1956
DOI: 10.1063/1.3059910
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Optical Properties of Thin Solid Films

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Cited by 324 publications
(120 citation statements)
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“…The amplitude of the reflected beam is a result of interference between all the optical paths and is determined by the wavelength of the incident light ( ), their incident angles ( ), refractive indices of all layers (n), and their thicknesses (h). Thus, the total reflectivity of light from the triple-layer system can be described by 16 …”
Section: Resultsmentioning
confidence: 99%
“…The amplitude of the reflected beam is a result of interference between all the optical paths and is determined by the wavelength of the incident light ( ), their incident angles ( ), refractive indices of all layers (n), and their thicknesses (h). Thus, the total reflectivity of light from the triple-layer system can be described by 16 …”
Section: Resultsmentioning
confidence: 99%
“…The oxide is transparent in the visible spectrum and so most of the re¯ection of incident light comes from the metal surface. Since the di erence in index of refraction of the metal±gas interface is higher than that of the metal±oxide interface [3], the metal surface under debonded oxide appears brighter than the same surface in contact with the oxide. An additional observation made was that the debonded regions of the scale form during cooling within a few minutes after removing a specimen from the furnace.…”
Section: Observations Of Scale Separationmentioning
confidence: 99%
“…This maximum is reached at h ∼ λ/n eff , where n eff is the effective refractive index of the film. In this maximum, an analytical solution of the Maxwell equations yields the following expression for the reflectance 44 ,…”
Section: A Enhancement Of Reflection Of the Optical Pulsementioning
confidence: 99%