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00:06
@Slereah I think you mentioned some of this stuff recently johncarlosbaez.wordpress.com/2024/10/31/bradwardines-rule
00:23
in the discussion of macroscopic mawells in jackson, he mentions that the equations vary wildly on atomic length and time scales. However, he only ends up doing a spatial average. What about a time average?
 
1 hour later…
01:47
@Mr.Feynman that's more meow meow than ACM
@SillyGoose On the chapter that he analyses that, he specifically covered the time average and found that it is not sufficient to solve the problem, whereas for any time slice, spatial averaging suffices.
That whole thing is a mess; even if yes, that is technically an interesting result, that is nowhere near how anybody would be attempting to solve for real physics.
@ACuriousMind miao miao would add that multipole expansion is the harmonic extension of Laurent series, famous from complex analysis, to 3D.
@Mr.Feynman you've put in such incredible amount of effort...
@Slereah I dont know what you mean; I would think that Caesar had to have enough interest in the issue to come up with what we honour him as the Julian calendar.
02:08
I don't think he personally made the research
02:32
That is definitely the case, but there must at least have been people knowledgeable enough to provide a smart enough person to come up with the system
Also, @Slereah, on your blog page samuel-lereah.com/articles/Physics/… , where, ignoring the trivial bit that the exponential of Hamiltonians that you have right at the top is missing the time factor and imaginary unit, and that the interacting Hamiltonian forces you to include the time ordering factor too, the next line is also in violation of BCH. Or rather, you might be interested in Zessenhaus' formula, or Magnus's expansion.
 
3 hours later…
 
1 hour later…
06:57
hi
07:14
what r the main defining physical features of the universe in ur view
i have arranged fundamental features of the universe into tiers
tier 1- locality, uncertainty principle
tier 2- principle of least action, local poincaire invariance
tier 3- gauge group U(1)xSU(2)xSU(3), Higgs mechanism
tier 2 should also have General Relativity in it
what would be the tiers according to u
this is in the Non Humean framework of physics. according to non Humeans, the laws of physics have other fundamental laws behind them
08:07
@Slereah would you be interested in working for this company?
 
2 hours later…
10:31
I would not
@RyderRude The quirk is, science is about criticizing and editing itself. We surely have not found the true physical laws, and even after we'd found them, we cannot confirm we did.
That's how the string theory rendered to be a fad.
@DannyuNDos why are you talking facts to someone who is trying to tierzoo physics?
10:48
*Cough*
10:59
Wow, nR MBT is so different from QFT. Green's functions having a physical meaning
I wonder, is there nothing like the LSZ in MBT? Or is it that the S-matrix is not relevant for condensed matter people?
Don't put too much effort in answering these questions, in case you decide to. They're just things I'm wondering now
@Mr.Feynman The S matrix calculation is relevant to cond mat too. Why would you think it is not? In particular, the Euclidean propagator is the partition function.
The euclidean propagator? Not the euclidean action?
Yes. It is actually a LOT different. There is no LSZ because it is not about particles coming in from infinity and scattering to infinity
I was wondering that because unlike QFT, in many-body theory (which is my focus, probably it was wrong to say condensed matter thereafter), they calculate observables using Green's functions, which do carry a physical interpretations because of obvious reasons I'm lazy to mention :P
@naturallyInconsistent Since I learned about relativistic QFT first, I was a little bewildered when I encountered the MBT version :D
@DannyuNDos yes. my analysis is about physics as we know it, what has been tested so far
11:06
Instead, you are dealing with "greens functions" that is not between vacuum states, but rather is between ground state. It is about correlation between excitations at different spacetime points
And these correlation function turn up in Kubo relations
@naturallyInconsistent what is ur problem??
That's another great point I've raised a few days ago. Even if you can write down an algebra with respect to which the Fermi Sea is vacuum, it is not the Fock Vacuum: it's not the "same" GF hep people would consider
Oh no they're about to flame D:
Calm down, people.
There is a LOT of mess because, for example, I was asking a senior colleague about Mahan's assertion that the 2-point correlation function is unphysical, not least because in basic SR QFT the 2-point Green's function is very important, and he was like "textbook authors can write whatever nonsense they want..." and miao miao immediately realised that it would not be useful to discuss that with him
@Mr.Feynman that wasnt going to happen
@Mr.Feynman The problem is, which Fermi sea? The Dirac's one cannot work.
@naturallyInconsistent I'm not sure "Fermi sea" was a correct choice of words; I meant the g.s. of an electron-many body system, i.e. filling the levels up to $k_F$.
11:12
@Mr.Feynman Yeah, that is an extremely important thing to keep in mind.
@naturallyInconsistent In relativistic QFT it is definitely unphysical in the sense that it carries no suitable interpretation whatsoever: no particles propagating from there to there. There is no position operator, at least not in standard presentations
In MBT they seem to give a proper physical meaning, as discussed in section 7 of Fetter&Walecka; the idea is the same of rQFT book, just this time a position operator is defined
@Mr.Feynman But you cannot say that. The 2-point GF in basic SR QFT is the single particle propagator that you have to renormalise with all the bubbles. It is extremely important to get correct.
Unphysical is not unimportant; I mean not observable :P
But a single particle propagator is the thing you use to define the dayum observable.
@Mr.Feynman it has a physical meaning in rQFT but in terms of fields rather than particles. u would have to think of fields as observables
then it just becomes an expectation value
there is a post about measuring this
11:16
The LSZ links what is observable (scattering amplitudes) to unphysical objects that are defined mathematically (Green's functions)
1
Q: How are general quantum correlation functions actually measured?

