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00:00 - 22:0022:00 - 00:00

00:34
Domain walls are a pretty good example of symmetry breaking
00:59
I concur. Was just reading up on them
01:32
@ACuriousMind Great answer on the instanton question! :D
01:47
@AngusTheMan thanks, although I only answered the "easy" part. ;) Currently working through Witten's "Topological Quantum Field Theories" to answer the part about Donaldson invariants.
 
1 hour later…
02:54
@ACuriousMind hey! What exactly is a partition function? I think I've learned enough in the last 3 days to perhaps understand it. I understand why $n_i = g_i e^{-\alpha + \beta \epsilon_i}$ maximizes $\Omega$ (Aka $W$) but I don't understand what $Z$ is or what it means.....I know $Z = \sum_i e^{-\beta \epsilon_i}$ but I don't get what this represents. Can ya help me understand this a little better?
 
2 hours later…
04:27
@StanShunpike In the simplest sense it's just a weighted count of qualifying states.
Where the choice of weighting makes it a normalizing factor for the odds of a state being occupied.
04:58
@dmckee can you teach me a bit about large N approximation, and planar diagrams. How does it work for say,. . your favorite matrix theory
well for a very simple theory
05:30
@kevinTahN. Uhm ... probably not. I mean, large N approximations ar what they are, but I can't even place the context for "matrix theory" here.
 
2 hours later…
07:05
@Bass Morgen.
@0celo7 Morgen :)
1
Q: arithmetic question

anna vIn this question there are eleven downvotes. I know from downvotes I have gotten that each downvote subtracts 2 points. 2x11=22 should be deleted. The user has a remainder of 8. How is this possible? Even if he/she came with the dowry of 100 from another site, still 8 is not what it should be:78...

hmm , ok I need some help. I want someone to devote a few chat texts to help me understand large n approximation.
@Bass Do you happen to know about wave-like solutions to Maxwell's equations in curved spacetime?
@0celo7 nope, but I doubt you're gonna find exact solutions that fit to every curved spacetime
07:11
@Bass I just want to see if the "center" of the wave packets follow null geodesics.
I don't need exact solutions...just some properties of exact solutions.
Day 1: It survived, for now
0
Q: Electronic spectroscopy question in a more physics oriented view. What is the operator that describes relaxation pathways?

SecretRecently I was studying spectroscopy in Symmetry and Spectroscopy: An Introduction to Vibrational and Electronic Spectroscopy p.357-358 as shown in the image https://i.sstatic.net/LSLyZ.jpg The author said the internal conversion (laballed IC in that energy level diagram) is isoenergetic, whi...

In SR one can show, rigorously, that a plane wave solution of Maxwell's equations travels along a null geodesic.
However there is no answer yet, still in a tumbleweed state
@Secret protip: use \text{} when you have words in your TeX
done
07:14
@Bass However, in GR, one must ignore a term in the Maxwell equations to get the same result.
@Secret protip 2: use \lvert and \rvert in bra-kets: these extend all the way down and have the same overall height as \langle and \rangle
---
done
@Bass Basically, try plugging in $A^\mu=C^\mu\mathrm{e}^{\mathrm{i}S}$ into Maxwell's equations
$C^\mu$ is a constant
in SR you get $\partial^\mu\partial_\mu S=0,(\partial S)^2=0,C_\mu\partial^\mu S=0$
If you take the derivative of $(\partial S)^2=0$, you get the geodesic equation
ok, I will learn anything anyone tells me to on here :D
Ok, I have to re-learn wtf a null hypersurface is
wald seems to think $\epsilon^{abcd}k_c\nabla_d(k_ek^e)=0,k=\mathrm{d} S$ is important
07:32
@0celo7 sorry, can't help you there..
08:14
0
Q: Can we get the hat frequencies?

John RennieI get the impression that the Darth Vader hat is the most popular. I can't imagine why, anyone would think that (a) physicists are all sci-fi geeks and (b) there's a new Star Wars film out. Anyhow, is there a way to find the numbers of Physics SE members currently wearing each hat?

