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18:00
after all, the canonical algebra is always determined by the kinetic part of the Lagrangian
free or interacting, the algebra is fixed by the form of the terms with derivatives
and those are usually the same for free and interacting theories
Oh so it is a valid assumption?
it's just the unitary thing at $t \neq 0$ that isn't?
what do you mean by valid? :-P
IMHO, it is reasonable
Is it mathematically objectionable
yes, like everything else
I mean obviously yes, physically the interacting theory will be somewhat similar to the free theory
but that's a far cry from being rigorous
18:03
but you can derive Feynman diagrams directly from the CCR, so I'm willing to accept them as good enough and move on :-P
But the only other way to get them is via the path integral, which is also not rigorous
screw path integrals
I'm fine with not too rigorous assumptions, but I would like to at least know what those assumptions are
the assumption is that $[\phi,\frac{\partial\mathcal L}{\partial\dot\phi}]\sim\delta$
for any theory, interacting or not
"As already mentionned, this is not possible. The field $\Phi$ must be more singular than $\Phi^0$ and this manifests itself afterwards in the need for an infinite renormalization of $\Phi$. The magic formula refers to the "unrenormalized field" $\Phi_u$. The true field is then written as $Z^{-1/2} \Phi_u$"
18:06
@JohnRennie lol
So yes apparently the $\Phi(x,0) = \Phi^0(x,0)$ is bullshit
Oh wait, there's more!
What are you talking about?
"Actually the justification of the last step is not possible. The vectors $e^{iH_0t} \Omega$ converge only weakly to a multiple of $\Omega_0$. The operator between the bars depends on $t$ and $t'$. As a consequence, it does not converge as $t$ or $t'$ tend to infinity."
@0celouvskyopoulo7 The interaction picture
And why it's all a lie
There are many reasons, apparently
it is the greatest lie that was ever told
You mean besides the whole "it was a virgin birth" thing?
I don't think they assume a virgin birth at all in QFT
So I think the three big lies to make QFT work are
1) you can multiply distributions fine
2) The field operator and the free field operators are kind of the same
3) The vacuum state is gonna be similar to the free vacuum state
Those are the three lies of QFT
18:16
I really dont think you need 2&3
sure, some people use that
but they are dispensable assumptions
what do u use instead, if you use the Hilbert space formalism
The path integral formalism doesn't assume that but it has other lies
QFT books are very bad
I have to write one of my own
Don't we all
QFT is wrong
18:18
well yes
I know
There are no lies in GR
cf above
QFT is wrong but its fun
and many of its ingredients can be as rigorous as you want
It's unfortunate that GR is perfect and QFT is awful when we can mostly test for QFT
But, why
How do physicists use provably false things?
How does their conscience allow it?
18:21
"provably false" != "morally false" :P
Guys, maybe a silly question, but Newton's second law basically states that we can add forces vectorially. However, (when mass is assumed constant) force is $F=m\frac{d^2r}{dt^2}$. Can't we just say that since position vectors can be added vectorially, then velocity and acceleration vectors can be added vectorially too, and if you multiply by a scalar (i.e., mass), this can be added vectorially too?
I get a stomachache if I use something that I know isn't completely true or whatever
Or if I doubt it's true
Maybe I should make a PSE post to check
@ShaVuklia That's not what the second law says
It just says $F=ma$
What about addition?
what if $m$ is actually a matrix?
MOND, V.2
18:23
@0celouvskyopoulo7 well it technically says $F_{\text{res}}=ma$.. but we already defined $F=ma$ for a single force.
$\boldsymbol F,\boldsymbol a,\boldsymbol v$ and $\boldsymbol r$ are all vectors
Did you have a class on that?
@AccidentalFourierTransform Jesus Christ
Italic bold?
oh no
you are one of those
@ACuriousMind Can I insult him?
18:24
@ShaVuklia In joshphysics' formulation, the point is not that you can add force vectors. The point is that the total force on an object will be the sum of the forces from the "isolated" interactions, and not something else.
@ShaVuklia Part of the definition of force is that you add forces vectorially.
That's what we mean by "force is a vector"
You have axiomatically no reason to believe that the sum of the isolated force vectors will be the total force - and that's what the second law in this formulation does.
@ACuriousMind What?
The axiom is that forces are vectors, hence you add them.
what do you call a duality with three things?
@AccidentalFourierTransform triality
18:26
Then the law says the total force (axiomatically the sum of individual forces) is the acceleration.
