Course of theoretical physics: Electrodynemics of continuous media |
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Page 375
We shall also suppose that the medium has no magnetic structure. First of all, we
shall show that under these conditions the non-linear permittivity is real. This
could be seen directly by expressing the components of the non-linear
susceptibility ...
We shall also suppose that the medium has no magnetic structure. First of all, we
shall show that under these conditions the non-linear permittivity is real. This
could be seen directly by expressing the components of the non-linear
susceptibility ...
Page 392
We see that the non-linear action of the field E, on the field with frequency m2 can
be described by means of an anisotropic permittivity 32111 =15: +'1zE1'E1")51x
+)82E11E111* +l'2E11'E1|=~ 1112-4) In a non-dissipative medium, the ...
We see that the non-linear action of the field E, on the field with frequency m2 can
be described by means of an anisotropic permittivity 32111 =15: +'1zE1'E1")51x
+)82E11E111* +l'2E11'E1|=~ 1112-4) In a non-dissipative medium, the ...
Page 426
This expression differs from the one for the field in a vacuum (see QED, §2) by
the factor (u/\/s)"1 in the normalization coefficients, which originates from the
factor \/s/u in the energy density (83.9) for a plane electromagnetic wave in the
medium ...
This expression differs from the one for the field in a vacuum (see QED, §2) by
the factor (u/\/s)"1 in the normalization coefficients, which originates from the
factor \/s/u in the energy density (83.9) for a plane electromagnetic wave in the
medium ...
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angle anisotropy anisotropy energy antiferromagnetic atoms axes axis body boundary conditions calculation charge circuit coefficient coefficients components conductor constant coordinates corresponding cross-section crystal Curie point curl H defined definition denote dependence derivatives determined dielectric diffraction direction discontinuity dissipation domains electric field electromagnetic field electrons ellipsoid energy flux expression external field external magnetic field ferroelectric ferromagnet field H find finite first first term flow fluctuations fluid formula free energy frequency function given gives grad Hence incident induction infinite integral isotropic Landau theory layer linear magnetic field magnetohydrodynamics magnetostriction magnitude medium normal obtain optical particle permittivity perpendicular perturbation phase plane polarization PROBLEM propagated properties pyroelectric quantities reflection refraction relation respect result rotation satisfied scattering shock wave significance solution sphere superconducting surface symmetry tangential temperature tensor theory thermodynamic potential transition uniaxial upper half-plane values variable velocity volume wave vector z-axis zero