knzhouThese days, the majority of work in theoretical particle, condensed matter, and AMO physics is about methods for calculating exotic correlation functions, of the rough form $$G_{ij} \sim \langle \mathcal{O}_i(t) \, \mathcal{O}_j(t') \rangle$$ though possibly also including time ordering, (anti)sy...

@Mr.Feynman it is not unphysical. fields are the fundamental observables
I'm afraid that's about condensed matter, which if you read is not what I'm currently talking about.
yes, i just noticed
@Mr.Feynman You must first have specific forms of the GF, then you can have LSZ act on them. In particular, if you use the infraparticle way to get the free-field electron get the Coulomb field around them, then the propagator is no longer the usual k^2-m^2 kind, and boom, your LSZ is fucked up
i will try to find something about rQFT. im positive that fields are observables
11:20
I really think the equivalent to LSZ in cond mat is just Kubo relations. You can just extract so much info from the correlation functions using Kubo just like how you use LSZ on GF.
Fields are not even hermitian...
@naturallyInconsistent Ah. More to read about it?
@Mr.Feynman their real and imaginary parts are hermitian
also, electric field is def an observable
@Mr.Feynman Infraparticle is the search term. I really really don't understand the whole structure, only that it is such a headache to work with.
I'll keep in mind for the future D:
@Mr.Feynman why do you even want to read from him? The amount of nonsense being spewed is just beyond refutation; I'm low-key holding back from labelling them as inappropriate.
11:22
I reply if I'm pinged typically
@Mr.Feynman You might want to low-key forget about them. ACM also said that he isn't into that; apparently, the winning move is to ignore those; the usual formalism with infrared renormalisation is sufficient to get good answers.
Oh, it's definitely not on my top priority list :D
13
A: Is the S-Matrix the only quantum field observable?

Matt ReeceCorrelation functions of local operators are the other observables that field theorists talk about most of the time: things like $\left<{\cal O}_1(x_1) {\cal O}_2(x_2) \ldots\right>$. But there's no shortage of observables in quantum field theory. The situation where you'll hear people say that ...

