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02:43
@Relativisticcucumber it should be 0
yes i realize my error was elsewhere
03:33
@SillyGoose thank u
 
3 hours later…
06:43
@Relativisticcucumber in finite dimensions this is true indeed
in infinite-dimensional cases too, if everything is well-defined
07:26
@Relativisticcucumber this is the simplest argument for why representations of the canonical commutation relations have to be infinite-dimensional! See e. g. my answers physics.stackexchange.com/a/149792/50583 and physics.stackexchange.com/a/783327/50583
08:06
Discovering trace-class operators
08:25
hi
Think I found a neat version of the reduction of GR to SR in a smoll neighbourhood
The diffeomorphism group of an infinitesimally thickened point (that stabilizes the central point) is the jet group
To first order? That's the general linear group
you can just look for the subgroup that leaves the metric invariant
Fuck :V
Looks like I'm late to the party
08:41
i feel the bot here knows physics well chat.stackexchange.com/rooms/155368/thinking-out-loud
i asked it some technical questions
about AdS/CFT
@Relativisticcucumber Miao miao looked up the many definitions of the word "functionalist" and have no idea which it is that would apply in this situation.
@Relativisticcucumber a wave packet is usually not an eigenstate of the Hamiltonian. The eigenstates of the Hamiltonian are maximally delocalised (crystal-)momentum eigenstates
I mean, Mr. F gave a very good summary
@Relativisticcucumber delocalised Bloch waves are physical solutions, just like plane waves are! But if you want "hovering around a particular atom", you want Wannier functions.
@SillyGoose If you read the Landau levels wikipedia page, it references and links to the de Haas-van Alphen effect, the wikipedia page of which states how it can be used to image the Fermi surface. This is illustrated beautifully in Ashcroft & Mermin.
@TobiasFünke never actually understood Landau levels because the derivation required strong fields but we don't seem to actually work with that strong. Also, the whole degeneracies part are just left as exercise to the reader. But Ashcroft & Mermin at least plotted de Haas-van Alphen effect beautifully. Not sure how much is understood, but pretty pictures~~
09:09
@naturallyInconsistent Well, the only thing I remember is what we've covered in a lecture some years ago :d... yesterday I checked my german version of Ziman, and some other famous german solid state book. The latter pointed to the work of Onsager regarding the Haas-van Alphen effect, where it seems he worked within the semi-classical framework
@Mr.Feynman I'd have chosen to say instead that it is not that the support is so important. It is rather that the ISW has beautifully simple results: equally spaced spectrum (and thus infinite) that is thus also extremely easy to work with, because the results are analytic. The reason why we do FSW right after that, is precisely to justify the use of ISW: we show that the non-analytical ugliness of FSW actually mostly give the same answers (for deep levels) near that of ISW, and only near the
highest, i.e. last few possible energy states, that the energy shifting is important. You can also estimate how many actual energy states there should be (as opposed to the ISW's infinitely many), and so that approximating the FSW with ISW is often justifiable.
@naturallyInconsistent the context was that of an old question of mine
@TobiasFünke didn't almost everybody do basic solid state stuff using semi-classical? The initial theories are all hodge-podge ones.
@Mr.Feynman without a link or something, that is too much work to unearth
No no, no need to. Basically Tobias commented and I was lazy to reply to a comment, so I replied here
omg main site shenanigans? naughty you
09:18
9
Q: "No local gauge invariant observables in gravity"... Is it a classical or quantum statement?

P. C. SpanielI have seen different explanations to understand why there are no local gauge invariant observables in gravity. Some of them explain that diffeomorphisms are a gauge symmetry of the theory and thus any observable evaluated at a spacetime point will be gauge dependent and therefore not an observab...

i think one needs to re-define observables in quantum gravity
@naturallyInconsistent yeah
but, as the answer shows, this is also true in classical GR. Nothing specific to quantum gravity
if we visualise diffeomorphism invariance as a symmetry about co ordinate transformations, then it is a gauge symmetry and the observables must be diffeomorphism invariant
observables in any QFT are attached to the manifold itself. it has nothing to do with co ordinates. so i don't think any problem arises in GR
but in the quantum GR case, problems may arise as the causality condition cannot be written down
as the metric is dynamical
10:00
general question: is the website with the friendly crow delivering papers down only for me?
@TobiasFünke the south east one is working
3
A: Did John Wheeler retract himself on the participatory universe claims?

