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Using interference in the frequency domain for precise determination of thickness and refractive indices of normal dispersive materials
96
Citations
16
References
1995
Year
Optical SignaturesOptical MaterialsEngineeringWave OpticNegative-index MetamaterialInterferometryMetamaterialsOptical MetrologyFiber OpticsDispersionOptical CharacterizationElectromagnetic MetamaterialsSurface ReflectanceOptical PropertiesPhotonic MetrologySpectral Interference LawComputational ElectromagneticsOptical SystemsReflectanceSpectral Interference PhenomenonNanophotonicsMaterials SciencePhotonicsPhysicsClassical OpticsTime MetrologyOptical MeasurementFrequency DomainNormal Dispersive MaterialsSpectroscopyApplied PhysicsRefractive IndicesMichelson Interferometer ConfigurationOptical System AnalysisWave InterferenceDiffractive Optic
Introducing a dispersive medium into one arm of a Michelson interferometer alters the spectral interference pattern, producing a zero‑order fringe at the wavelength where the net path difference vanishes. The study demonstrates spectral interference with a broadband white‑light source and theoretically analyzes the interference law for amplitude‑division interferometers, aiming to relate medium thickness to the zero‑order fringe width. Using a Michelson interferometer with a white‑light source, the authors measure spectral interference and apply a theoretical model of amplitude‑division interferometers to extract thickness from the zero‑order fringe. Experimental data across the visible spectrum yielded the refractive index n(λ) and thickness t of the dispersive medium with an accuracy of ~10⁻⁵.
We present an experimental demonstration of the spectral interference phenomenon, using a spectrally broad white-light source in a Michelson interferometer configuration. We also present a theoretical analysis of the spectral interference law for the general case of amplitude-division interferometers. When a dispersive medium is introduced into one of the arms of the interferometer, the spectral interference pattern changes drastically, with a change in the frequency modulation corresponding to the dispersive nature of the medium. A zero-order fringe appears at a wavelength where the net path difference between the two arms of the interferometer is zero. We relate the thickness of the dispersive medium to the width of the zero-order fringe. From the experimental data over the entire visible region of the spectrum we obtain the refractive index n(λ) and the thickness t of the dispersive medium, calculated to an accuracy of the order of 10−5.
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