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21:00
@DanielSank Is it a "definition-theorem-proof style" book?
@DanielSank Please sent it to me.
You have my email.
@ACuriousMind Because some of us still have some catching up to do in terms of GIFs viewed/time alive ;)
@ACuriousMind : chat looks like a broken instrument board because you won't talk physics. How about talking about time dilation? See if you can point out any problems with this here little answer of mine.
1) Vectors can be expressed in various bases. This is obvious if you draw an arrow on a piece of paper and draw two different coordinate axes.
2) It's useful to talk about linear transformations of vectors.
3) Those linear transformations can be expressed as matrices, but doing this requires a basis choice.
4) Changing a matrix/vector from one representation to another involves a transformation (which is unitary), and that transformation has the same matrix in the two bases it connects.
5) Integration and derivatives are linear operations. The exponentials diagonalize derivatives.
@Danu No.
@DanielSank So what kind of things do you write about?
21:02
@Danu It's a "This is pretty simple so let's make it as obvious as possible, with examples and really useful exercises" style book.
@DanielSank Ah
@Danu Yes, this sounds obvious but I'm not aware of any other document which takes this approach.
@0celo7 Ok will do in a second on one condition: you agree to actively send feedback about unclear sections, organizational issues, etc.
Ok?
But you're not doing the usual things like you know proving convergence and shit
@Danu Absolutely not.
@DanielSank Hey I'll also gladly do this
21:03
That's a complete waste of time IMO.
@DanielSank Sure. I don't promise to read the whole thing, of course.
@0celo7 Ok then it's a deal.
@DanielSank Ahem... For physicists
@DanielSank How do you explain that the Fourier transform relates the function on a (continuous!) interval with functions on a (discrete!) lattice in that "change of basis" point of view?
We don't have a patent on Fourier analysis :P
21:04
@Danu *GDP production
@ACuriousMind You just point out that $f(x) = \langle x | f \rangle$ for some abstract vector $f$ and then move on with your life.
@Danu Meh.
@DanielSank I don't follow
@DanielSank Honestly though, I think it's cool 'n' all for us to ignore those issues, but you shouldn't try to deny that those things are useful in other respects.
@ACuriousMind Is Stone-von Neumann the one which says $p=-\mathrm{i}\nabla$ is the unique rep?
(Google is your friend)
21:06
huh?
@0celo7 You know, you could have just googled "Stone-von Neumann theorem"
Guys
@ACuriousMind huh
Is there a general theorem when a green function is just the solution * $\theta(x)$
Because that kind of solution pops up often
@Danu Dude, even if you're a math student, you will pass through a point in your life where you need to understand wtf is going on without all the epsilons and deltas.
@ACuriousMind What don't you follow?
21:08
@ACuriousMind What do you actually mean by this?
@DanielSank But they are still interested in convergence, they just leave behind the need to prove it in the excruciating detail of hte epsilons and deltas
@DanielSank Yes. But as a mathematician you also need those things---I'm not objecting to you skipping it, just to your assertion that it is a "complete waste" of time.
@DanielSank How your reply answers my question. Like, at all.
@Danu Fine, it's a waste of time for anyone at the stage that they should be reading this text.
@ACuriousMind Then I failed to understand the question.
@DanielSank Periodic functions have discrete Fourier transforms.
21:09
@DanielSank Okay :) So can I see a copy? :D
@ACuriousMind Oh ffs ok yes that requires extra discussion.
@ACuriousMind Deltas everywhere
lol
Delta's are god damn functions :D
I don't think I've ever seen a Fourier transform in GR
Whatever... if you just think about it for half an hour you can figure it out. But you're right, I should put something about the Poisson summation formula in there...
21:11
@DanielSank Okay
Maybe g wave shit
Poisson resummation?
@0celo7 Source term in linear GR
Oh, not resummation
@Slereah what about it
21:11
Annoying that there are 2 different things with such similar names.
It's all Fourier shit
@Danu This
6
Q: What is the sum over a shifted sinc function?

DanielSankWhat is the sum of a shifted sinc function: $$g(y) \equiv \sum_{n=-\infty}^\infty \frac{\sin(\pi(n - y))}{\pi(n-y)} \, ?$$

There isn't a lot of Fourier in GR because GR is non-lineae
See the part about Poisson summation.
well I don't care about linear GR
21:12
But linearized GR, you can use Fourier 'til the cows come home
@DanielSank It's fine---I just learned about Poisson resummation in CFT and that's something different so I was confused.
