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

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98 CHAPTER 6. COMPOSITE MEDIA BASED ON AU/LIF ARRAYS3025Number [%]201510540 nma. b.01020Diameter [nm]3040 50Figure 6.1: Left panel: transmission electron microscopy image (courtesy <strong>of</strong> ICMM) <strong>of</strong>Fe 3 O 4 nanoparticles obtained by decomposition <strong>of</strong> an iron oleate complex in 1-octadecen<strong>and</strong> oleic acid (see text for details). Right panel: distribution <strong>of</strong> the particles hydrodynamicsize obtained from dynamic light scattering analysis on a colloidal suspension <strong>of</strong>Fe 3 O 4 /AO particles dispersed in hexane.Thetemplateforthedeposition<strong>of</strong>theFe 3 O 4 /OAnanoparticleswaspreparedaccordingto the procedure described in the previous chapters. First, a nanopatterned LiF(110)substrate was grown following the homoepitaxial deposition <strong>of</strong> t LiF ≈ 250 nm LiF atT = 300 ◦ C, which induced the formation <strong>of</strong> a well-developed ripple structure with amean periodicity Λ ≈ 35 nm; an AFM image <strong>of</strong> the surface is shown in fig. 6.2(a). Then,the 2D array <strong>of</strong> gold nanoparticles was obtained by grazing deposition <strong>of</strong> t Au ≈ 5 nmgold at T = 100 ◦ C <strong>and</strong> subsequent annealing at T = 400 ◦ C. We report in fig. 6.2(b)a representative AFM image <strong>of</strong> the array, where we can distinguish parallel chains <strong>of</strong>slightly elongated nanoparticles, oriented along the LiF ridges, <strong>and</strong> with mean in-planesemi-axes <strong>of</strong> a x ≈ 11 nm <strong>and</strong> a y ≈ 14 nm, respectively across <strong>and</strong> parallel the ripples.The corresponding Fourier spectrum, shown in the inset <strong>of</strong> the figure, confirms the orderedarrangement <strong>of</strong> the particles: the sharp intensity peak confined in the [1¯10] direction, <strong>and</strong>rapidly decaying in the [001] direction, shows that the periodicity <strong>of</strong> the underlying ripplestructure has been preserved within the Au NPs array, while the broader feature slowingdecaying in all directions, <strong>and</strong> slightly stretched in the [1¯10] direction, reflects the in-planeanisotropic shape <strong>of</strong> the particles.The deposition <strong>of</strong> the Fe 3 O 4 /OA NPs has been performed by immersing the Au/LiFsubstrate in a colloidal suspension <strong>of</strong> NPs dispersed in hexane with a concentration <strong>of</strong>≈ 6μg Fe per ml, for a period <strong>of</strong> time <strong>of</strong> about 5 minutes; then, the sample has beenwashed in pure hexane, in order to remove the particles weakly stuck to the surface,<strong>and</strong> dried under nitrogen flux. An AFM image measured after the deposition <strong>of</strong> themagnetic NPs is reported in fig. 6.2(c). The surface appears uniformly covered withFe 3 O 4 /OA nanoparticles, <strong>and</strong> no Au particle could be apparently singled out. From thesole inspection <strong>of</strong> the AFM image we cannot determine the exact thickness <strong>of</strong> the magneticNP layer. However earlier depositions on silicon substrates (not reported here) showedthat the Fe 3 O 4 /OA particles did not form more than a monolayer even after prolongedimmersions <strong>of</strong> several hours in solution; we can therefore expect that also in this case asingle monolayer <strong>of</strong> magnetic nanoparticles was deposited.

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