I went through the book "Surface Plasmons on Smooth and rough surface and on Gratings by Raether." If you look at the equations 2.4, 2.5, and 2.6 in the link below:
https://ui.adsabs.harvard.edu/link_gateway/1988STMP..111.....R/doi:10.1007/BFb0048317
Going through the 2nd page, we have the resonance condition of the surface plasmons:
kx=ωc(ϵ1ϵ2/ϵ1+ϵ2)^1/2
Here,
ϵ1,ϵ2ϵ1,ϵ2
are the dielectric permittivity of the metal and dielectric medium.
Where the dielectric medium of the metal is given by :
ϵ1=ϵ1′+iϵ1′′
and the dielectric medium permittivity is given as:
ϵ2
Are we considering the medium to be lossless as an assumption
Now, if we have a real
ω and ϵ2
we consider that the wave vector to have a real and imaginary part where:
kx=kx′ + ikx"
Real part of the wave vector is given by following expression:
kx′=ωc(ϵ1′ϵ2/ϵ1′+ϵ2)^1/2
and the imaginary part for the wave vector is given by the following expression:
kx"=ωc(ϵ1′ϵ2/ϵ1′+ϵ2)^3/2 (ϵ1"/2(ϵ1′2))
I would like to know how the mathematical expression values of
kx′ and kx′′
are obtained.
Can anyone please helo and suggest how these expressions are obtained.