Longitudinal plasmon oscillation

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Discussion Overview

The discussion revolves around the concept of longitudinal plasmon oscillation, particularly in the context of dielectric permittivity being zero. Participants explore the implications of this condition on the existence of longitudinal polarization waves and the behavior of electric fields in relation to displacement fields.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions how longitudinal polarization waves can exist if the dielectric permittivity is zero, suggesting that this condition implies no response should occur.
  • Another participant explains that with zero permittivity, it is possible to have an electric field without an associated displacement field, referencing the full Maxwell equations and the existence of free longitudinal solutions at slightly higher frequencies.
  • A different viewpoint is presented regarding the behavior of the dielectric constant at frequencies above the plasma frequency, indicating that while permittivity is zero, the electromagnetic wave equation suggests that the wave vector must also be zero, raising questions about the nature of the solutions.
  • One participant notes that the longitudinal dielectric constant depends on both frequency and wavevector, arguing that if the longitudinal dielectric constant is zero, then the electric field can still represent a longitudinal solution of the free wave equation.

Areas of Agreement / Disagreement

Participants express differing views on the implications of zero dielectric permittivity for longitudinal oscillations, indicating that multiple competing perspectives remain without consensus on the interpretation of the conditions described.

Contextual Notes

Participants reference specific conditions under which the dielectric permittivity is considered zero, and the implications for electric fields and wave solutions, but do not resolve the underlying assumptions or mathematical steps involved in these discussions.

scivet
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Kittel solid state physics book ( chapter 14)says when dielectric permittivity is zero, then longitudinal polarization wave possibly exists. It is hard to imagine how this is possible. Can anybody explain this?
If the permittivity is zero, then there shouldn'n be any response, right? How come the longitudinal mode-are generated?
 
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Given that [itex]D=\epsilon E[/itex], [itex]\epsilon=0[/itex] means that you can have an electric field E without an associated displacement field. If you take the full Maxwell equations you can see that for slightly higher frequencies there exist free longitudinal solutions of these equations which are not bound to external sources.
 
The epsilon is positive at the higher frequency than plasma, which means the transverse propagating wave. Right? So, epsilon is zero, then the electromagnetic wave equation says del^2 E is zero. How does this say the solution is longitudinal? It only says K, the wave vector must be also zero?
 
The longitudinal dielectric constant is a function of both omega and wavevector k.
If [itex]D_L(\omega,k)=0[/itex] due to [itex]\epsilon_L(\omega,k)=0[/itex]then clearly [itex]E_L(\omega, k)[/itex] is a longitudinal solution of the free wave equation.
 

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