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00:00
To put it in context, when he writes the Sobolev norm he writes it in italics, like it's something new.
It's used in the context of topology and the Cauchy problem.
It's an inequality imposed on the initial data's evolution within the future domain of dependence (which is a cone in $\mathbb{R}^{3,1}$) IIRC.
yeah... I don't think I can muster the power of will to care about these type of things right now... sawry :P
good luck with it though
It sucks that Math.SE is so saturated.
:/
sigh one of my matlab codes is giving trouble
Lol, Arnold's Analytical Mechanics book has 200 pages of appendices.
Damn
00:06
I have always wondered about the connection between Hamiltonian mechanics and symplectic geometry...this book seems to contain the answer.
Certainly does.
This is the go-to reference
Cool. Can I skip the Newtonian review and Lagrangian stuff?
does anyone know matlab =(
I'm taking a break from Wald to learn some more rigorous classical mechanics.
Reread Tong's Classical Dynamics lecture notes over the last couple hours, now I'm on an analytical mechanics kick!
@Danu: Are the symplectic diffeomorphisms Arnold speaks of canonical transformations?
@0celo7 Yes, canonical transformations are precisely the symplectomorphisms.
00:13
"The phase space is the cotangent bundle of the configuration space"
That's a lot cooler than saying phase space = p & q
"Hamiltonian mechanics cannot be understood without differential forms"
@0celo7 It's also more precise, because it tells you that the phase space is the cotangent bundle, and not just any vector bundle of the same dimension over the configuration space.
I swear people on this site quote him
@ACuriousMind I'm sure he explains this, right?
It's sure as hell not intuitive.
@0celo7 No idea because I haven't read him.
But he should
@ACuriousMind I didn't want to read about Lagrangian mechanics for the 10th time, so I skipped to page 161. I hope I didn't miss anything.
@ACuriousMind @Danu Is $\mathbb{R}^n$ self-dual? If yes, is there anything meaningful to that statement? If no, what is an example of a self-dual space and what meaning does that have?
@0celo7 Every finite-dimensional vector space is self-dual. It's only in the infinite-dimensional case that things start to go wrong.
00:20
@ACuriousMind So this doesn't imply anything special?
Not about $\mathbb{R}^n$, no.
Are you implying that it could mean something special?
For another space?
I have the feeling that the self-dual spaces are those that can carry inner products
Is $L^2$ self-dual?
00:23
How does one prove that?
By noting that every element of $L^2$ defines a continuous linear functional on $L^2$ through the inner product, and that every continous linear functional defines an element of $L^2$ by summing up its evaluation on an orthonormal basis.
More generally, every inner product space is self-dual by this argument, if I am not mistaken.
So is self-dual a tautology of having an inner product?
Yes, I think so, because given a self-dual space, you can define the inner product of $x,y$ just by the action of the dual of $y$ on $x$ (or vice versa)
Could be that this evaluation map fails some property of the inner product on some cases, though, I am not sure
What's a space that doesn't have an inner product?
Hm. Well, the space of tempered distributions doesn't have one, I think.
user54412
00:35
@ACuriousMind That seems too broad.
@0celo7 It's self-dual yeah
@ChrisWhite Probably, that's why I phrased it as "a feeling" ;)
as are all Hilbert spaces, I think, right @ACuriousMind?
@Danu I believe that is correct.
user54412
In fact in these pdf notes above example 4.8: (L^p)^* = L^{p'}, where 1/p + 1/p' = 1
00:37
Is knowledge of tempered distributions something I will need?
I think it is the completeness w.r.t. the inner product metric that forces self-duality
user54412
And in particular only for p = 2 is L^p its own dual
So perhaps the self-dual spaces are those that can carry inner products and be complete w.r.t them
@0celo7 For what?
user54412
I.e. Hilbert spaces
00:38
I've never had any practical use for them
Just checking, since @ACuriousMind brought them up. (As a counterexample.)
@0celo7 Well, you don't need to, but technically you don't know what a quantum field is if you don't know distributions ;)
only technically
They are the dual space of the Schwartz function of rapid decrease, and are also needed to properly define unbound states in QM
@ACuriousMind I'm fine with wavy thing in spacetime for now. You can keep your distribution theory.
user54412
00:39
@ACuriousMind I still don't know what a distribution is
But it's really technical, it doesn't lend much insight.