I learned a Chinese word yesterday
11:25
this answer says that correlation functions r observavles but he doesnt give any sources
I'm kinda amused that my tierzoo comment got starred. Like, I've specifically avoided casting any vote on the complaint that pinged meow too. If someone else was wanting to flag it, it would be funny.
@Mr.Feynman which is it?
in general, note that observables must be local smearings of fields or one would violate causality
@naturallyInconsistent 奶
Milk
this is the idea in Algebraic QFT. S-matrix is an approximate idea
@Mr.Feynman ... lots of fun ...
11:27
@naturallyInconsistent Context
@Mr.Feynman of course, the fun is all in the context miehehehe
Funnily enough, it is pronounced like the Japanese word ない, which means "there isn't"
heh
@Mr.Feynman also, there is a lot of inappropriate (racist) jokes just awaiting exploitation
and miao miao can say it; you likely cannot
@naturallyInconsistent I won't indulge in such mundane pleasure 💀
@Mr.Feynman just yesterday miao miao sent a new vocab to my friend: prurient
11:30
Ah, it means lustful
turned up on the court case that qwerty sent here: the "I know it when I see it"
miao miao iz just like, hmm, fun vocab, snatch
@Mr.Feynman i've heard stories of anglophones going to france/italy, trying to order a caffè latte by asking for a "latte" and ending up with plain milk
@qwerty lol yay~
lack toast in toblerone~
@naturallyInconsistent that's a very good bone apple tea
miahahaha
anyway, if you have more questions, send them quickly. miao miao is about to have to go for a massage at the gym
how are the two of you?
M I A O ~
Anyway, @Mr.Feynman in RR's latest link, there is an answer that Ron Maimon gave a comment that goes into slightly more detail: namely that even though an S-matrix itself is not an observable in one sense of the word, it is an observable in another sense.
11:58
@naturallyInconsistent I'm doing well, thanks :) remedial physics/maths reading :p
12:27
it is about the historical development of the principle of least action
"how many prefixes can we attach to `-morphism'?" -- Mathematicians, probably.
i've been told to understand DG I need to first read category theory
@qwerty Well, yes. Although abroad "latte" is caffè latte (I guess), here it's just the word for milk.
Similarly, if you step into an Italian bar and order a caffè (coffee), you will get an espresso
@qwerty I...don't think that's true in any defensible sense :P
(and I like category theory)
@qwerty Bullshit. Knowing category theory is good and helps but it's far from being fundamental
@qwerty i think category theory is suposd to be learned after u have learned all other branches of math
12:39
@ACuriousMind ok, I misrepresented, I started reading DG and writing down my List of Definitions including you-know-what, and I got suggested to read category theory
And even then, for basic DG, all the category theory that would be useful (not fundamental) is like the very basics: understanding what morphisms and functors are, so you understand that you're really defining the "same" things over and over
this is what mathematicians told me
@qwerty still a pretty weird suggestion, imo
one should learn linear algebra, abstract algebra, topology and differential geometry stuff before learning category theory
Like, with category theory you will understand that (in a given sense) there is no difference between a diffeomorphism of manifolds, an isomorphism of bundles, a vector space isomorphism: they're all isomorphisms in the sense of the given structure
Concerning functors, you may grasp a better idea of what a pullback is and what a pushforward is, but that's about the amount of category theory that I've encountered in DG
@RyderRude You can arguably get away with the basics of the first three (i.e. just the definitions of the structures)
12:43
@Mr.Feynman i didnt mean this as in pre-requisites for category theory. but more like : after u have learned this stuff, category theory helps u see connections between them
oh, okay
@ACuriousMind the culprit mathematician: "In my defense, I know qwerty and I know how she tends to understand things"
So your real name is qwerty :P
When all's said and done, the suggestion is like "you need to study Lie theory before learning QM"
probably I'm not going as deep as you all think :P I'm just reading wiki and SEP right now
that is a good analogy. lie theory only enhances Qm understanding after u have already learned qm
12:46
I know it's a good analogy, I'm never wro-HELLO @Relativisticcucumber
@qwerty My favorite one is itchyomorphism for a Poisson preserving morphism
@ACuriousMind That's some New Math shit
Surely the children will understand addition better if they are taught set theory
@Mr.Feynman 奶茶!!!
Slereah talks about math like Jesse Pinkman talks about meth
