knitr::read_demo("dipole_integrand", package="planar")

A dipole near a thin silver film can excite SPPs (on either side of the film, if sufficiently thin), resulting in a strong increase of the total decay rate. The calculation of Mtot requires an integral over the full spectrum of plane waves -- propagating (q<1) and evanescent (q>1). Here we visualise the integrand as a function of wavelength and q.



At very large q, the system is well-described by quasi-static image dipole interaction with a slow decay. This results in a time-consuming integration for Mtot, unless special care is taken to transform the integrand; in dipole(), the following transformation is used, $$\int_a^\infty f(x)dx = \int_0^1 f(a + t/(1-t)). 1 / (1-t)^2 dt$$



plasmonics/planar documentation built on Feb. 10, 2022, 5:55 a.m.