Faster than light in Quantum mechanics?

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Discussion Overview

The discussion revolves around the implications of phase and group velocities of electromagnetic waves in the context of quantum mechanics and de Broglie's theory. Participants explore the relationship between these velocities and the speed of light, particularly in materials like copper, and consider the validity of applying de Broglie's equations to different types of waves.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that the phase velocity of electromagnetic waves must always be greater than or equal to the speed of light, c, and challenge the initial analysis presented.
  • Others argue that the analysis conflates the phase velocity with the actual movement of energy, suggesting that group velocity should be considered instead.
  • A participant mentions that the group velocity in conductors can be twice that of the phase velocity, raising questions about their roles in de Broglie's theory.
  • There is a suggestion that the analysis may have overlooked quantum effects and involved integration over large areas and time increments, potentially washing out high-frequency effects.
  • Some participants discuss the implications of applying de Broglie's theory to massless particles and electromagnetic waves, noting that strange results can arise without proper modifications.
  • One participant introduces the concept of neutrinos potentially traveling faster than light due to their small mass and interactions with dark energy, although this remains speculative.
  • Several participants reference historical developments in the understanding of group and phase velocities, emphasizing the need for careful consideration of mass in the context of wave mechanics.
  • There is a discussion about the validity of the relationship v_p v = c^2 in vacuum versus in materials, with some asserting that it holds true for photons in vacuum but not necessarily in other contexts.
  • Participants explore the mathematical derivation of phase and group velocities from dispersion equations, indicating a technical approach to understanding these concepts.

Areas of Agreement / Disagreement

Participants express differing views on the application of de Broglie's theory to electromagnetic waves and the implications of phase and group velocities. There is no clear consensus, as multiple competing perspectives remain throughout the discussion.

Contextual Notes

Limitations include potential misunderstandings of the relationship between phase and group velocities, the assumptions made regarding energy movement, and the specific conditions under which de Broglie's theory is applied. The discussion also highlights the complexity of integrating quantum effects into classical wave theory.

stgdf01
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In <Engineering Electromagnetics> written by W.H.Hayt and J.A.Buck( 6th edition,McGraw-Hill,p372), the phase velocity vp of electromagnetic waves in copper at 60Hz (commercial electric power) is 3.2m/s. Substituting the value into vpv = c2 of de Broglie theory, v=108c should be much faster than light speed c in vacuum?
 
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Hi stgdf01 and welcome to the forum,

The analysis you posted sounds incorrect. Phase velocity (of the EM wave) must always be greater or equal to c. The analysis seems to have been done with the assumption that the AC voltage wave represents the actual movement of energy. It doesn't. The energy travels far quicker than the swinging of the voltage. But maybe the person doing the analysis meant the velocity of the conduction current? If so, then group velocity vg rather than phase velocity is the correct term to use.

vp vg= c2
 
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PhilDSP said:
The analysis you posted sounds incorrect. Phase velocity (of the EM wave) must always be greater or equal to c. The analysis seems to have been done with the assumption that the AC voltage wave represents the actual movement of energy. It doesn't. The energy travels far quicker than the swinging of the voltage.

The study to vp in conductors is based on first principle(Maxwell's equations) and has nothing to do with parameters in circuit theory such as voltage,inductance and capacitance. For example, J.D.Jackson's <Classical Electrodynamics> and D.J.Griffiths's <Introduction to Electrodynamics>.



PhilDSP said:
If so, then group velocity vg rather than phase velocity is the correct term to use.

vp vg= c2


The group velocity vg=dw/dk of low-frequency electromagnetic field in conductors is twice as much as vp=w/k (P.Lorrain, D.R.Corson, F.Lorrain, <Electromagnetic Fields and Waves>, 3rd edition). For commercial power in copper, vp=3.2m/s and vg=6.4m/s. In this case, neither vp nor vg can play the role of c2/vp in de Broglie's theory. Actually, it is v=p/m (m=E/c2) in point mechanis.
 
stgdf01 said:
In this case, neither vp nor vg can play the role of c2/vp in de Broglie's theory.

It sounds likely that the analysis involved integration over macroscopic areas of space and large increments of time. In that case the average variation of the EM values would have washed out the high frequency effects. That's what I was trying to express in the first response. The analysis apparently ignores quantum effects.
 
stgdf01 said:
Substituting the value into vpv = c2 of de Broglie theory, v=108c should be much faster than light speed c in vacuum?