08:37
Being downvoted by John Duffield because my (conventional) answer does not agree with his idiosyncratic views on relativity is getting to be something of an occupational hazard. I suppose it's just another of the hazards of life, like hemorrhoids or genital herpes.
@JohnRennie ...
Have your star
08:55
@0celo7 :-) Though I'd sooner have a Physics SE free of zealotry.
@JohnRennie currently formulating a question about solutions of Maxwell's equations outside of the geometric optics approximation
you might find it interesting
(in GR)
I'll have a look, though I was always profoundly uninterested in electrodynamics at school/university. It seemed to be just an excuse for examiners to think up unlikely scenarios for exam questions involving lots of vector calculus.
@JohnRennie this is certainly more interesting
basically, I'm wondering what happens to wave packets at distance scales where the curvature can go crazy
do they follow null geodesics?
Be sure to put in something that contradicts a statement by Einstein. You wouldn't want to deprive John Duffield of his fun.
@JohnRennie can you teach me large N approximation?
09:05
@dmckee is that all there is to it? why is it so important?
@JohnRennie hello, long time no speak!
been hanging out here for a while trying to trick people into teaching me large N approximation technique :~)
People here are rather hard to trick
Besides me
@kevinTahN. what is the large N approximation technique?
@StanShunpike Hi Stan. You'll only find me in the chat when I'm pinged or when I want to bitch about something :-)
Naturally, hence I take the time to say hi when u are here ;)
Omg u can wear the hats on ur profile pics?!?
That's what those are for! eureka
I don't know much about it but I think it is some technique used in qcd or something, but you can also use a version of it on simpler theories. You can also may be draw planar diagrams and stuff. Honestly I don't quite know, but . . . . also I think it might actually be called large N expansion . . .
some links to accompany this include books.google.com/…
and one more link comming up
@JohnRennie In Juan Maldacena's Tasi ads/cft lectures he begins with a disquisition of large n and planar diagrams , then precipitates a technique of how to guess some "equivalent string theory" and how to create a dictionary
09:17
Ah ok, you mean letting N go to infinity in an SU(N) representation. I'm afraid that's far outside my skill set.
@JohnRennie the tasi lectures I mentioned arxiv.org/pdf/hep-th/0309246v5.pdf
I see. . .
Unless you already have a good knowledge of quantum field theory it's going to be far outside your skill set as well.
@StanShunpike Keep up at the back there Shunpike! :-)
I have been told it can be treated outside of su(n) for some simple matrix models
Hahahahaha
In its full glory it is definitely outside my skill set lol
@StanShunpike can you discuss it in the scope of tractable simplified matrix models?
I would really love some input on this
@JohnRennie Is there a way we could formulate this within the bounds I mentioned and pose it here or may be to the Q&A section?
09:22
I am not knowledgeable about anything physics related that would be useful to u. Lol my skill set is amateur level. As in I own QCD books but can't understand them.
@kevinTahN. No idea. To be honest, unless you understand QFT well enough to figure it out for yourself I doubt you'd find any answer here very useful, or indeed comprehensible.
I don't have a grasp on qcd either but was assuming the technique could be explored outside of qcd on simple models
@JohnRennie yeah, I read a bit of it in the context of qcd but there were other subtleties that prevented me from getting the general concept (may be algorithm) for doing it. Was hoping Santa would point me to a simple model I could study this for Christmas
this physics.stackexchange.com/questions/123416/… is somewhat close, but might need an even easier toy model and more explanation lol
 
1 hour later…
10:54
0
Q: Do light waves precisely follow null geodesic paths in General Relativity?

0celo7In special relativity one may show that a plane wave solution of Maxwell's equations (in a vacuum), of the form $A^a=C^a\mathrm{e}^{\mathrm{i}\psi(x)}$ has the following properties: The normal $k:=\mathrm{d}\psi$ to the surfaces of constant $\psi$ is a null vector and the integral curves of $k$ a...

