Presentation on theme: "Guided Waves in Layered Media. Layered media can support confined electromagnetic propagation. These modes of propagation are the so-called guided waves,"— Presentation transcript:
Layered media can support confined electromagnetic propagation. These modes of propagation are the so-called guided waves, and the structures that support guided waves are called waveguides.
Symmetric Slab Waveguides Dielectric slabs are the simplest optical waveguides. It consists of a thin dielectric layer sandwiched between two semi-infinite bounding media. The index of refraction of the guiding layer must be greater than those of the surround media.
Symmetric Slab Waveguides The following equation describes the index profile of a symmetric dielectric waveguide:
Symmetric Slab Waveguides The propagation of monochromatic radiation along the z axis. Maxwell’s equation can be written in the form
Symmetric Slab Waveguides For layered dielectric structures that consist of homogeneous and isotropic materials, the wave equation is The subscript m is the mode number
Symmetric Slab Waveguides For confined modes, the field amplitude must fall off exponentially outside the waveguide. Consequently, the quantity (nω/c)^2-β^2 must be negative for |x| > d/2.
Symmetric Slab Waveguides For confined modes, the field amplitude must fall off sinusoidally inside the waveguide. Consequently, the quantity (nω/c)^2-β^2 must be positive for |x| < d/2.
Guided TE Modes The electric field amplitude of the guided TE modes can be written in the form
Guided TE Modes The solutions of TE modes may be divided into two classes: for the first class and for the second class The solution in the first class have symmetric wavefunctions, whereas those of the second class have antisymmetric wavefunctions.
Guided TE Modes The propagation constants of the TE modes can be found from a numerical or graphical solution.
Surface Plasmons Confined propagation of electromagnetic radiation can also exist at the interface between two semi- infinite dielectric homogeneous media. Such electromagnetic surface waves can exist at the interface between two media, provided the dielectric constants of the media are opposite in sign. Only a single TM mode exist at a given frequency.
Surface Plasmons A typical example is the interface between air and silver where n1^2 = 1 and n3^2 = -16.40- i0.54 at λ = 6328( 艾 ).
Surface Plasmons For TE modes, by putting t=0 in Eq.(11.2-5), we obtain the mode condition for the TE surface waves, p + q =0 Where p and q are the exponential attenuation constants in media 3 and 1. It can never be satisfied since a confined mode requires p>0 and q>0.
Surface Plasmons For TM waves, the mode funcion H y (x) can be written as The mode condition can be obtained by insisting on the continuity of E z at the interface x = 0 of from Eq.(11.2-11)
Surface Plasmons The propagation constant β is given by A confined propagation mode must have a real propagation constant, since <0,
Surface Plasmons The attenuation constants p and q are given
Surface Plasmons The electric field components are given
Surface Plasmons Surface wave propagation at the interface between a metal and a dielectric medium suffers ohmic losses. The propagation therefore attenuates in the z direction. This corresponding to a complex propagation constants β Where α is the power attenuation coefficient.
Surface Plasmons In the case of a dielectric-metal interface, is a real positive number and is a complex number (n – iκ)^2, and the propagation constant of the surface wave is given
Surface Plasmons In terms of the dielectric constants The propagation and attenuation constants can be written as
Surface Plasmons The attenuation coefficient can also be obtained from the ohmic loss calculation and can be written as σ is the conductivity