@Relativisticcucumber !!!
@Mr.Feynman I do like putting things in boxes. Actually I like real physical boxes too. I started bookbinding once and ended up making boxes once or twice... I may not like cats much, but they have the correct take on boxes...
@Mr.Feynman こんにちは
did i get it right? i know no japanese
12:50
@Slereah that's a punny name lol
It's not a very commonly used one, but I decided to spread it more
@Relativisticcucumber こんにちは。キュカンバーはどうですか。
Yes
wow wait i just seem to have learned ciao is hi AND bye
$$\mathrm{Poiss} \overset{🐟}{\longrightarrow} \mathrm{Poiss}$$
@qwerty You may not like cats but you are a cat deep down
12:52
everyone must like cats
Quantomorphism is also a good one because it sounds fake
@Relativisticcucumber Why is everyone so astonished that ciao is also a way to say bye?!
0.o i was shocked that it means hi actually
i think theres an impression that it means only bye
for example, theres a famous song that says "ciao adios im done"
@Fermion hi
12:53
Incidentally, the italian verb for "say hello" is "salutare", which also means "say goodbye". I'm very triggered by the fact that in English there is a single verb for "say hello", i.e. "greet" but not one for "say goodbye"
"farewell" is a bit too much :P
@Mr.Feynman wow never thought of that
hi @RyderRude
yeah i guess "bid farewell"
@Fermion did u just join the chat
even then tho bid cant stand on its own so this is a valid problem
12:55
I mean, yes, but it's kind of dramatic :P
George Carlin had a whole bit about how you could beef something up but not beef it down
Farewell is also a verb on its own, by the way
I think
@RyderRude yes
No, it's not D:
Then "bid farewell" be it
@Fermion we discuss physics, math and sometimes philosophy
and other casual things too, like rn
12:56
wow this q has been asked precisely reddit.com/r/words/comments/w9idvk/…
SO FAREWELL CAN BE A VERB! YEAH!
ok i migrate to condensed matter ,,,, ciao 朋友们
Bye bye, friend
I recognize only the second hanzi from Japanese :P
@Slereah It's probably the best way, yeah. I always forget about it, though
Not a single word though :P
12:59
it is lexicalized :p
How do I get the right to make up a word? :D
Just do it and see if other people go with it
From now on "bye" is a verb
Worked for Shakespeare
I guess I'm ancient
13:03
anyone see The Exorcist? is it still good
@Mr.Feynman i couldnt resist:
Sorry as far as movies with Linda Blaire go, I only like
@Relativisticcucumber top tier meme
@Relativisticcucumber I don't know if you know Liam Carpenter. He makes stereotypes videos about Germans (he's an Englishman living there)
And at the end of the end of his videos, Germans typically make a slight smile, probably more of a sneer.
That's how I imagine the scene unfold.
13:08
@Slereah nice..
She had a rocky career after the Exorcist
i also saw a movie called Hausu
it's the most bizzare thing ive seen
it is about cats
@Slereah what happened
just the luck of the draw I guess?
not everyone gets to have a splendid career after making one big movie
Linda Denise Blair (born January 22, 1959) is an American actress and activist. Her portrayal of Regan MacNeil in the horror film The Exorcist (1973) established her in popular culture and as a scream queen, earning her a Golden Globe and an Academy Award nomination. She reprised the role in two sequels: Exorcist II: The Heretic (1977) and The Exorcist: Believer (2023). Blair has starred in several television films, including Born Innocent (1974), Sarah T. – Portrait of a Teenage Alcoholic (1975), and Stranger in Our House (1978). Her role in the musical film Roller Boogie (1979) brought her a...
Depressing career
13:11
i read that people died making the Exorcist. so maybe she was affected too
@Slereah sad..
it seems she did a lot of horror movies
Repossessed
@Relativisticcucumber like the one at the end
im now veering quickly towards team "category theory isn't helping" lol
What about "it helps but it's not essential"?
im discussing the definition of a morphism and being offered a choice between standard pedagogy which apparently is "lies to children" and "the correct rigorous answer"
Category theory is good but it's more of an end of learning bit than a beginning
13:34
@Slereah insert pun about arrows and arrow of time
the concept of arrows are vexing indeed
@qwerty "Morphism" is just a fancy name for function
@ACuriousMind "lies to children", apparently.
@ACuriousMind the categorists will not approve of this
I mean...from the viewpoint of category theory, yes, kind of, but if you're not explicitly doing things in the categorial viewpoint it's just true
>"a morphism is a function that preserves some kind of structure" ---- this is the heuristic, non-mathematically rigorous definition that was used historically and that we tell students