anyone is welcome to take a crack at it
11:11
Hmmm, looks like @JohnDuffield 's answer on that natural units question is gone
@DanielSank I've heard VA Tech's technical writing class tells people that real scientists use $*$ for multiplication. cf. physics.stackexchange.com/questions/215408/…
(They will take off points if you use $\cdot$ or try to imply multiplication.)
@Huy how was the movie
pls spoil
Huy
Huy
@0celo7 much better than I could have ever imagined
would an SJW like it
Huy
Huy
@0celo7: hard to say without spoiling too much
@Huy pls answer my question above
ask one of your high school students who like physics
Huy
Huy
sorry that's trivial
won't bother my students with that
they have serious problems to work on
11:26
D:
dude how the fuck do they get so smart
Huy
Huy
it's a joke
they don't know GR
bullshit
Huy
Huy
one of the two girls cried today
the other one didn't
I was glad only one did
stop trying to unhurt my feelings
just give them my question and make it extra credit or something pls
@Huy why
they're doing PhD level math and are crying...wtf
Huy
Huy
cuz she got rekt at my exam
she said she prepared like a lot
and asked how this could be
and I said "idk"
11:30
because it's PhD level math and she's not autistic...
@Huy why don't they know GR
Are they the kind of people who think physics is too trivial?
@Huy do you know the proof of $$K(p)=\lim_{r\to 0}\frac{3}{\pi}\frac{2\pi-L}{r^3}$$
the thing with the Gaussian curvature and the circle
Huy
Huy
11:49
@0celo7 sorry i have no idea what u mean
Huy
Huy
sorry I need to write some exam questions
I think I have a good one
but I need to see how to properly translate and rotate it in R^3 now so that the numbers are a bit more difficult
post here
Huy
Huy
(but not too difficult)
trivial stuff
you know what the 3D rotation matrices are, right
Huy
Huy
yea
12:36
ok
then pick some nice angles and multiply away
Huy
Huy
I had to prove $S^3/ \{\pm 1\} \cong SO(3)$ on my diffgeo exam
I hate calculations
@Huy what's the difference between a space-filling curve and a curve dense in some set
@Huy you should have used Clifford algebra
Huy
Huy
not my thing
then you just show that $\mathrm{Spin}(3)=\mathrm{SU}(2)$
Huy
Huy
that I know
I think space filling curve is usually specifically about $[0,1]^n$
12:40
No, space filling curves fill space.
Huy
Huy
oh yeah
They're surjective.
Huy
Huy
yea
huh
does a dense curve not fill the thing
Huy
Huy
no
dense means the closure is the thing
12:40
yeah
Huy
Huy
$Q$ is dense in $R$
sigh
$Q$ is not a curve
Why would there be a different word for dense if it was the same thing?
@Danu that's what I'm asking
I don't see the difference
12:42
Google
Analysing some 4 years ago stuff from a user named Mrrl:

It is known whatever "?" is, there's a continuous map that can transform from "?" to the cross section immediately before and after "?"
@Danu does not help
It's just a bit annoying to you that you're constantly filling chat with your questions. But I guess that's my problem, not yours.
@Danu what?
Just exactly what I said.
12:45
@Qmechanic Hi, with regard to your answer here, what is a 2-cocycle obstruction? Can we have symlectomorphisms give rise to this problem, if so what are their implications for the physics? Thanks :) physics.stackexchange.com/questions/138099/…
beats me how my questions annoy you, sorry sir
I'll go fuck off then
bye
jeez, such drama
@Danu do you know spectroscopy to help me out on a conceptual question?
I don't know any spectroscopy.
ok nvm
12:50
@Secret what kind of spec?
virbonic spectroscopy
vibronic*
go on..
1
Q: Electronic spectroscopy question in a more physics oriented view. What is the operator that describes relaxation pathways?

SecretRecently I was studying spectroscopy in Symmetry and Spectroscopy: An Introduction to Vibrational and Electronic Spectroscopy p.357-358 as shown in the image https://i.sstatic.net/LSLyZ.jpg The author said the internal conversion (laballed IC in that energy level diagram) is isoenergetic, whi...

