Chapter 2 three-layer dielectric slab waveguides Slab waveguides simple geometric and basic structure analytic solution of guided modes and radiation modes TE and TM modes Ray optics begin by considering reflection and refraction at a plane dielectric interface then derivation eigenvalue equation Electromagnetic field theory identical eigenvalue equation, mode fields, mode numbers and cut-off condition etc Real index complex index Three-layer---multiple layer 2010-3-20 1 § Reflection and refraction at a plane dielectric interface § Snell’s laws § Fresnel’s laws § Normal incidence § Brewster angle § Critical angle § Phase shift on total internal reflection § Goos-Haenchen shift(古斯汉欣位移) § Summery and numerical example 2010-3-20 2 Reflection and refraction at a plane dielectric interface 3: reflected light x 1: incident light θ θ 3 1 n1 z −i(ω t −⋅ nk r) θ2 n2 Ee∝ 2: refracted light Figure −iwt () Incident wave: Ei = E1 eexp[ ikn( −+ x cosθθ z sin) ] 1 11 −iwt () Reflected wave: Er = E3 eexp[ ikn( x cosθθ+ z sin) ] 13 3 Refracted wave: −iwt () Et = E2 eexp[ ikn2( −+ x cosθθ 22 z sin) ] 2010-3-20 3 § Reflection and refraction § Snell’s laws (1)Description of Snell’s laws (2)Two mediums (3)Derivation of Snell’s laws --- ray optics (4) Derivatio
2 reflection and refraction at a plane英文 来自淘豆网www.taodocs.com转载请标明出处.