ConifoldNot exactly. In late years, Wheeler did not go back on observer participancy, but was agonizing over reconciling it with shared reality for different observers. That led him to some doubts about the role of consciousness, but not over the informational underpinnings of the universe folded into "i...

Wheeler had this idea that the observer shapes the universe by the choice of what to measure. this is a participatory universe, in which observers play an active role
but this idea is extremely difficult to reconcile with science. Wheeler struggled a lot with it :The last entry Wheeler ever wrote was in 2006, age 95, nearing death, his life now bookended by questions­. It consisted of a single sentence, left behind for the community: “Hope produces space and time?”"
 
4 hours later…
14:20
A lot of the nlab weirdness is really just due to them not specifying when they use the Yoneda lemma
They just think it is so natural
15:08
@naturallyInconsistent well in the subects of phil of mind functionalists believe mental states are characterized by what they do, not what they are made of/what physically constitutes them. so i extrapolated this notion to imply that the value i find in smth is based on what it does, not about the actual experience of engaging w that thing. perhaps a bit of a stretch idk
15:27
> SAY MORE ABOUT HOW!!!
DEFINE “LAZY SURFACE”!!!
I like how so many physics papers have these
Just writing [REMEMBER TO DO THIS SECTION YOU LAZY PIECE OF SHIT]
16:26
@Relativisticcucumber still confused but ok?
 
