Dielectric Function: Relation to Frequency & Wavevector

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    Dielectric Function
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Discussion Overview

The discussion centers on the relationship between the dielectric function, frequency, and wavevector, exploring theoretical aspects and implications in various contexts. Participants inquire about specific conditions for the dielectric function at different limits and the underlying reasons for these choices.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants propose that the dielectric function depends on both frequency and wavevector independently, as the response of the system can be probed with varying parameters.
  • Others argue that when probing with light, the frequency and wavevector are related by the equation ω/k=c, but this relationship may not hold in all media.
  • A participant notes that the response of the system is a property of the system itself and is independent of the type of probe used, whether it be light, electrons, or neutrons.
  • One participant mentions that the permittivity's dependence on frequency is complex and ultimately tied to the band structure of the medium, with a characteristic shape in isotropic media approximated by specific equations.
  • Another participant highlights that in solid state physics, k=0 is chosen for plasma oscillation while ω=0 is used for potential screening, suggesting these are pedagogical choices based on simplicity and familiarity.
  • It is noted that the macroscopic response of electrons in plasma oscillation corresponds to k approaching zero but involves finite frequency, while static screening considers a point charge at rest.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the independence of frequency and wavevector, as well as the implications of specific choices in the dielectric function. The discussion remains unresolved with no consensus on the best approach or interpretation.

Contextual Notes

Limitations include the complexity of the dielectric function's dependence on the medium's band structure and the potential variations in permittivity across different contexts. The discussion also reflects a range of pedagogical choices that may not encompass the full complexity of the topic.

sinayu71
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Hi guys:

Could someone kindly explain the relation between dielectric funciton (e) and frequency, wavevetor? What is the condition for wavevector e(k=0, w), e(k, w=0) and why?

Thanks a lot :smile:
 
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the dielectric function depends on both the frequency and wave-vector independently because I get to choose with what frequency and with what wave-vector I probe the system. The system will respond and the response is given by the dielectric function. For example, if I wanted to know how the system responds to a very long wavelength (k->0) probe I would care about [tex]\epsilon(k=0,\omega)[/tex]. If, on the other hand, I rather care about the response to time-independent fields of finite wave-length I would instead care about [tex]\epsilon(k,\omega=0)[/tex].
 
Are we talking probing with light here? In that case the frequency and the wavevector are not independent but related by [tex]\omega/k=c[/tex], right?
 
Repetit said:
Are we talking probing with light here?

not necessarily. the response of the system is a property *of the system* and is independent of the probe used be it light or electrons or neutrons or etc.
 
Repetit said:
Are we talking probing with light here? In that case the frequency and the wavevector are not independent but related by [tex]\omega/k=c[/tex], right?
Only in a vacuum. Inside a medium, particularly media whose permittivity varies as a function of position (waveguides, photonic crystals for example), the dispersion relation can get quite complex.

Sinayu71 - There is no simple way to obtain how the permittivity changes with frequency, since this function ultimately depends on the band structure of the medium.

For a regular, isotropic medium however, the permittivity does have a characteristic shape (minus the kinks and other perturbations), approximated in the optical region of the spectrum by the Selmier (sp?) equations.

Claude.
 
in the solid state physics book, when determine the plasma ocillation, k =0 is chosed in the dielectric funtion. However, the w=0 is chosed when discuss the potential screening. Can someone explain it?

thank you :shy:
 
It's a pedagogical choice and nothing more. Those two simple cases are presented *because* they are simple and well known limits; a general study of the dielectric function is not at the level of any textbook.

In the first example you give (plasma oscillation) one thinks of all the electrons moving together in the whole macroscopic metal--this response is obviously of macroscopic wavelength ([tex]k \to 0[/tex]) but finite frequency. For finite wavelength the plasma frequency is not the same as the k=0 case discussed in textbooks and is much more difficult to determine.

In the second example, one considers the static ([tex]\omega = 0[/tex]) screening of a point charge. If the point charge were not at rest in the solid the problem would again be more difficult.
 

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