Uniaxial crystal “ordinary index” no nx n y “extraordinary index” ne nz Call the unique direction z: “optic axis” Ordinary wave or ray: Any wave with polarization E to the optic axis (OA). The wave travels with index no. Extraordinary wave or ray: Any wave with E component along OA! (polarization in the k-OA plane) The wave travels with index between no and ne, which we call the function ne(q). Angle q between k and OA General case: 2k’s, 2S’s OA 2 x u y2 u z2 1 2 2 2 2 2 2 2 n n no n no n ne u becomes ne (q ) no ne no2 sin 2 q ne2 cos 2 q Crystals may be cut at any angle vs. the optic axis! k q Optic axis ne>no no>ne Don’t confuse s,p polarization with o,e polarization! No direct connection For this cut of crystal and k vector shown, an e-wave is the ____ a) s-polarization b) p-polarization c) both s,p are e-waves d) neither s,p are e-waves OA For this cut of crystal and k vector shown, an e-wave is the ____ a) s-polarization b) p-polarization c) both s,p are e-waves d) neither s,p are e-waves OA Finding E, S directions for the extraordinary wave Text gives equations for directions of S, E for ONLY the case in this picture: OA the interface…. so these equations aren’t very important… OA Finding E, B, S directions for the extraordinary wave x z Px x P y o 0 P 0 z k o E P 0 0 y 0 0 Ex 0 E y z Ez Gives ratios of E components Bo k Eo S E B o What is to what? E EE E P o OA S k Polarizing prisms Good for high powered lasers. (no heating from absorption) Cut and rejoin, with OA perhaps oriented differently. Polarizing prisms from uniaxial crystals In prism d, which exiting beam was the e-ray in the material it left? a) top b) bottom Polarizing prisms In prism a, the the beams are separated by TIR ___ So in this material which index is greater? a) n-e b) n-o Polarizing prisms In prism b, the beams (k’s) are separated by Snell’s law. Imagine the k-vectors are shown. So in this material which index is greater? a) n-e b) n-o