interesting :) I'll have a look over some books and see if they help!
Huy
Huy
@0celo7 halp with my problem in math chat
12:58
ok thanks
@0celo7 : yep. And your name isn't in the list.
Where can I find the book you authored @JohnDuffield
13:15
@skullpetrol It was not super interesting.
Too elementary; it was very pedagogical and qualitative.
13:48
@0celo7 Out of curiosity, which question?
This is going nowhere, I have sent him a message to ask for clarification
But logically, the boundary of al the slides should be homeomorphic to a circle
14:07
@skullpetrol : you can find some second hand copies on Amazon.co.uk. Ouch, £44 thru £88? That's ridiculous, and nothing to do with me. Aw, I imagine I've got a spare copy lying around. Email me at mynamealloneword at btconnect dot com and I'll send you one. There's a few things I'd change if I were writing it now, like calling a gravitational field a tension gradient instead of a pressure gradient. But there's nothing that has me wincing.
3
14:25
@JohnRennie : you were downvoted because your "conventional" answer did not agree with Einstein. I don't have idiosyncratic views, I referred to Einstein's E=mc² paper and energy in the form of radiation. And to other material re gluons and virtual particles. In fact your answer has so many issues. I'm rather surprised it got six upvotes. I'm also surprised the question was closed as "unclear what you're asking".
5 hours ago, by John Rennie
Be sure to put in something that contradicts a statement by Einstein. You wouldn't want to deprive John Duffield of his fun.
So predictable.
@StanShunpike: (outside QFT) the partition function is little more than the normalisation of your probability density - when divided by it, $\exp(-\beta H) $ becomes a proper density (classical) or a proper density matrix (quantumly)
@JohnRennie : if you contradict Einstein, a) you should be aware of it and b) you should be able to explain why. Trying to wriggle out of it by carping about me cuts no ice.
OK work calls, talk later.
 
3 hours later…
17:21
quick question: is there any constant tensor $a^{\mu\nu}_{\alpha\beta}$ constructed from $\eta^{\mu\nu}$ and $\varpesilon_{\alpha\beta\mu\nu}$, such that it is symmetric in its lower indices and skew-symmetric in its upper indices? I believe there is not, but I couldnt prove it. does any simple argument occur to someone here?
17:33
My favorite beef recently: people who tell new users that homework is OK if they show effort. The very first sentence in the meta answer we point to in the close reason contradicts that:
> It's not enough to just show your work and ask where you went wrong. If you just need someone to check your work, you can always seek out a friend, classmate, or teacher.
@dmckee Any recent examples?
Or maybe not, no reason to shame anyone
Yeah. I don't want to call out the user who triggered my rant.
That's good policy in general and I think this user in particular is a good one.
But yeah, I agree that effort and on-topicness are pretty orthogonal dimensions.
Re: this one
1
Q: Are orbitals physical quantities?

Emilio PisantyOrbitals, both in their atomic and molecular incarnations, are immensely useful tools for analysing and understanding the electronic structure of atoms and molecules, and they provide the basis for a large part of chemistry and in particular of chemical bonds. Every so often, however, one hears ...

