Abstract

Electromagnetic (EM) evanescent waves generated on material surfaces without external illumination are of particular interest. If materials are in thermal equilibrium, thermal fluctuation of current and/or charge is induced by stochastic thermal motion of conduction electrons (in metals) or by thermally-activated lattice vibrations (in polar dielectrics), which generates intense thermal EM evanescent waves [1]. If materials are driven out of equilibrium, say, by electric-field-induced currents or by chemical reactions, even stronger EM evanescent waves are induced because the fluctuation of current and/or charge is promoted by activated motion of charge carriers or electric dipoles in non-equilibrium states. Hence, a sensitive passive microscopy of EM evanescent waves with nanometer resolution is expected to provide us with a unique and powerful probe to the local kinetics of material phenomena in equilibrium and non-equilibrium conditions. We have developed such microscopes as described in the above, by incorporating ultra-highly sensitive detectors, called CSIP [2], into passive terahertz (THz) scattering-type scanning near-field optical microscopes (s-SNOMs) [3]. Owing to the high sensitivity, detailed nature of the thermal EM evanescent waves has been clarified through quantitative analysis of imaging of both metals [4, 5] and dielectrics. The spatial resolution reaches a value about 20nm (λ/750) [6]. We also demonstrate the potentiality and powerfulness of our system for probing non-equilibrium kinetics: We show that current-induced hot-electron distribution in narrow metal wires at room temperature is clearly visualized with nanometer resolution. These results show that our systems will find broad application areas in the near future.

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