Optics of a single Homogeneous and Isotropic Layer

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Presentation transcript:

Optics of a single Homogeneous and Isotropic Layer

Electromagnetic Treatment For the homogeneous and isotropic media, the whole structure can be described by

Electromagnetic Treatment We assume that a plane wave is incident from the left, the electric field vector can be written as

Electromagnetic Treatment For s wave, the electric field E(x) is Ey, and Hz can be obtained by Maxwell equations.

Electromagnetic Treatment Imposing the continuity of Ex and Hy at the interface x=0 and x=d leads to

Electromagnetic Treatment The Fresnel reflection and transmission coefficients of the dielectric interfaces for s waves as

Electromagnetic Treatment The transmission and reflection coefficients can be written as where

Electromagnetic Treatment A similar electromagnetic analysis for the p wave leads to exactly the same expressions for the transmission and reflection coefficients.

Airy’s Formulations The transmission and reflection coefficients can also be derived by summing the amplitudes of successive reflection and refractions.

Airy’s Formulations

Airy’s Formulations

Airy’s Formulations Substituting φ+π for φ in above expressions, we obtain

Airy’s Formulations In the limit when the thickness of the layer becomes zero, the reflection and transmission coefficients should become those of the interface between media 1 and 3.

Airy’s Formulations The presence of a half-wave layer with φ=π does not affect the reflection and transmission of light except for a possible change of sign.

An Alternative Derivation At the interface x=0, these are two incoming waves and two outgoing waves. The amplitudes of these waves are related by

An Alternative Derivation At the interface x=d, these is only one incoming wave and two outgoing waves. The amplitudes of these waves are related by

An Alternative Derivation By eliminating A, C, and D, we obtain

Transmittance, Reflectance, and Absorptance Reflectance is defined as the fraction of energy reflected from the dielectric structure and is given by Reflectance is meaningful only when medium 1 is nonabsorbing. If medium 3 is also nonabsorbing, the transmittance is given by The factor corrects for the difference in phase velocity.

Transmittance, Reflectance, and Absorptance Absorptance, which is defined as the fraction of energy dissipated, is given by A = 1 - R - T

A Thin Film on a Substrate