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01:10
I am trying to perform this variation, but to no avail.
i set up a lagrange-esque multiplier thing with $\delta S/V + \lambda_1 \delta E/V + \lambda_2 N/V = 0$, but I get a strange result at the end.
i compute that the above expression implies that $\log(n(1-n)) + \lambda_1 + \lambda_2 \epsilon = 0$
if i exponentiate, then i get $n(1-n) = \exp(-\lambda_1 - \lambda_2 \epsilon)$
meow
01:41
m e o w ~
 
2 hours later…
03:58
Can someone tell me how to get Maxwell equations in free space in tensorial form from $d*F=0$?
Most places discuss how to go from differential forms notation directly to vectors $\vec{E},\vec{B}, etc.$ but not to the $\del_mu F^{\mu \nu}=0$ thing
I plugged in the definitions of $*$ and $d$ to get a $\varepsilon_{\mu \nu \rho \sigma}\delta_\eta F^\rho \sigma dx^\eta dx^\mu dx^\nu=0$ from $d*F=0$
 
3 hours later…
07:02
@NairitSahoo To get to the standard form you have to dualise again, ie compute $\ast \mathrm{d} \ast F = 0$ and use the identities for products of 2 $\epsilons$
 
2 hours later…
09:07
Good morning, folks :)
1
Q: Is drift velocity defined at a point in space or defined for a region?

Sachin BhargavaJust wanted to verify if chatgpt is being correct here in all these 7 convos... I'm really sorry if this violates any community guidelines, I did not had that intention

unbelievable
09:26
hey :)
 
1 hour later…
10:55
yo
 
1 hour later…
12:07
hi
 
2 hours later…
14:08
how do you feel about statements like "reasoning is not the only way to approach truth"?
this statement is usually used by theists in god debates
14:39
@TobiasFünke unfortunately, entirely believable, this is the logical outcome of the "AI" hype. Welcome to the future! :P
Turns out that the category of simplicial sets is a nice little toy model for cohesion
Where the "cohesion" is just when you have a little edge between two points :p
Although I'm not entirely sure how it deals with "non-concrete" sheaves
I think it may be spaces with "wild" cohesions like "more than one edge between two points"
Crazy
Since the "codiscrete" space is just "the simplicial set that has an edge for every two points"
Hence more than one will fail to be injective
15:08
@TobiasFünke Since I refuse to read what chatGPT says about physics, will you tell me what's unbelievable? The AI reply or that a user asked if the AI is correct?
@SignorFeynman the latter
15:32
does anyone know where the expression for entropy of a normal fermi liquid comes from?
15:50
@TobiasFünke and you have to consider that this is already one step above the worst case, which is just believing what it generates without trying to check
It's a turbocharged version of the crackpot problem - it has always been easier to produce nonsense than to debunk it, but now it's additional orders of magnitude easier
is (3.4) supposed to be the other way around?
so that the integrand is $\lvert p \rangle \langle p \lvert q \rangle \langle q \lvert$
oh wait no
16:08
@ACuriousMind we must train the machine on Duffield's book
16:29
It has been quite a while since vzn ( @vzn ) posted, we're talking during covid times, unfortunately I think the worst can be presumed... I'll just say despite the raucous debate (something we all agree to in these scientific discussions) and the kinds of typical half-cocked layman mistakes, it was always fun chatting with vzn and I appreciated their desire for open-mindedness/truth
16:56
I am a little confused by this message, bolbeteppa. That user has been inactive for 274 days, which is a couple of years later after the pandemic
Also people sometimes just stop coming?
without even perishing
17:29
hopefully they r well
@SignorFeynman I don't think that 274d thing is right, the 'recent' tab gives 2021 as the most recent activity but that 274 days thing says that was when the last message was... Activity everywhere (blog etc) all just disappeared/stopped in the middle of a global pandemic
Mhhh, In 2023 there was this message mhhh
Sep 1, 2023 at 19:46, by user 726941
Wow, vzn has been gone for ~671 days?
There is something wrong with the last seen, then
17:51
Judging by the blog about page and the chats here, he was an older software engineer who had the fire of vishnu lit underneath him to understand theory but didn't study it properly, activity stopped early in 2021 and the vaccines didn't come out until the end of the year en masse
Obviously anything could have happened, but yeah...
I am glad that I (and ACM etc) am opposing his claims on his research page :p
Ah, I see :(
I wouldn't call him a crank, but he was always veering down that road but kept it within bounds to be able to talk here
46
Q: Why are most cranks old men?

AllureWhat To Do When The Trisector Comes claims that most cranks (for lack of a better word) are old men (trisector refers to a specific type of crank): One obvious characteristic of trisectors is that they are old. The typical trisector heard of the trisection in his geometry class, but did not s...

i am feeling bad reading his blog. he is really enthusiastic
life is meaningless just like that
18:10
If you read between the lines, I was trying to tell vzn not to waste his time doing physics without studying it properly (pretty sure I directly said to read the basics multiple times in here), this stuff is no joke, it's hard enough when you know the basics let alone ignoring them and plowing into it
> "Twelve-thousand working hours! Full-time is forty hours a week for fifty weeks, so the poor deluded man had devoted the equivalent of six years of his life to something as useless as trying to find two even integers whose sum is odd."
On that note
19:06
Questions:

1.) How would you with an equation describe a canonical transformation?
Is it $\delta f = \epsilon \{f,G\}$ where $f$ is some function $\epsilon$ is some incremental change and $G$ is the generator?

