AVS 61st International Symposium & Exhibition | |
Nanometer-scale Science and Technology | Monday Sessions |
Session NS+EN-MoA |
Session: | Nanophotonics and Plasmonics |
Presenter: | Timo Lichtenstein, Leibniz Universität Hannover, Germany |
Authors: | T. Lichtenstein, Leibniz Universität Hannover, Germany U. Krieg, Leibniz Universität Hannover, Germany C. Tegenkamp, Leibniz Universität Hannover, Germany H. Pfnür, Leibniz Universität Hannover, Germany |
Correspondent: | Click to Email |
An efficient way to transfer energy, e.g. light, into an electronic system is by excitation of plasmons. Due to their flat and almost linear dispersion, allowing extreme confinement in a broad frequence range, and their natural function as wave guides 1D plasmons are particularly interesting.
As we show here for the system Ag adsorbed on Si(557), the interaction between adsorbate layers of transition metal atoms and strongly anisotropic surfaces can lead to various quasi-one-dimensional (1D) signatures, which, however, are not all necessarily metallic. Using low energy electron diffraction in combination with scanning tunneling microscopy and electron energy loss spectroscopy, we correlate the structure, determined by SPALEED and STM, with the properties of low dimensional collective excitations, as measured with momentum and energy resolving electron loss spectroscopy. Semiconducting structures with double periodicity along the chains are formed Ag coverages below 0.3 monolayers (ML). At higher coverages, the formation of wires with (√3x√3) order sets in. Only these wires turn out to be metallic, as is evident from the appearance of plasmonic losses, which show 1D dispersion only along the wires. This 1D property even persists up to one monolayer, where a densely packed arrayof metallic (√3x√3) stripes is formed. We show evidence that the metallic property is induced by an extrinsic doping process of excess Ag (or other) atoms localized at the step edges, which can be reversibly removed and added. With this system we were able to explicitly show that the 1D plasmon frequency depends on the electron density proportional to √ne also in the 1D case, and that the confinement of the electrons on the wires is also dependent on doping concentration.