Open to suggestions on how best to phrase the question
@EmilioPisanty Not off the top of my head. Since I started teaching I have gained a renewed respect for the importance of the words we use, but at the same time they are often a matter of convention.
The result is that these matter feel simultaneously arbitrary and important to me.
Which feels like a recipe for pointless dissension.
@dmckee Heh.
Yeah, I'll rephrase it a bit to emphasize the technicalness and manybodiness of the argument.
17:59
@JohnDuffield Huh?
@dmckee Just rephrased it.
@EmilioPisanty Here you go
@Huy ok
Had a glass of mead today. That stuff is way too sweet. Dunno how the Nords in Skyrim do it.
18:22
@JohnRennie My question is up, check the GR thingie. Would appreciate at least some thoughts in the comment section.
@0celo7 Suppose you zoom in to a small part of the wavefront, then even if the wavefront is curved it's going to look like a plane wave. In that case wouldn't the Poynting vector always point in the null direction?
How is the Poynting vector defined again?
I thought it was $E\times B$ or something...
B cross erm, Jesus I've forgotten.
I've never seen the Poynting vector appear in SR/GR.
E cross H - I wasn't even close :-)
18:25
@0celo7 : the list of people who voted to delete my answer.
@JohnRennie In any case, I'm more interested in the global properties of the wave.
@JohnDuffield I did not vote to delete it.
I know. That's why I said you weren't in the list.
Globally the wave is going to be focussed by the curvature. I'm not sure you can usefully talk about a direction globally.
Yeah, your point?
Forget it.
18:27
@JohnRennie Isn't $H$ just $B$ up to some factor or something.
@JohnDuffield ok.
Have I mentioned I always hated electrodynamics? :-)
yeah
But why does the Poynting vector point in the null direction
Here's the Poynting vector for an electromagnetic wave:
@0celo7 Just a convenient way to define the direction
@JohnDuffield indeed...
18:29
And here's the Poynting vector for a static field.
Is the direction of the Pointing vector the same as for $\vec A$?
Wait, @JohnDuffield , how is the Poynting vector defined in relativity?
Poynting vector
Because the Poynting vector as shown in @JohnDuffield 's pic is not pointing in the null direction.
@JohnDuffield Force of habit.
Yes, but you asked about plane waves
No
I said wave-like solutions
18:31
I don't think the Poynting vector is defined any different in relativity.
@JohnDuffield how is the cross product defined in SR/GR
To be honest I have no chance of providing a useful answer to your question.
@JohnRennie but you're the GR dude
Cross product of what?
@JohnDuffield the definition of the Poynting vector requires a cross product
18:33
where is @MarkMitchison and @DanielSank?
@0celo7 Your not looking for a cross-product exactly. You're looking for a contraction of the electromagnetic field tensor that reduces to the appropriate cross-product in the flat-space case. Right?
Hmmm ... and presumable the time-like component of that result will be, what, the energy density?
@dmckee Can you find me one?
In geometry, curvilinear coordinates are a coordinate system for Euclidean space in which the coordinate lines may be curved. These coordinates may be derived from a set of Cartesian coordinates by using a transformation that is locally invertible (a one-to-one map) at each point. This means that one can convert a point given in a Cartesian coordinate system to its curvilinear coordinates and back. The name curvilinear coordinates, coined by the French mathematician Lamé, derives from the fact that the coordinate surfaces of the curvilinear systems are curved. Well-known examples of curvilinear...
@dmckee Ah!
So something like $T^{00}$?
but that's not a vector
@0celo7 Guess so. I'm a bit out of my depth on this stuff.
18:35
@0celo7 : see Space and Time where Minkowski said this: "In the description of the field caused by the electron itself, then it will appear that the division of the field into electric and magnetic forces is a relative one with respect to the time-axis assumed; the two forces considered together can most vividly be described by a certain analogy to the force-screw in mechanics; the analogy is, however, imperfect". The field of the electron is the electromagnetic field.
E and B denote the forces that result from electromagnetic field interactions.
And I have to go. Back later.
@ACuriousMind so what about within QFT? rhat was why i took the time to learn about it
@JohnRennie wassat
@dmckee would e.g. Jackson have this
ah!
$F_{0\mu}F_i{}^\mu=S_i$, @dmckee @JohnRennie
that's $T_{0i}$
18:51
@0celo7 Looks promising.
@dmckee now what
that's some crazy 3-vector, which are not useful in GR
@0celo7 Well, there is a time-like part that comes out of your contraction, so the whole thing is still a four vector right?
@dmckee No...$F_{0\mu}F_i{}^\mu=\epsilon_{ijk}E^jB^k$
if you get the summation notation
Now you try to make that four vector play the same part as the plain Poynting vector plays in E&M the Mawell, not Einstein way. The spacial part is going to point in the direction of energy flow.
well I wonder what $F_{0\mu}F_0{}^\mu$ is
@dmckee yes...
time to read the Wiki article on the Faraday tensor
18:56
Ah, yes. latin versus greek indicies. I don't do that stuff very often.
@dmckee Note that in my question I use abstract Latin indices ;)
