Surface Plasmon Polaritons (SPPs) - Introduction and basic properties

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ω T = 0 Aluminium ω L = ω P
Free <strong>and</strong> bound electrons in metals ε bound ε drude Bound electrons contribute like a Lorenz oscillator where ε = ε + ε ε metal drude drude 2 ω p, d 1− ω − iγ ω = 2 d bound 2 ω p, j ∑ 2 ω −ω − iγ ω ε bound = 2 j 0 j
Page 1 and 2: Surface Plasmon Polaritons (SPPs) -
Page 3 and 4: • free electrons in metal are tre
Page 5 and 6: Optical technology using - propagat
Page 7 and 8: Subwavelength-scale plasmon wavegui
Page 9 and 10: Literature: Light-matter interactio
Page 11 and 12: EM-waves in matter (linear media) -
Page 13 and 14: One-oscillator (Lorentz) model from
Page 15 and 16: Optical properties of polar crystal
Page 17 and 18: General dispersion for nonconductor
Page 19: - Intraband transitions - longitudi
Page 23 and 24: Dielectric function of metals and p
Page 25 and 26: z x Surface polaritons (SPs) Couple
Page 27 and 28: z z x x Derivation of SPP dispersio
Page 29 and 30: x-component: Metal Diel. I: II: I /
Page 31 and 32: E k k k 2 x 2 zd 2 zm SP 2 ⎛ ω
Page 33 and 34: ω p ω Plasmon polaritons: photon
Page 35 and 36: z x dielectric () ε d ω metal ()
Page 37 and 38: ω photon in air Dispersion and exc
Page 39 and 40: E ε d ε m ε 0 θ0 k x R z Excita
Page 41 and 42: z ε d ε m ε 0 x k c ω = k = ω

Surface Plasmon Polaritons (SPPs) - Introduction and basic properties

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