multilayer: multilayer
In planar: Multilayer Optics

Description Usage Arguments Details Value Author(s) References

Multilayer Fresnel coefficients

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multilayer(wavelength = 2 * pi/k0, k0 = 2 * pi/wavelength,
  angle = asin(q), q = sin(angle), epsilon = list(incident = 1.5^2, 1.33),
  thickness = c(0, 0), polarisation = c("p", "s"), d = 1, dout = d, ...)

`wavelength`	[vector] wavelength in nm
`k0`	[vector] wavevector in nm^-1
`angle`	[vector] incident angles in radians
`q`	[vector] normalised incident in-plane wavevector
`epsilon`	list of N+2 dielectric functions, each of length 1 or length(wavelength)
`thickness`	vector of N+2 layer thicknesses, first and last are dummy
`polarisation`	[character] switch between p- and s- polarisation
`d`	vector of distances where LFIEF are evaluated from each interface
`dout`	vector of distances where LFIEF are evaluated outside the stack
`...`	unused

solves the EM problem of a multilayered interface

fresnel coefficients and field profiles

baptiste Auguie

Principles of surface-enhanced Raman spectroscopy and related plasmonic effects. Eric C. Le Ru and Pablo G. Etchegoin, published by Elsevier, Amsterdam (2009).

planar documentation built on May 2, 2019, 3:23 a.m.