1997
DOI: 10.1051/mmm:1997113
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Low-Loss EELS Study of Oxide-Covered Aluminum Nanospheres

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1998
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Cited by 14 publications
(6 citation statements)
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References 17 publications
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“…Comparing the ϩ plasmon resonance energy close to the center of different size particles it can be noticed that the resonance is shifted to lower energies as the spheres become smaller. This is in contradiction to what is observed in the case of small metallic particles [48][49][50] where the volume plasmon resonance energy has tendency to rise to higher values. In the case of metallic particles, this blueshift is ascribed to the effect of dispersion in a finite medium.…”
Section: B Size Dependence and Particular Featurescontrasting
confidence: 99%
“…Comparing the ϩ plasmon resonance energy close to the center of different size particles it can be noticed that the resonance is shifted to lower energies as the spheres become smaller. This is in contradiction to what is observed in the case of small metallic particles [48][49][50] where the volume plasmon resonance energy has tendency to rise to higher values. In the case of metallic particles, this blueshift is ascribed to the effect of dispersion in a finite medium.…”
Section: B Size Dependence and Particular Featurescontrasting
confidence: 99%
“…Models developed within the frame of classical dielectric response theory 34 have been used with success to interpret plasmon losses in electron energy loss spectroscopy. Such models predict correctly the resonance energies and the intensities of the surface and volume plasmon excitations for different geometries such as thin slabs, 35 spheres, [36][37][38][39] layered spheres, 38,40,41 spheres halfway embedded in a supporting medium, 42,43 and cylindrical channels [44][45][46][47] and explain size-dependent variations of the peak position. The electronic properties of the material composing the nanoparticle are taken into account via its frequency-dependent dielectric function.…”
Section: Introductionmentioning
confidence: 99%
“…A shift to lower energy is expected at the interface with an oxide, as observed at planar interfaces 8,9 as well as nanostructure-oxide interfaces. [10][11][12] The condition for resonance at planar interfaces between two materials A and B is 1A ()ϩ 1B ()ϭ0. 1 While the dielectric functions for the bismuth nanowires and templates have not been determined, 5.5 eV is a reasonable energy to expect for an interface plasmon based on the bismuth 21 and alumina 22 bulk values.…”
Section: Resultsmentioning
confidence: 99%
“…Studies of plasmons at planar interfaces and at nanoparticle interfaces have been used to assess interfacial chemistry and properties. [8][9][10][11][12] By coupling an EELS spectrometer with the powerful imaging capabilities of the TEM, it is also possible to select those electrons that have undergone a specific loss event during their transit through the sample and display the spatial variation of that loss event in an image. Such ''energy-filtered imaging'' of the plasmon excitations can be used to identify those regions of the sample that sustain a plasmon mode.…”
Section: Introductionmentioning
confidence: 99%