Polarizaition and susceptibility

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SUMMARY

The relationship between linear polarization and susceptibility is expressed in two forms: time domain as P(t) = χE(t) and frequency domain as P(ω) = χ(ω)E(ω). The time-dependent equation should be represented as a convolution integral, P(t) = ∫ χ(t-τ)E(τ)dτ, which transforms into the frequency domain via Fourier transform. A frequency-dependent susceptibility indicates dispersion, and if the material's response is instantaneous, the convolution simplifies to the first expression. This clarification highlights the importance of understanding the convolution relationship in polarization and susceptibility.

PREREQUISITES
  • Understanding of linear polarization and susceptibility in materials
  • Familiarity with convolution integrals in signal processing
  • Knowledge of Fourier transforms and their applications
  • Basic principles of dispersion in physics
NEXT STEPS
  • Study the convolution theorem in the context of linear systems
  • Explore frequency-dependent susceptibility in materials science
  • Learn about the applications of Fourier transforms in electromagnetism
  • Research texts that detail the relationship between polarization, susceptibility, and electric fields
USEFUL FOR

Physicists, materials scientists, and students studying electromagnetism or optics who seek to deepen their understanding of polarization and susceptibility relationships.

KFC
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In some unit, the relation of (linear) polarization and susceptibility can be written of

[tex]P(t) = \chi E(t)[/tex]

but I also read some expression in other text reads

[tex]P(\omega) = \chi(\omega) E(\omega)[/tex]

why change the time to frequency? Why polarization depends on frequency?
 
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Your equations are not really written correctly. The first one, the time dependent one, should really be written as a convolution: The polarization of a linear isotropic medium with a local but noninstantaneous response (but still independent of time) is:

P(t)=[itex]\int \chi(t-\tau)E(\tau)d\tau[/itex]

And taking the Fourier transform of this equation provides your second expression.

If the material responds instantaneously and has no memory[[itex]\chi(t-\tau) = \chi\delta(t-\tau)[/itex]], then the convolution integral reduces to your first expression.

Having a frequency-dependent susceptibility is simply dispersion.
 
Andy Resnick said:
Your equations are not really written correctly. The first one, the time dependent one, should really be written as a convolution: The polarization of a linear isotropic medium with a local but noninstantaneous response (but still independent of time) is:

P(t)=[itex]\int \chi(t-\tau)E(\tau)d\tau[/itex]

And taking the Fourier transform of this equation provides your second expression.

If the material responds instantaneously and has no memory[[itex]\chi(t-\tau) = \chi\delta(t-\tau)[/itex]], then the convolution integral reduces to your first expression.

Having a frequency-dependent susceptibility is simply dispersion.

Oh ... I just wonder why in textbook they don't say it is a convolution! So you mean in frequency domain susceptibility is the repsonse function?

BTW, can you tell me one text in which the author show clearly the convolution relation b/w polarization, susceptibility and field? I am writing a short report and need a reference
 

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