1 hour later…
17:42
@naturallyInconsistent they're saying the function of the book in teaching the subject well by being self-contained is more important to them than it's experiential quality of being nice to read
17:57
@ACuriousMind yes
also look acm its ur favorite:
SvNT
I do love me some SvN
18:49
hello everybody
19:25
hello
morning
Afternoon
Why do people refer to relativity as "Einstein's relativity"?
@DanielSank Well, isn't there also "Galilean relativity"
Not that I've heard of.
19:31
Galilean invariance or Galilean relativity states that the laws of motion are the same in all inertial frames of reference. Galileo Galilei first described this principle in 1632 in his Dialogue Concerning the Two Chief World Systems using the example of a ship travelling at constant velocity, without rocking, on a smooth sea; any observer below the deck would not be able to tell whether the ship was moving or stationary. == Formulation == Specifically, the term Galilean invariance today usually refers to this principle as applied to Newtonian mechanics, that is, Newton's laws of motion hold in...
alternatively they might be taking a side in the relativity priority dispute :P
If I say "I'm studying relativity", don't you interpret that as the theory devised by Einstein?
@ACuriousMind The ":P" means this is not to be taken seriously, right?
I don't seriously think that's the case in most cases
@DanielSank I do, but that doesn't preclude that it makes sense to talk about "Galilean relativity", too
19:34
but they might be mirroring the phrasing of someone who was using that phrase to make clear they credit Einstein
but more realistically I think the most common reason will just be a not particularly mindful reference to authority - everyone knows Einstein was a genius, so calling it "Einstein's relativity" increases the perceived importance of the subject
just found this article, but I've only read the abstract:
mmm, in protest I will start saying "Heisenberg's quantum mechanics" just to annoy people.
we love making history about individual people, it's a subconscious reflection of the Great Man theory of history in action
@DanielSank around 6000 google hits for that exact phrase, you're not the first
sure not. it is a common phrase lol
...to distinguish it with Schrödinger's quantum mechanics, in a historic context
well, "Heisenberg's matrix mechanics" would be the more common way to say that, I think
19:42
okay, I agree. And similarly Schrödinger's wave mechanics or so
@ACuriousMind definitely this. and it also seems a little dated in fashion.
the analogue to "Einstein's relativity" could be something like "von Neumann's quantum mechanics" (?)
@TobiasFünke probably not - the level of functional analysis at which von Neumann engaged with quantum mechanics is not how QM is done in practice :P
@ACuriousMind Dirac's? :d
yeah, that's more fitting
19:46
@ACuriousMind I would also say it's just name dropping to increase the perceived important of the author at times too
I was looking through Weber's book on gravitational waves and the number of [insert famous name] (personal communication) references was a little alarming
If one wants to emphasize the difference to e.g. "Galilean's relativity" or if one wants to emphasizes Einstein's role in the development, then I don't think it is unusual or "inappropriate" to say "Einstein's relativity"...
@TobiasFünke that's why I said "at times" :p
@DanielSank ey it's been a while
how's life
@ACuriousMind Yes. It's a thing I do not much like :-)
Hero worship never ends well.
@Relativisticcucumber whenever he mentions SvN I feel so weak in QM :P
@ACuriousMind I mean, saying "Hilbert's relativity" would be like saying that a kind stranger who helped me on the streets is my dad :P
19:58
how do you know the kind stranger isn't your dad?
(I'm not really following the metaphor :P)
ooo shots fired
@ACuriousMind Incidentally, I find that if on the one hand many people do that, on the other hand you have many people apparently loathing this tendency to a fault, which I never understood
also why did SvN get starred, is there some kind of joke?
@qwerty not that I'm aware of
I mean, I think it is ok to glorify some individuals in science, as long as you understand that their words is not absolute
I don't like when people have to tell you every time that Einstein or Feynman or whoever else was "a person like us". I don't like thinking that all scientists are equal
20:02
@Mr.Feynman well we've discussed a bit before: is is reflective of reality firstly, and secondly is it beneficial to the culture in science ( i mean students and academics as well as popular culture) to think that way
@ACuriousMind I was trying to say that Hilbert did something important, but the fundamental idea of GR (as we know it today) is Einstein's (or at least not Hilbert's :P)
omg roasted
@Mr.Feynman Well, see, in even saying this you're implicitly saying that it's somehow important to get right whose idea it was. I'm not saying this is wrong in all possible meanings, but the question is: Why do you think it's important?
@Mr.Feynman All scientists are equal, but some are more equal than others.
I think it is important, yes. Not for science, but for history of science.
20:05
And why is the apparently most unpopular answer to reject the notion that these kinds of inventions have to belong to a single person or a very small group of people?
@TobiasFünke Yes, basically what I think about our farm :P
@TobiasFünke oink
@Mr.Feynman Then you should oppose calling the Einstein-Hilbert action that, since that was mostly Hilbert's doing!
if it's Einstein's relativity, then it's Hilbert's action
now, I think that's a silly argument, but I think that people would add Einstein to the action but not Hilbert to the relativity hints strongly towards a less-than-purely-historical thing going on
@ACuriousMind 100% agree
@ACuriousMind mhhh, no. I probably phrased it incorrectly. Of course that holds true in many cases. Most of the theories as we know them today come from the effort of multiple people. I was talking about the fact that many people seem to dislike when one single scientist is glorified (not talking about anyone here specifically, irl experience) and need to remind you that he was human or that he is not a god. Of course I know that :P
@ACuriousMind it is "historical" - history is a narrative written by victors :p
20:09
I'm not buying that someone calling himself "Mr. Feynman" isn't talking about someone specific :P
If you wonder why I mention that now it's because these same people also tend to find any possible caveat to give credit to someone else in order to downplay someone more famous :P
@ACuriousMind not specific here
I always get into fights about this with a friend of mine, okay? :P
@Mr.Feynman i think there's a difference in downplaying contributions and not buying into fanboy/girl-ing culture, don't you?