2.) Is the time flow a canonical transformation with the Hamltonian as the generating function?
19:20
The field whose excitations are photons, is called a massless spin1 vector field. At the same time it is also a gauge field?
hi meow
@Slereah well unless you're in new york
people really insist there's a difference between bagels and pizza in new york vs other places
personally i don't really see it
@imbAF yes, all massless spin-1 fields are gauge fields, we've been over this: chat.stackexchange.com/transcript/71?m=67055988#67055988
@User198 there are several slightly inequivalent definitions of "canonical transformation", if you pick one where they are the symplectomorphisms, then yes, all such transformations are the flows of Hamiltonian vector fields
Uh, perhaps there needs to be a "locally" there - this is false on non-simply-connected phase spaces
19:43
If we consider curvature coupling terms like $R\phi$ for a Klein-Gordon field in curved (but non-dynamical) spacetime then there are certain values of the coefficient for which the theory is conformal. So $T:=T_{\mu}^\mu=0$. Now I was thinking that if I now make the gravity dynamical, $T=0$ implies that $R=0$ (via contraction of Einstein field equations) that is the curvature coupling vanishes. Is this correct line of thought or am I messing up the different notions of energy-momentum tensors?
This would be a strange conclusion, right? Gravity when made dynamical decouples "conformal scalar" with itself or something like that. (Although there's still minimal coupling...)
Hi, Sanjana. Long time no see
Hello everybody
@Sanjana That is correct
in a conformal theory you will lack some degrees of freedom in GR
Hii @SignorFeynman how are you? Yeah I just got stuck in some admin-like duties at school. No time for physics :(
@Slereah Oh wow. Do you have some other examples or some generic argument in mind for that?
19:57
Wait am I even right or am I thinking of the Cotton tensor
let me check some things
The thing I have in mind is that in GR, you have roughly two components to the curvature, you have the dilations (volumes change), which are indicated by the Ricci scalar, and you have the shears (squeezing) which are indicated by the rest of the Riemann tensor
@ACuriousMind So the excitations of gauge fields are vector bosons? And all gauge fields are interaction fields among excitations of other fields which are not gauge ones i.e two spin1/2 field?
yeah I think you just have R = 0
It's not that wild, you have plenty of real fields which are conformally invariant?
Like the EM field
You can check that the Ricci scalar for the Nordstrom black hole is zero
@imbAF I don't really like calling particles "excitations of fields", but yes, that terminology is common enough. I'm not sure what you mean by them being "interaction fields" - there is nothing else to interact with in free EM, for instance.
I am trying to ask you if
gauge fields are a representation of particles which facilitate interaction
i.e photons between fermions
I don't know what that means
20:06
ok
In QED the electrons and photons interact. It's common to call the photons the "mediators" of the EM force because the Coulomb force comes from a diagram where "two electrons exchange a photon". But you can have plenty of interactions between particles that don't involve gauge bosons (just write down a theory with two scalars $\phi_1,\phi_2$ and a term like $\phi_1^2\phi_2 ^2$)
@ACuriousMind in the pocket of big Higgs
I thought that interactions are made possible only, exclusively via gauge fields, the massless spin 1 vector field for interaction among charged particles, the gluons among quarks etc
@Sanjana The irony of life is to keep having frictions when I'm studying superfluids :P
@imbAF It's true that in the Standard Model, all the interactions are either via gauge bosons or things that come from gauge bosons (the W-/Z-bosons of the weak interaction are massive and hence not directly gauge bosons, you will learn about that when you learn the Higgs mechanism). But it is not a general rule in QFT, as I said you can easily write down interaction terms that do not involve gauge bosons.
20:12
You can write down such terms, but does that mean, you encounter such scenarios in nature ?
as I also just said, not in the Standard Model
I've heard of BSM, but I am not sure if you mean that?
For example in the $\phi^4$ theory which imbAF should already know, the scalar field interacts with itself via scalar fields
but they can appear in effective theories, e.g. the 4-fermion vertex of the Fermi theory of weak interaction
My connection is lagging, so I may be a little late
20:16
One additional question. I might butcher what I am trying to say but hopefully you get the idea
A theory, the way I understand it, is represented via the lagrangian density. A free such lagrangian only "contains" in its description one type of particle (excitation). For a lagrangian which also contains an interaction part, this lagrangian involves 2 or more theories/ qfts in its description. In other words 2 or more different excitations
@Sanjana Also remember that you don't even need it to be conformally invariant for that to work
Oh wait I am being wrong
nvm
Thought the massless case might also be of zero trace due to being scale invariant but apparently not
hiya tobias
21:03
@imbAF no, as I said before you can have a self-interacting field
Well, a self interacting field would be an exception
$$\mathcal{L}=\frac{1}{2}(\partial_{\mu}\phi)^{2}-\frac{1}{2}m^{2}\phi^{2}-\frac{\lambda}{4!}\phi^{4}$$
I just replied to your question
in the sense that all the particles involved or that belong to the theory
are of the same type
Which means only one type of excitation
21:17
does anyone know what the meaning of forward scattering is here?
this is in the context of motivating landau fermi-liquid theory
does it mean $\lvert p_1 \rangle \otimes \lvert p_2 \rangle \mapsto f(x,x',x'',...) \lvert p_1 \rangle \otimes \lvert p_2 \rangle$?
where $f$ is some generic function

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