Undergrad Phase velocity and frequency of a matter wave

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The discussion centers around the relationships governing matter waves, particularly the equations λ = h / p and E = h f, and their implications for phase velocity and frequency. It highlights the differences between non-relativistic and relativistic quantum mechanics, noting that the inclusion of rest mass energy affects the frequency and phase velocity but not the de Broglie wavelength. The conversation also touches on the challenges of measuring frequency and phase velocity for particles like electrons, suggesting that while wavelength can be inferred from diffraction, frequency remains elusive. Ultimately, the participants agree that the choice of model—non-relativistic or relativistic—determines the applicable equations and interpretations, with no observable quantities being altered by the inclusion of rest energy. The discussion concludes with a recognition that understanding these relationships is crucial for accurately describing matter waves in quantum mechanics.
  • #31
Philip Koeck said:
Are the equations on Wikipedia right?
Post 25 in this thread suggests a different expression connecting E and f.
I think you are confused going between non-relativistic "energy", which is all kinetic, and relativistic "energy", which includes mass-energy. These are not the same quantities. One is not a low-speed approximation of the other.
 
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  • #32
PeroK said:
I think you are confused going between non-relativistic "energy", which is all kinetic, and relativistic "energy", which includes mass-energy. These are not the same quantities. One is not a low-speed approximation of the other.
Yes, I know.
According to the Wikipedia text E = h f, where E is the total relativistic energy, including the rest mass term.
According to post 24 the relationship is E - m0c2= h f, if I'm not mistaken.
I'm simply wondering which of the two is correct for relativistic velocities.
 
  • #33
Philip Koeck said:
Yes, I know.
According to the Wikipedia text E = h f, where E is the total relativistic energy, including the rest mass term.
This must be correct.
Philip Koeck said:
According to post 24 the relationship is E - m0c2= h f, if I'm not mistaken.
I don't see that in post #24.
Philip Koeck said:
I'm simply wondering which of the two is correct for relativistic velocities.
It's the total relativistic energy. It must be.
 
  • #34
PeroK said:
I don't see that in post #24.
In post 24 it says vΦ= ω/k, and then ω is replaced by E - mc2, as I read it. (The h cancels or is set to 1, c is set to 1).
 
  • #35
Particles are not waves and you should not confuse their equations - phase velocity isn't so meaningful for particles.
 
  • #36
Philip Koeck said:
In post 24 it says vΦ= ω/k, and then ω is replaced by E - mc2, as I read it. (The h cancels or is set to 1, c is set to 1).
Okay, I'll let @ergospherical explain that!
 
  • #37
ergospherical said:
Particles are not waves and you should not confuse their equations - phase velocity isn't so meaningful for particles.
Yes, I'm getting that impression.
Just to make sure, from your expression for vΦ, what do you get when v approaches c and does vΦ ever exceed c (as the Wikipedia text claims)?
 
  • #38
Philip Koeck said:
At least to me that leads to a problem.
If it's enough of a problem that its effect on your answer matters, then obviously you are dealing with a case where the non-relativistic approximation won't work for you and you need to use the relativistic equations.
 
  • #39
Philip Koeck said:
I'm simply wondering which of the two is correct for relativistic velocities.
In relativity rest mass is part of the total energy. So it has to be included.
 
  • #40
ergospherical said:
In the relativistic region the phase velocity is ##v_{\phi} = \omega/k = (E-m)/p##, i.e.\begin{align*}
v_{\phi} = \frac{\gamma - 1}{\gamma v}
\end{align*}For small ##v## expand ##\gamma = (1-v^2)^{-1/2} \sim 1 + v^2/2## (and similarly ##1/\gamma \sim 1-v^2/2##) to get\begin{align*}
v_{\phi} &\sim \frac{(v^2/2)}{v}(1-v^2/2) \sim \frac{v}{2}
\end{align*}omitting terms ##O(v^3)##.
Could you share a source for the relationships you use in the first line?
Especially E -mc2= ħω, if that is what you are using.
Is there a book that says that?
 
  • #41
Philip Koeck said:
When I write m I mean the relativistic mass, not the rest mass.
Don't do that. It kinda sort of works if you're just doing a semester or so of special relativity with classical objects (but even that is discouraged these days - why start with something that has to be unlearned to move beyond that first semester or so?) but fails dismally as soon as you start thinking quantum mechanics.

With QM in the picture: If relativity doesn't matter there is no relativistic mass, if it does matter you have to use the relativistic ##E^2=(mc^2)^2+(pc)^2## instead of anything involvng relativistic mass.
 
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  • #42
A (hopefully) final question on this:
Clearly the wavelength of a matter wave can be measured directly in a diffraction experiment so the relation p = h k can be tested experimentally by sending particles of known p through a grating.

Is there a similar way to test E = h f?
Can f be measured directly without inferring it from E?

Or, alternatively, is there a way to measure the phase velocity of a matter wave?
 

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