@ACuriousMind In fact I always wondered why it's the EH action and not the H action. I think that the most accurate representation is Einstein's relativity+Hilbert's action. Anything else is wrong
honestly the history of science seems rather complicated and diving into it seems like a full-time academic pursuit
@qwerty yes, that is correct and I admit that I have a strong fanboy tendency myself
20:12
@Mr.Feynman ::shocked Pikachu face::
4
As you can guess from my parasocial behaviours :P
Damn, the chat is roasting me hard tonight
yeah indeed
Anyways, as I said I think that calling it just the "Hilbert action" and "Einstein's relativity" is the way to go. Now the question is: why do people call it EH action and refuse to say "Einstein-Hilbert's relativity"? Well, I think because the action is an important contribution but it's almost more of a tool, an alternate derivation of the EoM, which ontologically (?) wouldn't have the same importance as the whole theory.
In other words, putting Einstein's name in the action is in this sense more acceptable than putting Hilbert's name in relativity
Stigler's law of eponymy, proposed by University of Chicago statistics professor Stephen Stigler in his 1980 publication "Stigler's law of eponymy", states that no scientific discovery is named after its original discoverer. Examples include Hubble's law, which was derived by Georges Lemaître two years before Edwin Hubble; the Pythagorean theorem, which was known to Babylonian mathematicians before Pythagoras; and Halley's Comet, which was observed by astronomers since at least 240 BC (although its official designation is due to the first ever mathematical prediction of such astronomical phenomenon...
@ACuriousMind C'mon, don't tell me it's just the username :P
20:21
@qwerty I'm hesitant to use that phrase or to agree too much with its implication that history is a one-sided parade of propaganda. Think of all the atrocities of victors we do know about, and all the failings of great historical people - if they wrote that, they did a pretty bad job at hiding their faults!
(Remember, I grew up in a country where "history is written by the victors" is a phrase with a very different historical weight than in most other Western countries)
@Mr.Feynman not exclusively, but it's certainly not helping!
Oh God, I thought I was hiding it well :P
@Mr.Feynman my brother in physics, you made the starred post about tattooing Qmechanic's favourite quasisymmetry on your body
4
And you snakes keep starring that!
It was a moment of weakness
@Mr.Feynman Anything you say can and will be used against you (it seems)
20:30
@ACuriousMind yes, you're right, of course. there is indeed nuance; but broadly I feel like the general message of being sceptical of what the historical narrative is (with the nuance you mention, and not just going into... history denial? is that the term?) is still defensible as "correct".
@TobiasFünke Yeah, since qwerty joined the gang, I get more roasts :P
Which is funny because it's not the only online place where people like to roast me 💀
@qwerty Yes, skepticism is good - a blanket assumption that it's one-sided is not, I feel
@Mr.Feynman I'm sorry mr F :P it's very much not targeted!
@ACuriousMind I suppose it depends on what level you're learning or studying history as well? if you get the cliffs-notes version (which I what I feel happens in physics when you get told "Einstein came up with relativity") I think that tends to be more one-sided as it's been simplified/reduced. If you're an actual historian, you know more details, more sources and "sides" to put it that way
yes, certainly
Can anyone explain the relation between the solution to the klein gordan equation and harmonic or quantum harmonic oscillator? What does this mean for the particle?
20:46
@imbAF sorry, can you be more specific? what exactly do you mean?
@qwerty I have a thick skin :P
In my lecture we started with the klein gordan eq. and we arrive at the following point:
$(\frac{\partial}{\partial^2} + \vec p^2 + m^2)\phi(t,\vec p)=0$
And this was said to be the harmonic oscillator equation or is related to it, no idea what the notation (harmonic oscillator ) in the notes is supposed to mean. Anyway, because in QM we dealt with the algebraic and analytical solution of the QHO, the equations there, those of motion (I assume) did not look like what we wrote in the lecture
So in conclusion I don't know the tie made between KG equation and qho or harmonic oscillator
@TobiasFünke
@imbAF See chapter 1.5 in Weigand's notes [pdf link] for a properly written explanation of the analogy.
Mode expansion ?
yes, you have correctly read the title of chapter 1.5. :P
20:54
I mean I am asking because I don;t read klein gordan
And I though I was at the wrong chapter
But ok
thank you
Do you not see that eq. (1.58) is the KG-Hamiltonian, i.e. what you are asking about?
Very good notes, btw
@ACuriousMind I see it. Thanks
I think that the notes are good, but I believe that their purpose is to remind someone who was already a good understanding of QFT, in other words, has read the books Weingard recommends, about a concept. Unless I am wrong and reading this would suffice. I am talking in general now, not particularly for the KG equation question that i posed earlier
@imbAF They are most definitely not, these are the notes of the course in which I learned QFT and I did not read any of the books while I was taking the course.
@ACuriousMind Then that's awesome. I won't have to read 800 pages of schwarz during break time from uni
really thanks
21:06
I mean, that doesn't mean there aren't some things that some of the books explore in more depth or topics left out, but for an intro to hep-th QFT it is reasonably complete
@imbAF you can trust ACM, as he took the course on which the notes are based :P
Iirc
@Mr.Feynman I literally just said that :P
You know I don't read the chat (I was about to type "ah, he said that")
Yeah of course. I also believe that what I am doing is into of QFT
and will be doing it until the end of semester
So the book will do
@ACuriousMind actually there is more in those notes about Wilsonian renormalization than in many intro QFT books
21:54
@SirCumference It's pretty good. We are making a lot of progress in quantum computing.
I am slowly making progress on a "book" about engineered quantum systems.
 
2 hours later…
23:33
I have a question regarding atomic orbitals of two atoms
If one atom is at a certain position in the coordinate frame e.g origin, and the 2nd one is at distance R at some angle $\phi$ from the x axis. Would a rotation of the frame so that the new x' "contains" both atoms, change or simplify the calculations for a matrix element of the Hamiltonian?
In condensed matter theory
It was said that a change of the coordinate system does affect the calculations of a matrix element
How would that be the case?

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