Abstract
In a seminal paper, published over half a century ago, R.H. Ritchie [1] used Bloch’s hydrodynamic model (HDM) of an electron gas (EG) [2] to describe collective, or plasma excitations by fast electrons in thin metallic films. Ever since, this model played an important role as a phenomenological approach, which often gave qualitatively correct and physically transparent results for many interesting surface and bulk phenomena [3, 4, 5, 6, 7, 8, 9, 10, 11]. With the advent of nanotechnology, interest in plasmon excitations at the surfaces of nano-particles and at the metal-dielectric interfaces grew over the past few years at an unexpectedly fast rate, forming an entirely new research area named Plasmonics [12, 13]. Even in these modern developments where surface plasmon excitations are studied by means of the currently most sophisticated ab initio methods, such as Time-Dependent Density Functional Theory (TD-DFT) [14, 15, 16], the HDM continues to play an important role owing to its versatility in handling the often complex geometry and heterogeneous composition of nano-structures [15].
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Acknowledgments
The authors are grateful to all their collaborators who, over the years, have contributed to the results presented in this review.
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Villo-Perez, I., Mišković, Z., Arista, N. (2010). Plasmon Spectra of Nano-Structures: A Hydrodynamic Model. In: Bârsan, V., Aldea, A. (eds) Trends in Nanophysics. Engineering Materials. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-12070-1_10
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