@Slereah Yes, I know you can think of them as a nice Dirac delta comb, but that would require introducing distributions
@ACuriousMind Everyone loves distributions!
Delta's are god damn functions
:D
@Danu mb I should talk about that
it's in BLT, right?
21:13
$\delta(0) = \infty$
@0celo7 Blumenhagen
Good way to bother a mathematician
@Slereah ::eye twitches::
I know that for some people (1 or more) Fourier is everything, like a stance.
Oh wait
21:14
@ACuriousMind Take that.
I can do worse
$\delta(0) = \aleph_0$
@Slereah Have mercy!
$\delta(0) = \aleph_0 + \omega + \infty + \text{Card}(\{ x \vert x = x\})$
@Slereah so, is $2^{\delta(0)}=\aleph_1$?
Yes, that's the Dirac distribution for the space of all functions
21:15
Don't they do that in Faddeev-Popov
@DanielSank 2006?
34 pages?
I was expecting 800+
@DanielSank do you need someone to solve the exercises
@ACuriousMind Shitty notation ;)
I guess Mr. Daniel Sank disagrees
Whatever, I'm considering dropping that entire section.
Mar 3 at 20:10, by Chris White
@0celo7 marking every vector indiscriminately with a ket is akin to marking every vector indiscriminately with an abstract index -- it is indicative of the author fundamentally not understanding the structure of the mathematical objects they're working with
@ChrisWhite you should fight DS
@DanielSank The vector space axioms? :P
@0celo7 Wow.
@DanielSank Uh-oh :P
21:19
@Danu I wrote most of this when I was an undergraduate. This whole thing happened because my quantum mechanics professor started talking about momentum space and using Fourier transforms and nobody had any idea what he was on about.
@DanielSank why is $V$ bolded?
Then he said "look, it's just a basis transformation" and everything clicked.
Shankar's QM books states this multiple times
I wrote this document because I realized that nobody in my class (or department) really understood how these things were related.
mb that's why I don't get why you're writing this
21:20
@0celo7 Yeah, well that's why I recommend Shankar, but we didn't use it in undergrad.
@DanielSank your example with the two masses is straight from Shankar
Go look around on main. You'll see people recommend Griffiths to n00bs.
> The symbol $|\,\,\rangle$, called a ket, indicates a vector.
@DanielSank Hey, I like Griffiths.
I also never really used the Fourier transform in that book.
@0celo7 Yeah, I found later that Shankar does some, but not all of what's in my document.
21:21
As far as I remember...
@DanielSank the typesetting could be refined, I'd be happy to do it while reading...
@0celo7 Please don't pepper chat with specific comments about it.
It's in a github repository. Just file issues and pull requests.
> Keep in mind that |v + w> is
simply a shorthand for writing the vector that is the sum |v> + |w>
@DanielSank I don't know what that means
@0celo7 Why do you keep posting excerpts? Are you making fun of me or what?
gtg for a minute
@DanielSank No, but that statement is not good
when you start labeling kets by eigenvalues, that's wrong
21:23
@DanielSank I think he wants me to fight you over your notation :P
^ ...perhaps
Ocelot, always trying to stir up trouble... ;)
that's why you love me
You know, when I was in school my math teachers were always really insistent
YOU MUST PUT THE ARROW ON THE VECTOR
Nowadays I realize that math people don't give a shit
Mar 1 at 18:48, by ACuriousMind
I don't love you, and what little brainpower I had available today has been drained already, so I'd prefer not to think hard in the next hours
21:25
he was hungover when he said that
he didn't mean it
(incoming...)
@Danu No, I can't bear to see his little heart break.
@DanielSank I don't know how to use GitHub!
Ahhhhhhh! I have comments!
I don't know where to put them!
I thought I might write another book. Using my stack exchange answers to help out here and there. I also thought I might have a chapter or two about physicists and the state of physics.
lol
21:29
What was that about being nice?
@ACuriousMind What are you saying
@JohnDuffield I'm nice :)
@Danu Chap. 9 of BLT.
@ACuriousMind Ok, my life is over. I just sent a snap containing just "huh?" to Rebecca. I'm an addict
why did you do this to me
Who is Rebecca
your mom
That is not my mom.
Anyway, I was thinking of stuff like this, but more so. Thoughts?
21:35
You might have the wrong mom.
