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General chat for Physics SE (physics.stackexchange.com). For M...
14:28
@ACuriousMind Oks thank you
13:45
@Slereah Ok thank you
13:43
2.) Momentum in CM: $\{\cdot,p\}=\frac{\partial \cdot}{\partial q}$

in QM $\hat p=-i\hbar\nabla$ its similar.

What about $\{\cdot,q\}=-\frac{\partial \cdot}{\partial p}$ in QM, is there expression akin to the momentum one in QM?
13:42
1.) Momentum is the generator of translation $\{f,p\}=\frac{\partial f}{\partial q}$

$q$ is the generator of momentum, but from the Poisson brackets, I get it with the $-$ sign: $\{f,q\}=-\frac{\partial f}{\partial p}$ by definition. Is it correct than to say that "$q$ is the generator of momentum" or should I now say that the "$q$ is the negative generator of momentum" or sth like that? It bothers me that both expressions are not the same, but we talk like they are. Or am I missing something?
09:50
@SirCumference Sir Cumference really cool name xD
09:49
@ACuriousMind True
09:40
@naturallyInconsistent Yeah, thats the whole formalism. It would be cool if it was like the Poisson-Hamilton equation or Hamilton-Poisson.
yst 21:11
Ok thanks
yst 21:11
@ACuriousMind It doesn't exist, yeah
yst 21:03
If asking such question makes sense xD
yst 21:02
In theory at the exact same time*
yst 21:02
What do I get when I measure spin along 2 different axis, but at the same time?
yst 19:31
I want to learn more about density matrix, mixed states, phase space formalism; but I am looking for a gentle intro to those topics. Does such a book exist?
yst 16:56
@RyderRude Hah ok thanks.
yst 16:55
@Feynmate Ok thanks
yst 16:08
What is this equation called in the literature $\dot f = \{f,H\}$ ? Classical Heisenberg equation of motion? I couldn't find much sources that name it explicitly.
Wed 17:12
@Feynmate xD
Tue 21:16
@TobiasFünke Maybe I overcomplicated, disregard the equations. All in all, saying that "Schrodinger equation is a statement of conservation of energy" is not a correct statement (even meaningless), right?
Tue 21:14
@TobiasFünke Ok thanks.
Tue 19:36
I saw on one page today (not about physics, but a page connected with education in general; some university information posts and some administration): "Schrodinger equation can be regarded as a statement of conservation of energy in quantum mechanics." Idk why they are writing about the Schrodinger equation at all. xD

But how wrong is that?

I think it is wrong, because (I guess) the person writing that thinks that $i\hbar\frac{\partial \psi}{\partial t}\equiv \hat E= \hat H \psi$ so $\hat E= \hat H \psi$ and that is wrong. Should I notify them that that post is wrong?
Tue 19:05
Good evening
Tue 15:04
Alright, thanks.
Tue 14:56
We can integrate the action of a system over arbitrary small time intervals, and hence get arbitrary small values. But does it physically have any meaning when the action of a system is smaller than $h$?
Tue 14:14
@SillyGoose But that is from maths perspective; differential geometry. I was thinking more about mechanics but described via geometry.
Tue 14:12
@Slereah Hm. Thanks. That occured to me, but I wanted to be more specific, otherwise I could just say its "mechanics".
Tue 13:55
When talking about geometric mechanics (1) , symplectic geometry (2), contact geometry (3), Poisson geometry (4) , usage of Lie groups in mech,...

What would be the "roof" term that accompanies all of that? Is it geometric mechanics?
Tue 13:37
@DIRAC1930 Boltzmann would agree
Tue 13:36
@RyderRude Doing too much philosophy without physical exercise is not a good thing. Mens sana in corpore sano.
Feb 15 21:52
@ACuriousMind Ok thanks.
Feb 15 21:52
@ACuriousMind Its not. I just found about it today. Like Schrodinger equation for open systems.
Feb 15 21:51
@ACuriousMind So for most systems considered in QM the ehrnfest theorem is useless?
Feb 15 21:50
@ACuriousMind Have you heard of Lindbladian ?en.wikipedia.org/wiki/Lindbladian
Feb 15 21:49
It is a coincidence that $V(\langle x\rangle) = \langle V(x)\rangle$ when $U$ is quadratic.
Feb 15 21:49
@ACuriousMind True
Feb 15 21:47
But only for "nice" systems. That have nice quadratic at max potentials.
Feb 15 21:46
@RyderRude I was reading about Ehrnfest theorem, the expecectation values of the operators correspond to the classical behaviour of the system.
Feb 15 21:39
Here is a really nice answer by Terrence Tao that talks about different types of viewing mechanics:
https://mathoverflow.net/questions/225814/does-quantum-mechanics-ever-really-quantize-classical-mechanics
Might be helpfull for someone
Feb 15 12:38
@TobiasFünke Ah ok thanks.
Feb 15 12:37
@ACuriousMind Understandable. I will restrain for asking such questions furthermore. Although some of the answers I got in this chat were helpful, so I am thankful for that.
Feb 15 12:32
True true
Feb 15 12:30
But I agree with you 100%
Feb 15 12:30
Yes yes I understand that. But it is a super fast resource
Feb 15 12:29
xD
Feb 15 12:28
Often, however, the Schrödinger equation is difficult to solve (even with a computer). "Therefore, physicists have developed mathematical techniques to simplify these problems and clarify what is happening physically. One such technique is to apply a unitary transformation to the Hamiltonian. Doing so can result in a simplified version of the Schrödinger equation which nonetheless has the same solution as the original."
Feb 15 12:27
I read this on the wiki en.wikipedia.org/wiki/…
Feb 15 12:26
2.) Do some people do unitary transformations on the Hamiltonian, and calculate the evolution on a system that way, instead of solve the Schrodinger equation?
Feb 15 12:25
No until now. I think I understand it now. We use unitary transformations because they preserve the inner product, so measurements will always be correct.

And it is U dagger on the left because that is how a bra transforms under a unitary transformation and U on the right because that is how a ket transforms under a UT.
Feb 15 11:45
It reminds me of kind of when you act on a vector with a rotation matrix from one side and its transponse on the left to make a rotation.
Feb 15 11:45
Hm. My question is than this:

When considering a unitary transformation of a state $\psi$ if we want $\psi '$ we get it by $\psi '= \hat U(t) \psi$. Ok.

For operators we do:

$\hat A'=\hat U \hat A U^\dagger$

Why do we do it in that way for transforming operators?
Feb 15 11:36
So just because $U(t) is time dependant it turns $\hat A_S$ into a time dependant quantity?