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Morphology and plasmonic properties of self-organized arrays of ...

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Chapter 4Self-<strong>organized</strong> nanoparticle<strong>arrays</strong>: optical <strong>properties</strong>In this chapter, we present the optical characterizations <strong>of</strong> the specimens during all thesteps <strong>of</strong> the fabrications, from the bare LiF substrates to the 2D <strong>arrays</strong> <strong>of</strong> gold nanoparticles.4.1 Optical <strong>properties</strong> <strong>of</strong> Lithium Fluoride substratesIn this section we will focus on the characterization <strong>of</strong> the optical <strong>properties</strong> <strong>of</strong> the LiFsubstrates. As will become more clear in the next chapter, they will play an importantrole for the modelling <strong>of</strong> the optical response <strong>of</strong> the gold NP.Lithium fluoride is a well-known material for dosimetry <strong>and</strong> optoelectronics. It hasa very wide b<strong>and</strong> gap <strong>of</strong> 13.6 eV, so in the visible <strong>and</strong> near-IR range it behaves like atransparent, non absorbing material (transmittance higher than 90% in the range 0.1 ÷7μm[194, 195]). Its optical characteristics have been extensively investigated mainly inconnection with its color centers [196–199]. These, usually induced by oxygen <strong>and</strong> metalions impurities, introduce weak absorptions in the 200-350 nm region [200, 201], conferringthe crystal a characteristic yellowish color.Transmittance0.950.90 [deg]8.07.57.0182181 [deg]0.856.5180123E [eV]45123E [eV]45Figure 4.1: Panel a: transmission spectrum measured at normal incidence on a doublesidepolished LiF(110) sample in the as received state. Panel b: Ψ (red curve) <strong>and</strong> ∆(black curve) spectra measured on a single-side polished LiF(110), at incidence θ = 50 ◦ .61

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