Group velocity and phase velocity of a matter wave

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Discussion Overview

The discussion centers around the relationship between group velocity and phase velocity of matter waves, specifically exploring the derivation of the phase velocity from the relation \(\omega^{2} = k^{2}c^{2} + \frac{m^{2}c^{4}}{\hbar^{2}}\). Participants engage in mathematical reasoning to clarify these concepts, with a focus on the conditions under which these velocities are defined.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant successfully derives the group velocity as \(v_g = c^2\) from the given relation.
  • Another participant suggests that differentiating the expression for \(\omega(k)\) yields \(v_g = \frac{k}{\omega}c^2\), leading to confusion regarding the relationship between phase velocity and particle velocity.
  • Some participants argue about the correct expression for phase velocity, with one asserting that it is \(v_p = \frac{c^2}{v}\), while others challenge this interpretation.
  • There is a contention over the correct differentiation process, with some participants advocating for a direct approach without taking the square root, while others provide alternative methods.
  • One participant expresses frustration over perceived misunderstandings and mistakes made by others regarding the definitions and relationships of the velocities involved.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the derivation of the phase velocity and its relationship to particle velocity. Multiple competing views and interpretations of the mathematical relationships remain unresolved.

Contextual Notes

The discussion highlights limitations in assumptions regarding the definitions of phase and group velocities, as well as the conditions under which these relationships hold true. There are unresolved mathematical steps and differing interpretations of the differentiation process.

andrepd
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Hi. Today I sat my final first year Modern Physics exam. It went very well, however I got stuck in one question. It asked (i) to prove the following relation for the matter wave \omega^{2}=k^{2}c^{2}+m^{2}c^{4}/\hbar^{2} and (ii) to obtain the group velocity and phase velocity of a matter wave from that relation. (i) was easy, so was obtaining the group velocity, but I got stuck on obtaining c^2/v for the phase velocity. If someone could walk me thorough that deduction, I would appreciate it. Thanks.
 
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The phase velocity is v = ω/k. The group velocity is g = dω/dk. Differentiate the relationship you have, and you get 2 ω dω/dk = 2k c2, which immediately gives you vg = c2.
 
If I'm not mistaken, differentiating our expression for ω(k) yields vg=(k/ω)c^2, which, if we know beforehand that the phase velocity equals c^2/v, can express as vg=v. However, I'm unsure how we get from vf = ω/k = \sqrt{\frac{k^{2}c^{2}+m^{2}c^{4}/\hbar^{2}}{k^{2}}} to vf=c^2/v.
 
andrepd said:
If I'm not mistaken
You're mistaken.
 
Bill_K said:
You're mistaken.

Care to explain then? dω/dk=d/dk(\sqrt{k^{2}c^{2}+m^{2}c^{4}/\hbar^{2}})=1/2*(k^{2}c^{2}+m^{2}c^{4}/\hbar^{2})^{-1/2}*2kc^{2}=\frac{k}{\omega}c^{2}=\frac{v}{c^{2}}*c^2=v

This was my thought process. Care to point my mistake?

EDIT: This, however, presumes previous knowledge that vf=c^2/v. Hence my question.
 
andrepd said:
Care to explain then? =\frac{k}{\omega}c^{2}=\frac{v}{c^{2}}*c^2=v
This was my thought process. Care to point my mistake?.
In the last step you've used v = k/ω, whereas actually v = ω/k.

It's easier anyway to do it the way I showed. Do NOT take the square root. Simply differentiate the given relationship as it stands. The LHS is ω2, and its derivative is 2 ω dω/dk. The RHS is k2c2 + m2c42, and its derivative is 2 k c2. That gives what you want immediately.
 
This yields the the same result for the *group* velocity. However, I am having trouble with the derivation of the *phase* velocity, \omega/k, which, in the context of matter waves, is not equal to v, but rather to c^2/v.
 
The phase velocity is always ω/k, andrepd, I don't care what the context. It's the group velocity that may differ. This is a general fact for wave motion of any kind: sound waves, water waves, gravity waves, matter waves or what have you. The phase velocity is the velocity at which a wave crest travels, and the expression for it just comes from taking exp(i(kx - ωt)) and rewriting it as exp(ik(x - vt)), from which v = ω/k. If you're still not clear, I suggest you read the Wikipedia page.
 
I know that, however, that is now what I was looking for. I know that the phase velocity equals ω/k. Again, I wanted to know how I can prove this relation \omega/k=\sqrt{\frac{k^{2}c^{2}+m^{2}c^{4}/\hbar^{2}}{k^{2}}}=c^{2}/v

I've figured it now. For the record:

\sqrt{\frac{k^{2}c^{2}+m^{2}c^{4}/\hbar^{2}}{k^{2}}}=\sqrt{c^{2}+\frac{m^{2}c^{4}}{k^{2}\hbar^{2}}}=\sqrt{c^{2}+\frac{m^{2}c^{4}}{\gamma^{2}m^{2}v^{2}}}=\sqrt{c^{2}+(1-v^{2}/c^{2})\frac{c^{4}}{v^{2}}}=\sqrt{c^{2}+\frac{c^{4}}{v^{2}}-c^{2}}=c^{2}/v

That was it.
 
  • #10
I know that the phase velocity equals ω/k
You've said repeatedly that it wasn't.
I've figured it now.
Good. Now try figuring out the easier approach in #2.
 
  • #11
You. are. wrong. I don't know if you still haven't understood what I needed, but you nevertheless made several mistakes.

"vg = c2"
It's not, according to the very wikipedia article you linked me to, vg = c2/v, where vg is the group velocity, vp is the phase velocity, and v is the particle velocity.

"You're mistaken."
I most certainly wasn't, seeing as your next post contained the exact same differentiation I made, calculated in a slightly different way.

"In the last step you've used v = k/ω, whereas actually v = ω/k."
I did not. I assumed vg = ω/k = c2/v.

"The phase velocity is always ω/k"
Correct

"v = ω/k"
Incorrect. the phase velocity is ω/k, not the particle velocity. Once again. vp = ω/k = c2/v

"You've said repeatedly that [phase velocity] wasn't [equal to] ω/k."
I searched the thread, and can find no statement of the sort. I find this:
derivation of the *phase* velocity, ω/k,
 

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