Be careful it is not your own
@Slereah step mom?
Also no
I have a step dad, but he is not called Rebecca either
heh
@0celo7 What did I do? You started saying it.
@ACuriousMind ever since you pointed it out I can't stop
@ACuriousMind in one line, what does the Feynman propagator mean
21:37
It's a time symmetric propagator
a what now
if you had to explain to someone why you want to calculate it
in one line
@0celo7 wat
what would you say
It's a propagator where the integration contour goes between the poles
21:38
sigh...
Well you asked
@0celo7 It's the probability amplitude for a particle to go from x to y. (True enough to shut them up :P)
But then that is also true of the retarded and advanced propagator!
OK, I knew that, but I thought it was "wrong"
@0celo7 It's true in usual QM and free field theories, and false in general QFT
21:39
@ACuriousMind why is it wrong in interacting theories?
Because for a start there's no particles in QFT
is it true of the corrected propagator?
What Slereah said, you can't even define the notion of particle properly.
It is even impossible
@ACuriousMind so what does it mean then
21:40
There's theorems and all
@ACuriousMind I'm still not convinced of that, but whatever
@0celo7 It's the Green's function for the classical equation of motion. It "propagates" a given source/disturbance through the field
If you assume the usual Hilbert space structure and Lorentz invariance, you can't have a notion of particles
@ACuriousMind Ok, we're doing that thing were you're saying things I know and my question isn't precise enough
Isn't the Green function the other one
The... Dyson function?
there's like 7 different contour integrals in QFT
I can never remember which is which
21:42
@Slereah Yeah, it might not be exactly the "Green's function", but close enough, we're physicists!
To give you a rigorous mathematical explanation, the contour integrals are : Above contour, below contour, 'round the pole contour, 'round the other pole contour, in betweeny contour, 'round both poles contour and 'round both poles contour but doing a figure 8
haha
Above and below are retarded and advanced
Feynman is in between
the others are the... non-green function ones, I think?
Any mods around? @DavidZ, @Qmechanic?
Like just solutions of $D\varphi = 0$
21:44
I'm not sure my examples of applications of Fourier transforms should come from QFT, now that I think about it
@EmilioPisanty Does it need to be a Phys mod?
@EmilioPisanty I see @dmckee lurking
@ACuriousMind Are Fourier transforms used in Riemannian geometry?
I've never seen it.
@ACuriousMind Naw, last seen an hour ago
I've seen generalizations of the Fourier transform used in Riemannian geometry
It's called the...
21:46
@ArtOfCode Would be preferable but maybe you can help
Hm do I have it somewhere
@EmilioPisanty Try me :)
Or maybe even a neutral look would help more.
@0celo7 Geez, I'm not your personal math encyclopedia. Google "Fourier transform Riemannian geometry" :P
@ACuriousMind that never occurred to me.
21:47
I honestly don't know if you're joking oO
user54412
ACuriousMathopedia
@ACuriousMind I'm actually not.
Ok, so I'm going a math presentation, I guess. I need to learn how to use the LaTeX presentation thingie
What's it called?
And how do I import the official school PP template into Beamer?
"Exact QED Path Integration of the Maxwell Action, with Gravitational Curvature and Boundary Terms, Using Pontryagin Duality"
Ah, that's the one
Pontryagin Duality
21:49
That's some topological group thing
@ACuriousMind Basically, I need all the examples for applications of Fourier transforms
Morse theory?
@0celo7 Good luck with that
Well then maybe take classical examples of it
My classical examples are QFT
Fourier transform is gonna be mostly solids, EM, heat equation
Shit like that
QFT also yes
I'm gonna do a lot of QM
21:50
Anything linear really
Oh electronics also
But I don't think any of the undergrads have taken a formal QM course -.-
@Slereah don't know shit about that
@0celo7 is gonna be the worst fucking student
huh?
He's gonna be all UH ACTUALLY PROFESSOR THAT'S NOT PART OF THE HILBERT SPACE
@Slereah I have never done that. No. Definitely never...
21:52
@Slereah mb I should take the functional analysis QM course before the physics QM course
::gets out Shankar::
::finds multi-line equations::
So this is why scattering sucks
Has anyone seen the Canadian kid recently?
@0celo7 You mean @HDE226868? ;D
@ACuriousMind No.
21:59
@0celo7 Wouldn't be the first Canadian to disappear from this chat, I've not seen Jim in ages, either
Do they freeze to death or something?

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