2022
DOI: 10.1016/j.apsusc.2021.151885
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Influence of roughness, porosity and grain morphology on the optical properties of ultrathin Ag films

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Cited by 14 publications
(8 citation statements)
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“…In the reflection and transmission spectra acquired in the 280–1900 nm wavelength range (Figure a,b, respectively), the ITO/glass substrate shows an oscillating behavior due to interference fringes arising from multiple internal reflections inside the ITO coating. By modeling the substrate as a two-layer system with a 1 mm-thick BK7 glass (with a fixed refractive index from Rosete-Aguilar et al) and a 130 ±5 nm-thick ITO coating layer, the ITO dielectric function was obtained by fitting the experimental data through the DEMON code . The set of oscillators identifying the ITO dielectric function and reported in the Supporting Information (Section S3) was obtained by fitting the ITO/glass experimental R and T data.…”
Section: Resultsmentioning
confidence: 99%
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“…In the reflection and transmission spectra acquired in the 280–1900 nm wavelength range (Figure a,b, respectively), the ITO/glass substrate shows an oscillating behavior due to interference fringes arising from multiple internal reflections inside the ITO coating. By modeling the substrate as a two-layer system with a 1 mm-thick BK7 glass (with a fixed refractive index from Rosete-Aguilar et al) and a 130 ±5 nm-thick ITO coating layer, the ITO dielectric function was obtained by fitting the experimental data through the DEMON code . The set of oscillators identifying the ITO dielectric function and reported in the Supporting Information (Section S3) was obtained by fitting the ITO/glass experimental R and T data.…”
Section: Resultsmentioning
confidence: 99%
“…Reflection ( R ) and transmission ( T ) spectra have been acquired at normal incidence by a Perkin-Elmer Lambda 950 Spectrometer in the 250–1900 nm range. The optical spectra have been modeled and fitted through the home-made DEMON software by employing a multilayer model with each layer dielectric function being described by Bruggeman’s effective medium approximation (BEMA). The quantity false( R exp R model false) 2 + false( T exp T model false) 2 was minimized to refine the parameters in the multilayer model.…”
Section: Methodsmentioning
confidence: 99%
“…Consequently, once the gold layer is initiated, the optical and thermal properties change to a composite structure where the growing gold layer is optically in series with the AuC x core material relative to the laser flux and is thermally in parallel relative to the substrate heat sink. While a concentric bi-layer model using gold surrounding an AuC x core was explored, the optical absorption below ~50 nm is very sensitive to the surface roughness [ 52 ], which significantly enhances the optical absorption. Using standard gold properties has the effect of significantly reducing the structure temperature below the decomposition temperature, primarily due to significant reflectance but also due to enhanced thermal conduction (see SI-3 for an example and model details).…”
Section: Resultsmentioning
confidence: 99%
“…31,32 The properties of Ag thin films generally depend on thickness. 33 Increasing the film thickness induces a rougher surface structure than that of thinner films, and rough surfaces cause optical loss from the scattering of light. Therefore, thin silver films are expected to improve the photoresponse of photodetectors.…”
Section: Introductionmentioning
confidence: 99%
“…However, gold is an expensive material, and copper is easily oxidized in the atmosphere. Therefore, among these materials, silver thin films are appropriate for electrodes in optoelectronics and are widely used. , The properties of Ag thin films generally depend on thickness . Increasing the film thickness induces a rougher surface structure than that of thinner films, and rough surfaces cause optical loss from the scattering of light.…”
Section: Introductionmentioning
confidence: 99%