@ACuriousMind it's just like... good to know tempered distributions exist
nothing else really
as far as I can tell
Wavy thing is full of insight, on the other hand.
even in my MQM course we never really needed it
@ChrisWhite You're not getting anything more precise than "linear thing that eats functions" from me
(which is basically how they are indeed defined)
00:41
also @0celo7 maybe it is a good idea to study some diffgeo before reading Arnold
@Danu My diffgeo is good. (In my mind)
Ah cool
user54412
@ACuriousMind See, I do know what a dual space is. I've never been able to get a straight answer as to whether they're really the same thing.
just saying cause you asked about symplectomorphisms
(I know my diffgeo is mediocre at best, and I know what they are :P)
but maybe it was just my prof choosing random topics
My question was more a "I'm pretty sure I'm right, pls confirm"
00:43
wouldn't be the first time, lol
Ah, yes
I have Jost and Lee, which I've been meaning to read. No time though
So my DG is from lecture notes, Wald and Straumann
Lee is really nice
absolutely excellent
Do I need to read his topology book before his smooth manifolds book?
no
I didnt
He has a very concise yet extensive survey of basic topology as an appendix
@ChrisWhite It depends, because the continuous and algebraic dual are two different things. (The latter is just the dual space without requiring them to be continuous). I think the distributions on a function space are indeed just the continuous duals.
00:46
Yeah I think so too ^
distributions are kind of a analysis/topology thing so they should be continuous
(yes, this is how I do math lol)
Is the dirac delta technically a distribution?
yes
Is it continuous?
ehm I think so
don't think about this handwavy physics way of thinking about it as an infinite spike
Wow, does Arnold really need to prove that the wedge product is associative?
00:48
aren't almost all useful algebraic operations associative?
Stuff like that I just YOLO
The only thing I can think of that isn't is the octonions
but then again... who cares about octonions
Lol
awaits shitstorm
Never heard of them
00:49
really?
Doesn't mean much tho
c'mon you should know the chain
@Danu I'm all self-taught
Chain?
@0celo7 It is in the sense that the prescription "multiply the dirac delta with a function and integrate" is a continuous linear functional on the real functions
$\mathbb{N}\to \mathbb{Z}\to \mathbb{Q}\to \mathbb{R}\to \mathbb{C}\to \mathbb{H}\to $... octonions
(idk the symbol for octonions)
H is the quaternions
00:50
Was just about to ask what the symbol is
I know that
What does the chain say though
I just call it a chain
it's not a technical term
wiki says $\mathbb{O}$
(well it is but I'm not using it as such)
@Danu Strictly speaking, the tensor product is not on the level of elements, for example
oh right makes sense
00:51
lol what does it say
@ACuriousMind Shhhhh :P
@0celo7 The chain gains nice algebraic features up to $\mathbb{C}$, and then starts to lose features.
So @0celo7 you're not a student in the usual sense?
@ACuriousMind Yeah, it's beautiful
At least Arnold uses $f^*$ for the pullback.
(H loses commutativity, O loses associativity too)
@0celo7 Is there anyone who doesn't?
00:52
Wald got it into his mind that $f_*$ is the pullback.
hahaha, nice.
damn physicists!
@Danu I'm in high school. So, yeah, a student.
Ah like that
I always forget where the star goes for what.
Also from your profile: You are reading Hawking & Ellis and Wald before Weinberg?
You do realize that Weinberg's book is not that advanced, right?
00:54
Yes, but it's a different topic :)
More astrophysicsy
Gravitation & Cosmology will be hella boring
after Wald/H&E
I read the first half already
right
I learned GR from Zee and Weinberg
so just the cosmology left
I learned it from Carroll
00:55
Then I reinforced with Straumann, Wald and H&E
I think Weinberg would be my number 2 for GR, but I HATE HIS TYPESETTING
Oh yeah some Carroll in there too
(with a passion)
I love Straumann, but I hate \var cap Greek letters with a passion.
That shit is not slanted.
@Danu Are you referring to the idiosyncratic notation, or the look of the formulae?
00:56
BOTH!!!
@ACuriousMind there's nothing wrong with his GR notation
Hehe :D
urrrrgh :P
Although using $I$ for action is weird.
@0celo7 Not as much as his QFT notation, but it's not perfect IIRC
Right, wtf is that!
00:57
@0celo7 There's nothing wrong with his QFT notation, either. It's just different from what everybody else uses :P
^No, it's wrong
Just... no. Not like that. No.
What is wrong with his QFT notation?
Have you looked at his book? It's literally unreadable to me because of the terrible notation
I have the first two!
Point something out that is wrong.
I mean not factually wrong
but morally wrong
00:59
That's what I mean ;P
I don't see anything wrong
Have you read different QFT books?
Zee, Tong's lecture notes
I have P&S on my list
Oh yeah, also his damn tables of content

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