The dielectric function of a metal using LD model.

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SUMMARY

The discussion focuses on the dielectric function of metals using the Lorentz-Drude (LD) model, contrasting it with the classical dielectric function ε(w) = ε’ + iε’'. The LD model incorporates both intraband (free-electron) and interband (bound-electron) effects, with the imaginary part representing attenuation through Lorentzian absorption lines. Participants seek clarification on the symbolic form of the dielectric function as applied in the LD model, particularly in relation to the equations presented in the paper "Optical Properties of Metallic Films for Vertical-Cavity Optoelectronic Devices." The conversation highlights the importance of Kramers-Kronig relations in deriving the real part of the dielectric function.

PREREQUISITES
  • Understanding of the Lorentz-Drude model in solid-state physics
  • Familiarity with Kramers-Kronig relations
  • Knowledge of dielectric functions and their components
  • Basic grasp of optical properties of materials
NEXT STEPS
  • Study the derivation of the dielectric function in the Lorentz-Drude model
  • Research Kramers-Kronig relations and their applications in optics
  • Examine the symbolic forms of dielectric functions in various materials
  • Explore the optical properties of metallic films in optoelectronic devices
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Researchers in condensed matter physics, materials scientists, and anyone studying the optical properties of metals and their applications in optoelectronics.

sixers0130
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I'm studying the dispersive properties of metals using Lorentz-Drude model, but I'm confused about the equation set-up.

What is LD model different from the classical dielectric function using for other dielectrics? Namely: ε(w) = ε’ + iε’' where the imaginary part is the attenuation.

In LD model, ε is composed of intraband (free-electron) effects and interband (bound-electron) effects. Physically what do they mean?

Thanks for the help!
 
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btw, does anyone know what is the dielectric function (in symbolic form) they are using?

http://ab-initio.mit.edu/wiki/index.php/Meep_Tutorial/Material_dispersion
 
sixers0130 said:
btw, does anyone know what is the dielectric function (in symbolic form) they are using?

http://ab-initio.mit.edu/wiki/index.php/Meep_Tutorial/Material_dispersion
You could be a bit more specific. Do you mean the first formula ## \epsilon=(ck/\omega)^2##? That is just the relation between the dielectric constant and the index of refraction ##\epsilon=n^2##.

It would be useful if you could cite the form of the LD model you are referring too.
I think the Lorentz Drude model assumes absorption (or equivalently imaginary part of epsilon) to be described by a sum of Lorentzian lines. The real part can then be obtained using Kramers Kronig relations. The absorption lines are due to inter- or intraband transitions.
 
Dear DrDu,

Thanks for the reply and sorry about the confusing! I mean the second formula from the page where numbers are used to plug in. I try to compare this one with LD model from the paper "Optical Properties of Metallic Films for Vertical-Cavity Optoelectronic Devices" where equations are stated in the attachment.

They look very similar. I try to compare if there is just some variable exchange but couldn't find it. So I'm just wondering what would the symbolic form of the second equation from the site would be.

Thanks so much for the help again!
(btw can someone teach me how to type equations within text?!)
 

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The terms with the "b" (supposedly for band or bound) describe the reaction of bound electrons in a harmonic oscillator with frequency ##\omega_j##. Correspondingly the f_jare called oscillator strengths.

Up to the 1, the term with "f" can be seen to be of a similar form with ##\omega_j## being equalt to 0. Hence these electrons are unbound or free.
 

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