This result of de Broglie theory is usually explicitly derived for matter waves. You will of course get strange results when you try to use it without proper modification for particles without rest mass and em waves.
 
neutrinos as being said faster than light,,have very small mass and could be compound of gravity also accelerating speed such as dark energy particles..therefore interacting with light much like gravity does..as a mediator..a boson wave..already there..QED
 
Cthugha said:
This result of de Broglie theory is usually explicitly derived for matter waves. You will of course get strange results when you try to use it without proper modification for particles without rest mass and em waves.



E=hw and p=hk is of course tenable to photons otherwise the Compton effect, photoelectric effect, blackbody radiation and others cannot be interpreted. In history, these two relations are concluded from experiments to massless photons and then de Broglie extended to massive matter waves(electrons,say).
 
stgdf01 said:
E=hw and p=hk is of course tenable to photons[...]

Sure, but that does not have anything to do with [tex]v_p v=c^2.[/tex] This result is derived explicitly in the nonrelativistivc limit for matter waves and requires w and p to depend on mass. Some good textbooks on this topic state this explicitly. Even the really basic about about basic knowledge for engineers by Hennecke mentions this.
 
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Cthugha said:
Sure, but that does not have anything to do with [tex]v_p v=c^2.[/tex] This result is derived explicitly for matter waves and requires w and p to depend on mass. Almost every good textbook on this topic states this explicitly. Even the really basic about about basic knowledge for engineers by Hennecke mentions this.

Actually the history behind that for waves in general extends much further back in time:

The idea of a group velocity distinct from a wave's phase velocity was first proposed by W.R. Hamilton in 1839, and the first full treatment was by Rayleigh in his "Theory of Sound" in 1877.[6]

http://en.wikipedia.org/wiki/Group_velocity
http://en.wikipedia.org/wiki/John_William_Strutt,_3rd_Baron_Rayleigh
 
  • #10
Cthugha said:
Sure, but that does not have anything to do with [tex]v_p v=c^2.[/tex] This result is derived explicitly in the nonrelativistivc limit for matter waves and requires w and p to depend on mass. Some good textbooks on this topic state this explicitly. Even the really basic about about basic knowledge for engineers by Hennecke mentions this.


But in optics and electromagnetism, [tex]v_p v=c^2.[/tex] is still valid to a field(photons) in vacuum. On the other hand, the photon can be described in relativistic mechanics as a special case of V=c and [tex]m_0=0[/tex]
 
  • #11
PhilDSP said:
It sounds likely that the analysis involved integration over macroscopic areas of space and large increments of time. In that case the average variation of the EM values would have washed out the high frequency effects. That's what I was trying to express in the first response. The analysis apparently ignores quantum effects.

I regards this as a counter-example of [tex]v_p v_g=c^2[/tex],although [tex]v_p v=c^2[/tex] is universal.That is to say, the group velocity vg is not always equal to V. It can be applied to explain why those experiments of superluminal group velocities vg>c are not really faster than light v>c.
 
  • #12
stgdf01 said:
But in optics and electromagnetism, [tex]v_p v=c^2.[/tex] is still valid to a field(photons) in vacuum.

Yes, in vacuum. You were interested in light in a material, no?

stgdf01 said:
On the other hand, the photon can be described in relativistic mechanics as a special case of V=c and [tex]m_0=0[/tex]

You can treat a photon as having [tex]m_0=0[/tex] if you include the full relativistic mass [tex]E=\sqrt{(m_0 c^2)^2 +(p c)^2}[/tex] in the derivation.

However, you get the [tex]v[/tex] in [tex]v_p v=c^2[/tex] in common de Broglie theory by using [tex]p=m v[/tex]. For photons you do not have this explicit dependence and just use [tex]p=\frac{h}{\lambda}[/tex], so you only arrive at the trivial [tex]v_p =\frac{c}{n}.[/tex]
 
  • #13
If we know or can determine the dispersion equation (which doesn't include a mass term) then we can find the phase velocity algebraically and the group velocity by taking the derivative of the dispersion equation (or its roots) with respect to wave number.

[tex]v_p = \frac {\omega}{k} \ \ \ \ \ \ v_g = \frac {\partial \omega}{\partial k}[/tex]

For example: the FT of [itex]\ \ \ (\nabla^2 - \frac {1}{c^2} \frac {\partial^2}{\partial t^2}) \phi = 0 \ \ \[/itex] is [itex]\ \ \ (-k^2 + \frac {\omega^2}{c^2}) \phi = 0 \ \ \[/itex] so that [itex]\ \ \ D(\omega, k) = -k^2 + \frac {\omega^2}{c^2}[/itex]

then [itex]\ \ \ \ \omega = ±ck \ \ \ \[/itex] giving [itex]\ \ \ \ v_p = ±c \ \ \ \[/itex] and [itex]\ \ \ \ v_g = ±c \ \ \ \[/itex]
 
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