- Electric susceptibility
The electric susceptibility χe of a
dielectric material is a measure of how easily it polarizes in response to anelectric field . This, in turn, determines the electricpermittivity of the material and thus influences many other phenomena in that medium, from the capacitance ofcapacitors to thespeed of light .It is defined as the constant of proportionality (which may be a
tensor ) relating anelectric field E to the induceddielectric polarization density P such that:mathbf P}=varepsilon_0chi_e{mathbf E},
where varepsilon_0 is the electric
permittivity of free space.The susceptibility of a medium is related to its relative
permittivity varepsilon_r by:chi_e = varepsilon_r - 1.
So in the case of a vacuum,
:chi_e = 0.
The
electric displacement D is related to the polarization density P by:mathbf{D} = varepsilon_0mathbf{E} + mathbf{P} = varepsilon_0 (1+chi_e) mathbf{E} = varepsilon_r varepsilon_0 mathbf{E}.
Dispersion and causality
In general, a material cannot polarize instantaneously in response to an applied field, and so the more general formulation as a function of time is
:mathbf{P}(t)=varepsilon_0 int_{-infty}^t chi_e(t-t') mathbf{E}(t'), dt'.
That is, the polarization is a
convolution of the electric field at previous times with time-dependent susceptibility given by chi_e(Delta t). The upper limit of this integral can be extended to infinity as well if one defines chi_e(Delta t) = 0 for Delta t < 0. An instantaneous response corresponds toDirac delta function susceptibility chi_e(Delta t) = chi_e delta(Delta t).It is more convenient in a linear system to take the Fourier transform and write this relationship as a function of frequency. Due to the
convolution theorem , the integral becomes a simple product,:mathbf{P}(omega)=varepsilon_0 chi_e(omega) mathbf{E}(omega).This frequency dependence of the susceptibility leads to frequency dependence of the permittivity. The shape of the susceptibility with respect to frequency characterizes the dispersion properties of the material.
Moreover, the fact that the polarization can only depend on the electric field at previous times (i.e. chi_e(Delta t) = 0 for Delta t < 0), a consequence of
causality , imposes Kramers–Kronig constraints on the susceptibility chi_e(0).ee also
*
Application of tensor theory in physics
*Magnetic susceptibility
*Maxwell's equations
*Permittivity
*Clausius-Mossotti relation
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