh, sure. But my point is that, if you cube both sides, then that relation can only be true if there's other such relations.
@Danu: In both my books (where it's relevant) I have the students do vector proofs that the altitudes, perpendicular bisectors, and angle bisectors intersect, respectively, in three points. Then you want to show that those three points are collinear, and — in the appropriate order — are in a 2:1 ratio. I think that's all gorgeous.
01:51
By labelling each of those square roots as $\alpha_k$ or $\beta_k$
Just to get to less tedious algebra.
@Semiclassic: True enough.
@TedShifrin We can't prove $\not\exists(a,b)\in\Bbb N^2: a+a=b+b+1$
LOL @DHMO.
@TedShifrin can we?
Well, you can if mod 2 is well-defined. :)
01:52
@TedShifrin Because of the nice pictures, or is there a better reason to like it much? :P
But that begs the question (which we all take for granted).
@TedShifrin no, I don't [take for granted].
if $\alpha_1+\alpha_2+\alpha_3=\beta_1+\beta_2+\beta_3$, how does that imply $\alpha_1^2\alpha_2^2 \alpha_3^2=\beta_1^2\beta_2^2\beta_3^2$
@Danu The geometric aspect of Galois theory is pretty as well
@TedShifrin that is essentially the statement itself
01:53
^^ @Semiclassical
You've also got $\alpha_1^2+\alpha_2^2+\alpha_3^2=\beta_1^2+\beta_2^2+\beta_3^2$
@Krijn I don't know any Galois theory :(
@Danu: I don't have physical applications. Although, now that you bring it up, there's another point which is fascinating. What's the point that minimizes $Ax + Bx + Cx$ for vertices $A,B,C$ and point $x$?
I didn't say I knew, I was just reformulating it
@TedShifrin I guess I'm supposed to put $x$ somewhere inside the triangle?
01:54
@TedShifrin I don't quite get that expression
@Krijn: Unless you mean arithmetic algebraic geometry, the geometry is reaching.
@Danu: Maybe.
But sure ...
for starters.
yeah $\alpha_1^2+\alpha_2^2+\alpha_3^2=\beta_1^2+\beta_2^2+\beta_3^2$ makes sense, but what do you have to do to get to $\alpha_1^2\alpha_2^2 \alpha_3^2=\beta_1^2\beta_2^2\beta_3^2$ @Semiclassical
@Null Objection: you essentially labelled yourself and the pope with the same label. That does not make you the pope.
Should that be $|AX|$, for instance?
$Ax$ meaning... Inner product?
01:55
@TedShifrin Que?
@Semiclassic: Of course. I was being lazy.
Ohhh
I see
No, no. What Semiclassic said.
I forgot the plane geometry notation :P
That'd be the Fermat point, if memory serves
01:55
I tend to prefer $\|\overrightarrow{AX}\|$, but I was lazy.
Hush @Semiclassic.
My prof asked me a similar question, but with 4 vertices on a square..
Fiine.
Spoiler :D :P
It made me think for a bit :)
So the point is how to construct it I guess
Very not unique for a square.
01:56
And it actually had a connection to the physics we were working on, amusingly enough.
@TedShifrin how can you rearrange $\alpha_1^2+\alpha_2^2+\alpha_3^2=\beta_1^2+\beta_2^2+\beta_3^2$ to get $\alpha_1^2\alpha_2^2 \alpha_3^2=\beta_1^2\beta_2^2\beta_3^2$?
Right, @Danu ... and it has a physical interpretation, unlike the others.
@Hiro: SOMEWHERE you have to use some geometry :P
@TedShifrin like what kind of geometry are you talking about lol
@TedShifrin I might think about it some other time---I have to admit that those construction problems can be kind of fun. Do you know the game Euclid?
lengths and altitudes, @Hiro.
No @Danu
01:58
You have to do constructions in plane geometry, progressively harder ones.
I'm not sure how much of this is really geometry, though.
I think it's mostly just implications from algebra, and that's pretty boring.
I did say ugh^3 and ick a few times, @Semiclassic.
As you show you're able to do some constructions, you are allowed to use them (via a "shortcut button") in the next levels. euclidthegame.com/Tutorial
It's super cool
01:58
I bet Pythagoras comes in ...
The last few levels took me a while :D
probably.
I won't even go there, @Danu.
Of course, the real challenge is doing the levels with minimal number of lines ;D But I'm not hardcore enough
I mean, you can write down the area of the triangle in three different ways
01:59
D'aww Ted. It's so much fun!
For $a,b\in\Bbb N$, prove that exactly one of the following is true:
$\exists n\in\Bbb N:a+n=b$
$a=b$
$\exists n\in\Bbb N:b+n=a$
I'm not so much a game-player, @Danu, other than bridge.
And cribbage.
and that imposes some further relations on the altitudes and lengths.

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