I've seen Witten use it, it must be a word :P
oh then Im totally using it
Yes, there's an SO(8) triality.
@ACuriousMind English to Witten dictionary takes a whole new meaning now
but how do we know then that we can add velocity vectors vectorially?
@0celouvskyopoulo7 I think we're trying to say the same thing.
@ShaVuklia They're...vectors. Of course you can add them, that's part of the definition of a vector
18:28
but a single force is also a vector by definition...
I need a new punny math username
And you add forces
Please help
I'm confused what the confusion is
And why this is so important to you
@ShaVuklia Yes, and you can add force vectors.
18:28
@ACuriousMind Admit it, you don't read what I write
CisIsJustAPhase
cis is a less commonly used mathematical notation defined by cis(x) = cos(x) + i sin(x), where cos is the cosine function, i is the imaginary unit and sin is the sine. The notation is less commonly used than Euler's formula, e i x {\displaystyle e^{ix}} , which offers an even shorter and more general notation for cos(x) + i sin(x). == Overview == The cis notation was first coined by William Rowan Hamilton in Elements of Quaternions (1866) and subsequently used by Irving Stringham in works...
@ShaVuklia Did you even look at Arnold?
@AccidentalFourierTransform That's gonna get me banned
@0celouvskyopoulo7 I'm reading Goldstein
but maybe I should, though I thought it was too difficult for me
let me recheck
18:29
@ShaVuklia You need to read Arnold.
@AccidentalFourierTransform Should be pretty obvious
The abstract formulation of Newtonian mechanics begins with the Galilean group on an affine space.
@ShaVuklia The second law doesn't say "you can totally add force vectors", it says "the sum of the individual (isolated) force vectors (the "total force") is equal to mass times acceleration".
The thing isn't that you can add forces, it's that their sum is actually physically meaningful and equal to $ma$.
ok, maybe Arnold is doable for me (i have it in front of me now)
Hehehe, maybe Arnold is doable
18:32
@ACuriousMind give me one sec to let that sink in
huh
actually affordable
oh
it's not even that long
I'd be better off reading Federer
0
Q: QFT and its lies

SlereahI have been trying to figure out all the erroneous assumptions of QFT (as performed in an operator theory) that allow it to function as it currently is. So far, the three big candidates I found are these : The product of distributions is allowed in some sense (this runs afoul of Schwartz's imp...

a good title
@ACuriousMind can you give me vamp powers pls
One last try then; A force $i$ is by definition: $\vec F_i=m\frac{d\vec r_i}{dt}$. So for the vector sum of all forces $i$ on some object with mass $m$, we get: $\sum_{i}\vec F_i=\sum_i m\frac{d^2\vec r_i}{dt^2}=m\sum_i\frac{d^2\vec r_i}{dt^2}$. However, just like we can add position vectors and velocity vectors, we should be able to add acceleration vectors. So we simply get $m\frac{d^2\vec r}{dt^2}$, where $\frac{d^2\vec r}{dt^2}=\sum_i\frac{d^2\vec r_i}{dt^2}$.
what is Schwartz's theorem @Slereah
@ShaVuklia No need to put vector arrows
18:37
ok
Schwartz's impossibility theorem states that you cannot have a differential algebra on the space of distributions.
or use index notation if you have to
@Slereah By differential algebra you mean an algebra with an endomorphism acting according to the Leibniz rule?
There's no algebra on distributions that satisfies the Leibniz rule for derivatives
yes
in my eyes, we are just adding acceleration vectors, so I don't see what exactly it is that Newton's second law is giving
The distribution algebra as they are done today get around this by having some products not be distributions
18:39
why do you always say "interactive" instead of "interacting"?
@ShaVuklia A headache, that's what it's giving
sigh:P
I'll correct it
Why do you want a differential algebra?
@AccidentalFourierTransform Probably French something
@0celouvskyopoulo7 Apparently, I only need to know about differentiable manifolds
18:40
@ShaVuklia The point is that you defined the $F_i$ from the accelerations in isolation. The second law is in a setting with many different objects that are not in isolation. You have, from the axioms so far, no reason to believe that the sum of the forces (or accelerations) in isolation should be the actual total force/acceleration in this situation. That it is is the content of the second law.
@0celouvskyopoulo7 Well to solve PDEs you usually want to be able to use derivatives
@ACuriousMind RIGHT, thanks. I think that answer suffices
@BernardoMeurer What?
