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08:29
@MoreAnonymous i think the mass independence idea only holds for expectation values. if we initialise two different wavefunctions with same initial $\langle X \rangle, \langle V\rangle$, then they have the same $\langle X(t) \rangle$ regardless of their mass. this is just Ehrenfest's theorem
idk how else to define a notion of "same initial velocity" without using expectation values
08:48
in classical mech too, two different masses behave the same under gravity only if u initialise them with the same x and v. if u initialise them with the same x and p, then they behave differently
09:09
i think the core of equivalence principle is whether or not the laws in zero gravity frames are the same as the laws in free fall frames. Mass dependence/independence stuff is not that important
09:38
gday
09:49
Why, hello
hello hello :)
 
3 hours later…
13:08
pseudoscience believers r always trying to convince u that their ideas r scientific
especially astrology believers. and they just think u r not open minded
13:22
@User198 I'm not sure what makes a canonical transformation "cool" :P Locally, it's effectively just a coordinate change, and if you're lucky you can find coordinates in which the equations of motion are particularly simple (cf. Action-angle coordinates), this is not different from any other formalism of mechanics.
13:35
@ACuriousMind i have never encountered these co ordinates
I'm not sure what you expect me to do with that information :P
this looks really advanced. looking forward to learning it
it uses group theory stuff physics.stackexchange.com/a/440133/156987
@User198 u can also just do algebra
it uses algebra to solve for $x(t)$ of the free particle
it is really strange that one can solve these particular classes of differential equations using just algebra
i was once looking for a generalisation of this idea. this idea seems to work when the diff equations can be expressed using commutators, which is a very specific class of differential equations
13:56
It's just Lie theory.
yes. but how to get a general diff equations solving techniques out of this
it is a really unique technique
There is one book that Qmechanic always mentions about DE and Lie groups
usually, one can solve a coupled system of ODEs when the coefficients are constant
like matrix exponentiation
but I think this idea allows u to solve more complicated differential equations
Applications of Lie Groups to Differential Equations - Olver
but u need to be able to look at a differential equations and find. Lie -algebra in there
@SignorFeynman oh
i was once trying to get a general technique out of this. but I couldn't get very far. it seemed to apply to a very specific class of diff eqns
@SignorFeynman thanks
the idea I had was that, if i have a diff eqns dx/dt = f(x,p) and dp/dt=g(x,p), and if I am able to map x and p to operators on a vector space, and if I am able to re-write the equation as dx/dt=[O, X] for some O, then I can use this technique
14:09
@SignorFeynman that book seems to fill a unique niche. I started on it last year but haven't made much progress
I haven't read it so far, I only know of it from Qmechanic's answers :P
And I'm a bibliography maniac
iirc there's some stuff on Noether I couldn't find elsewhere
That's the context of those answers
Probably it was related to Noether's second theorem
when I read the intro to the Olver book it was so surprising and seemingly profound that I texted two maths postdocs asking if they knew this stuff and if so why I had never been taught it before :P and at least one answered "cos I didn't know it either"
On average, math people are not very accustomed with Lie theory, unless they are geometers
14:14
that seems surprising to me
I would dare to say that the average physicist has a superior running knowledge about Lie groups :P
I may be mistaken, though. That's just the sample of mathematicians that I know
yeah it's so central in physics
I'm bewildered. I've just found one book about applications of Lie groups to DIFFERENCE equations
I suspect they mean something else by "difference equation"
:S
weird indeed
Oh, no. They really mean difference equations
Applications of Lie Groups to Difference Equations - Vladimir Dorodnitsyn
I'll never open that again :P
14:27
I thought lie groups would imply CTS stuff and difference eqns discrete stuff...
i think the crucial idea here is carrying over the Lie bracket structure from the vector fields to the functions
like, carrying over the commutator of vector fields to the Poisson bracket of functions
and once we have a Lie algebra structure on the functions, we can use this technique
so, in what ways can one inherit a Lie algebra on the functions using the commutator on vector fields. the Poisson bracket is one such way
like, the Poisson bracket satisfies $[X_f, X_g]=X_{\{f,g\}}$
@qwerty same
@SignorFeynman xD. it sounds intriguing tho
fqq
fqq
15:22
@SignorFeynman as in "know how to run away from it"
16:04
I was thinking about the running coupling, but I guess that'll do :P
 
3 hours later…
19:13
gauge field of SU(3) does such a field exist? Isn't a gauge field a QFT that is invariant under gauge transformation. And isn't SU(3) a transformation that changes coordinates, which is the opposite of a gauge transformation ?
It does exist (QCD) and it is not a coordinate transform
isn't SU(3) spatial rotation ?
19:31
No, that's $\mathrm{SO}(3)$ and a gauge field is not a QFT
so a massless spin 1 vector field is not QFT?
I jyst mean that a gauge field is not the gauge theory
It's like saying that a wavefunction is quantum mechanics
19:47
I am talking about a gauge field being a quantum field which is invariant under gauge transformation
but anyway I got So and SU mixed
20:13
Can someone help me understand what structures I am dealing with here
for a)
Because I am confused
what is a three-component complex scalar field ?

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