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03:00
good
thats better
mmmm some actual physics
go go gadget ACM
answer
@enumaris What I was talking about wasn't physics?
elliptical PDEs? -.-
lots of things are elliptic PDEs
03:03
@user400188 What page in Schwartz?
Page 5, (25 if you have the same pdf as me)
I once and only once encountered an elliptical integral
it was for trying to solve for the EM field of some distribution of charges
that has nothing to do with elliptic PDE
forgot all the details
so I dunno what elliptic PDEs are then lol
Laplace's equation is the simplest and most obvious one.
03:07
o
what makes them elliptical?
wikipedia discusses the classification here: en.wikipedia.org/wiki/…
interesting way to classify it
@user400188 Okay, so, as you correctly observe, in a true $L\to\infty$ limit this doesn't make a whole lot of sense because the $E_n$ all go to zero. But that's fine - in the passage to the continuum limit, we have to think in terms of densities instead of actual values: The meaningful quantity is not actually $E(\omega)$ - note that it's infinite since it has $L^3$ in it, but the energy density $E(\omega)/L^3$.
In that computation, Schwartz is not actually taking a true limit $L\to\infty$, he's just saying that we treat $L$ as so large that the $E_n$ become continuous, i.e. we get an integral, but it's still finite otherwise the $L^3$ wouldn't be there
ayyyy, finally some hand wavy maths, now this feels like home
This is always what scares me the most
03:12
don't you dare make it a rigorous definition
How can $L$ be so large that $E_n$ becomes continuous, without $L$ being infinite?
It can't, it's a trick :P
yesssss
accept it, you know in your heart that you want to do hand wavy math, that's why you became a physicist
krank
Well, I suppose that answers everything about the question (even if the last bit wasn't as satisfactory as I would like it to be). Your answer was good though.

Thanks for the help @ACuriousMind and @0celo7
03:24
@ACuriousMind Yo
@user400188 Here's a way to arrive that the formula without taking this weird limit: The energy density is the integral of the energy of a state times the density of states. If you compute the density of states, you find it is independent of $L$, so you can evaluate this formulation of the integral without having $L$ show up at all.
Suppose I have family of operators $L_t\in \mathscr B(X,Y)$ between Banach spaces such that $t\mapsto L_t$ is continuous
Then you can formally (and trivially, since it doesn't occur) take the limit $L\to\infty$.
And suppose each is boundedly invertible
Ah that makes more sense
03:26
and suppose I solve $L_t\psi_t=\gamma_t$, for some family $\gamma_t\in Y$ with $\gamma_t\to 0$
must then $\psi_t\to 0$ in the topology of $X$?
I don't have the slightest idea
I might if I thought a bit about it, but I'm about to go to bed
ok, good night
Good night @ACuriousMind.
I guess one needs to know if $t\mapsto \psi_t$ is continuous in a sense
I haver to leave too. Bye @everyone
03:28
Thanks, good time-of-day to you too
@ACuriousMind I bet we have $t\mapsto (L_t)^{-1}\gamma_t$ being continuous, and it $\to 0$.
@ACuriousMind Ah, I do think bounded inversion is continuous so this makes sense.
04:22
@ACuriousMind Toilet math: $$\| \psi_t\|= \| (L_t)^{-1}\gamma_t\|\le \| (L_t)^{-1}\|\cdot \|\gamma_t\|.$$ Now since $t\mapsto L_t$ is continuous in $\mathscr B(X,Y)$, the set of norms is bounded. But apply this and use the same logic on the inverses to conclude that the norms of the inverses are bounded. Thus $$\|\psi_t\|\le C\|\gamma_t\|\to 0.$$
However, one must use the fact that $L_t$ never hits the zero operator, which is true for $t$ close to $\infty$.
3.5
3.5
04:34
waddup physics fellows
@goodnight No one here knows any physics
Ah
You're just the guy who changes name every moon
who?
IceLord, Blue, 3507, so on
wait
those are the same person!?
04:49
?
Come on
who is that
wait ur saying this isn't the krusty krab
A young physics major at UoT ;)
idek what physics is
i'm doing aboriginal studies
:p
That just makes you even more of a physics major tbh
alright
waddup are you at waterloo
04:53
you're not doing math or physics?
lol
I am :p
ok
non-stem people are not allowed here
@goodnight Nope, I'm living in Santa Barbara
tfw ur a leaf
Embracing my ultimate failure
04:54
@BernardoMeurer work?
oh right
did you apply to waterloo
The lowest of the low :)
@goodnight Dude what is with these names
apps close in jan
04:55
I'll apply for transfer
@BernardoMeurer did you watch community
But I'll finish the year here
Nope
Did not watch it
well you don't need to since you're basically living it
that's not a bad thing
@BernardoMeurer but applications
are due in JAN
even for transfers
that's two months out
what is your issue?
I am aware. That means I'm not applying to waterloo this year
04:56
??
I honestly don't even know what I'm doing with my life anymore
living it?
I suppose
@0celo7 well it takes a long time
my life has no meaning since ACM became a coder
@goodnight ??
04:58
kek
@BernardoMeurer Ok I will call you on Sunday
let's talk
can I talk too
Who are you?
you tell me
@0celo7 Thanks
@0celo7 You have his number? o_O
04:59
dude are you fried
he's been over this a billion times
@SirCumference I say this in the nicest possible manner, but you don't seem to be the sharpest tool in the shed.
I'm so confused...

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