@0celouvskyopoulo7 What what
18:42
You only need to know about differentiable manifolds?
I need to remember I'm doing physics, and not just maths:P
As opposed to what?
@ShaVuklia Bah
Do math
none of this crap in math
People always explain exactly what they mean, there's no ambiguity, and no errors
@0celouvskyopoulo7 Yes, for Analysis II
@0celouvskyopoulo7 that's why maths is fundamentally less exciting than physics, I think
at least for me
(i) I was joking
(ii) that's a terrible opinion if true
18:43
haha oh sorry:P
@0celouvskyopoulo7 You should've used an irony mark there :P
All your fields are shit
Computer Science rocks
Pffh, astrophysics is best physics
Whatever Quavo does is the best field, tbh
the best field is $\psi$
18:44
The best field is $\Bbb C$
1+1=0
delete that
you have two flags already
@Slereah haha that comment
haahahahahahah
18:45
delet this
@AccidentalFourierTransform Me?
Wait why
In the pertubation expansion the terms are large (infinite) and need 'renormalization'. — lalala 4 mins ago
fucking physicists, honestly
18:46
infinite is fairly large
@AccidentalFourierTransform Why did you make me delete that...?
You tell them their theory is shit and then they do something more shit to get out of it
@0celouvskyopoulo7 Quavo is shit
@SirCumference trolling is a art?
@AccidentalFourierTransform ...I hate you
I'd think there'd be a rule about claiming flags when there are none
@SirCumference Please delete this.
@SirCumference There is.
@ACuriousMind would it be an equivalent second law if we said that the force vector associated with an interaction in isolation is the same force vector when there are other interactions as well?
@AccidentalFourierTransform not a troll, just showing how bad your grammar is
18:49
@AccidentalFourierTransform Do you think the content of that link is appropriate to post here?
lol, didnt read past the first paragraph
delet it pls
Maybe...read further next time :P
@AccidentalFourierTransform No, I think your is correct.
Ahahah
I just got a downvote
rob
rob
@0celouvskyopoulo7 You're correct: your's correct.
18:51
@rob Of course it is.
He's trying to troll me.
Some QFT lad is mad
@AccidentalFourierTransform What is your comment supposed to mean?
@Slereah Well...when I saw the title I immediately hovered over the downvote button until I had read it :P
The title was non-negotiable
clickbait
@0celouvskyopoulo7 idk
18:54
I really need to be studying
What am I doing with my life
Why does this chat exist?
@0celouvskyopoulo7 Without this chat I would spend too much time actually doing things
Which will inevitably lead to world end
@0celouvskyopoulo7 To trap people like you, apparently :P
@BernardoMeurer You still haven't told me why you "only" need to know smooth manifolds, or what you need to know about them.
Ah, yes, and to distract Bernardo from achieving total potato dominance
@ACuriousMind Have I told you my latest step towards complete planetary destruction?
@0celouvskyopoulo7 Because that's all my course covers apparently
18:55
@BernardoMeurer You punched your wall and bloodied your hand? :P
And I don't know, I learned how to prove something is a smooth manifold
That's not what smooth manifolds are about
@ACuriousMind Yes, no. I got an FPGA and have been doing work on it :P
What did you learn about them?
Why does force exist?
18:56
@0celouvskyopoulo7 I don't know what they're useful for yet
I learned parametrization
and path gradients (?)
@BernardoMeurer I read your bragging about running linux on it, yes
@Abcd Because otherwise the world would be pretty boring.
@ACuriousMind Yes, I will continue to brag until I run doom on it
@Slereah Does a metric like $$g_{ij}=\left(1+\frac{\mathcal M}{|x|}\right)^4\delta_{ij} +p_{ij},\quad |x|^2|p_{ij}|+|x|^3|Dp_{ij}|+|x|^4|D^2p_{ij}|\le C$$ look like a decent enough metric on a Cauchy surface?
@ACuriousMind Serious answer please :/
@Abcd Why should he
18:57
@0celouvskyopoulo7 No, that metric looks very indecent to me
@0celouvskyopoulo7 wat
@0celouvskyopoulo7 Why shouldn't he?
ugh you two
@Abcd I don't know what a serious answer would be. Why does anything exist?
@ACuriousMind Because God decided to make it.
18:58
@0celouvskyopoulo7 Ah! that's cool.
@Slereah This is allegedly isometric to Schwartzschild when $p_{ij}\equiv 0$
is that obvious to you?

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