>"a morphism is an arrow in a category" --- this is the modern fully rigorous definition. It turns out that to make the concept general enough, we are forced to consider things more general than functions
13:42
@qwerty I know of no "morphism" in the context of introductory differential geometry that's not just a function
i doubt these two ideas are related. As in, the morphisms in Cat theory do not need to preserve any structure. They're just functions
but in non cat theory contexts, whenever we use morphism, we have to preserve some structure i guess
e.g. homomorphism, isomorphism
sure, if you're doing the abstract kind of differential geometry like the nLab does where you want to have generalized smooth spaces instead of just manifolds, then this becomes relevant because many of the non-manifold smooth spaces are not "sets with extra structure" so the morphisms involving them are not maps on sets obeying some extra properties
but manifolds are sets with extra structure and the morphisms between them are functions between those sets obeying certain properties
If your goal is "I want to learn differential geometry", then I absolutely think it's not useful to bother with category theory at the start
question is, can you do GR on a non-concrete smooth space
Although I'd suspect that any finite dimensional smooth space is concrete
i think homomorphism is the general term for structure preserving functions. other structure preservations r special cases of homomorphisms
but diff geo instead uses the term homeomorphism for some reason
maybe cuz homeomorphism is a special kind of structure preserving map. So they invent a new name
homeo is not homo :p
13:48
in general, one can also have homotopy maps
@Slereah what is the difference??
@RyderRude Homeomorphism is not a differential geometry term, it's the name for a isomorphism of topological spaces.
@ACuriousMind yes. That's what i meant
it's not what you said
not at all
Why don't they call this a homomorphism
@ACuriousMind sorry. I thought topology was part of dif geo, sort of
@ACuriousMind culprit mathematician: "the problem is that I can't tell qwerty the traditional pedagogy because she will complain I'm lying if I give anything other than the rigorous definitions". I reserve my own opinions, I'm just going to read and make notes I guess >.<
13:50
but i see ur distinction. Maybe u use the term diff geo only when u have an atlas
@qwerty Interesting reply, but the category-free version is perfectly rigorous. There's a difference between not being rigorous and not using category theory :P
Differential geometry is when you have a differential structure
As the name implies
yes. I wasn't precise enough. But my question is : can we say that homeomorphisms is a kind of homomorphism for topological manifolds
@RyderRude You're just throwing around the words here and it's evident you don't understand their respective definitions. Homomorphisms are not isomorphisms, in general.
Homeomorphisms are the isomorphisms in the category of topological spaces
It's the continuous maps that are the (homo)morphisms in that category
the two definitions feel totally contradictory, but apparently this is ok >.<
13:53
@ACuriousMind but that's what I said i suspected. Homomorphism seems to be the general term for structure preserving maps. And homeomorphism a special case of structure preserving maps. In general, one can also have homotopy of topological manifolds
If you want a homomorphism that isn't a homeomorphism in topological spaces, just pick a projection
Like the map from a space to a point
@qwerty which two definitions?
is homotopy the most general kind of homomorphism for topological manifolds? @Slereah
no that is another word yet :p
Apr 19, 2020 at 6:41, by Slereah
Between homology, homothetie, holonomy, homotopy and homomorphy
It's a tricky thing
13:55
@ACuriousMind whether a morphism is a special kind of structure-preserving function; or an abstracted generalisation of a function
@Slereah i thought homotopy is a structure preserving map..
@qwerty It can be both, depending on the category!
this seems like overloading terminology lol
In the category of sets, the morphisms are just functions between sets. In any category of "sets with structure" (like manifolds), the morphisms are special kinds of functions preserving the structure. In a category that's made out of things that are not "sets with structure", the morphisms are more generalized objects
but homotopy only seems to preserve homotopy groups. I'm not sure if it preserves topology in any sense
while homeomorphism preserves topology
13:56
Math uses a lot of similar sounding words
u must learn them
@RyderRude It's not. Please stop throwing around random terms.
i have learned these... I'm just trying to organise them
@ACuriousMind it preserves homotopy groups
the typical example of morphisms that aren't functions in category theory are when the category is a partial order
@RyderRude No, what you mean is a homotopy equivalence, not a homotopy.
Then the morphisms are just an order relation
13:57
@ACuriousMind yes
i understand the distinction
homotopy is defined between curves on the same space
while homotopy equivalence is between different spaces
Like you can treat $\mathbb{Z}$ as a category, in which case the presence of a morphism between two elements means that they are ordered
i meant the latter
@Slereah one can always insist not to learn them.
@Slereah yes
@naturallyInconsistent yes, but then you'd be @RyderRude
13:59
@ACuriousMind thanks, I'm copying this to my notes xD
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