which are equivalent to Greek ones :)
@dmckee self-educated guess: $F_{0\mu}F_0{}^\mu=|\vec E|^2$
Do Newton's laws imply "conservation of energy"? Or is that principle a separate thing from those?
@dmckee what's the significance of that in EM
@StanShunpike They do!
You want the proof?
Yes! I'd love it
Note: this is also useful for solving any ODE of the form $y''(x)=f(y)$
$F=ma=\ddot x$ (set $m=1$ for sanity)
Let $U=-\int F\,\mathrm{d}x$, i.e. $U'=-F$
Let $E:=\dot x^2/2+U$
then $\dot E=\dot x\ddot x+U'\dot x=\dot x(\ddot x+U')=\dot x(\ddot x-F)=0$
19:03
wow
chain rule used to take the time derivative of $U$
yeah keep going
...
that's it
$\dot E=0$
@StanShunpike now the trouble is when you have $F\ne F(x)$ but instead $F=F(x,\dot x)$
i.e. nonconservative forces
remind me what that is
friction
@dmckee could explain better
basically a force that is not the derivative of something
19:07
Wow, that's a really simple result to prove. Interesting!
Cool!
it's more difficult in 3 dimensions
Newton's law imply the simple conservation of mechanical energy directly.
you need some vector calc...but that's about it
You have to be a little clever to include thermal energy (mechanical equivalent of heat and/or kinetic theory as a starting place).
so not "difficult," just more machinery
19:08
Then you have to start generallizing to field energy in E&M and the like.
Or at that point you can just appeal to Noether's theorem, which gives a much less muddled foundation for the whole thing.
@dmckee at that point why not just use Noether's theorem
heh
Gat minds. Or at least twisted ones.
well great mind tell me what significance $|\vec E|^2$ has pls
@0celo7 Yeah I wouldn't put that in the category of difficult. More tedious.
@0celo7 It's the energy density of the field to withing some constant factors of $c$ and 2 and maybe some $\pi$s depending on your units.
19:11
@dmckee energy density also has a $+|\vec B|^2$
@dmckee brb solving Maxwell's equations
@0celo7 But in free space the fields are proportional to one another. So you can express it in terms of just one of them.
also note that that's in your precious flat space
I'm looking at GR scales where everything we know and love ought to break
Npote that I said "free" (as in matter free) not "flat". I don't know anything about what significance it might have in strongly curved space.
yes, $|\vec E|=|\vec B|$ in flat space and in a vacuum
@dmckee because Maxwell's equations are completely different in curved space!
if you read my question you would know that :(
I'd like @DanielSank to have a look at the comments of John Rennie's answer of physics.stackexchange.com/questions/224845/… , I think Daniel could make valuable comments.
19:43
@BalarkaSen what are you doing here
Looking for Danu
@BalarkaSen hmm, you don't want to do some physics
too busy hat-hunting
uhhhhh
hats are going to disappear in january i think
i haven't figured out how to use more than 1 hat at once
19:59
@no_choice99 why do you think there's a way
because I think I had seen John Rennies with several at once, but I may be wrong
@no_choice99 he's magic tho
20:32
@0celo7 Suppose I am considering a box resting on the surface of the earth. In the context of GR, is it appropriate to say that the box is in the earth's gravitational "field"? I forget if the fact that gravity "isn't a force" means that it also isn't a field.
I suppose EFE implies field
yes
note that it is always in the Earth's field
since gravity never "dies"
what do you mean?
define "gravitational field" first ;P
@StanShunpike the box always feels gravity due to the earth
Well, I always think of the Newtonian gravity because I use it most frequently.
it's not like you can actually go to $r=\infty$
20:34
@0celo7 How do we know we can't go to $r = \infty$
?
or is that just an assumption
@StanShunpike what
$r=\infty$ is not a place
it's a limit
a limit in which an asymptotically flat gravitational field will "die off"
ah okay
i get it
@StanShunpike in any case, the wording is not important
hell, I can call gravity a force all day long
doesn't change my math ;)
really?
I thought one of the points about GR was it wasn't a force
define force
vzn
vzn
21:22
@dmckee wondering more the connection between instantons & solitons... re wikipedia article on instantons:
> Note that there is sometimes also a corresponding soliton in a theory with one additional space dimension.
21:52
the shocking moment when you see other members of the PSE on your suggested linkedin contacts! small world eh!
hey guys
I feel a little bit embarassed to join up a conversation like that and asking for some suggestions on physics textbooks oriented on problem-solving ,but that's what I've been told to do...so if you can help I will be really gratefull....
@Mr.Y What level and topic did you have in mind?
0
Q: Is there a Maupertuis principle for General Relativity?

0celo7The motion of a point particle in classical mechanics is given by Newton's equation, $\mathbf{F}=m\mathbf{a}$. Suppose all forces considered are conservative and we have a constant total energy $h$. Let $M$ be the configuration space of our system, $T^*M$ its cotangent bundle, $(\mathbf{q},\mathb...

Random thought turned into a question
@Alarge Well the standard curriculum used at high school level(I finished high school and am taking gap year )
00:00 - 22:0022:00 - 00:00

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