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book of abstracts - IM2NP

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A B S T R A C T S TUESDAY, JUNE 29 N A N O S E A 2 0 1 0<br />

Room Calendal<br />

8H30-9h10<br />

IR and THz near-field nanoscopy for characterizing nanoscale materials and<br />

devices<br />

Rainer Hillenbrand (Nanooptics Group, CIC nanoGUNE, 20018 Donostia - San Sebastian, Spain)<br />

r.hillenbrand@nanogune.eu<br />

The development <strong>of</strong> novel nanoscale materials, composites and devices requires ultrahigh-resolution<br />

microscopy tools for characterization and mapping <strong>of</strong> local material properties and nanoscale confined light<br />

fields. In this talk, I will demonstrate a near-field optical microscopy technique providing a spatial resolution<br />

<strong>of</strong> about 10-20 nm independent <strong>of</strong> the wavelength. It is based on elastic light scattering from the probing tip<br />

<strong>of</strong> an atomic force microscope (scattering-type near-field optical microscopy, s-SNOM [1]). Besides an<br />

introduction <strong>of</strong> the technique, I will demonstrate some s-SNOM applications including infrared and terahertz<br />

mapping <strong>of</strong> chemical composition, free-carrier concentration in semiconductor nanodevices [2], strain fields<br />

and nanocracks in ceramics [3], as well as the visualization <strong>of</strong> the near-field oscillations <strong>of</strong> optical and midinfrared<br />

plasmonic nanoantennas [4].<br />

[1] F. Keilmann and R. Hillenbrand, Philos. Trans. R. Soc. London, Ser. A 362, 739 (2004)<br />

[2] A. Huber, et al., Nano Lett. 8, 3766 (2008)<br />

[3] A. Huber, et al., Nature Nanotech. 4, 153 (2009)<br />

[4] M. Schnell, et al., Nature Photon. 3, 287 (2009)<br />

9H10-9H30<br />

The Suzuki surface as a template for nano-objects: An atomic force microscopy<br />

study.<br />

C. Barth, R. Peresutti, M. Gingras and C. R. Henry (CINaM - CNRS, Campus de Luminy, Case<br />

913, 13288 Marseille Cedex 09) barth@cinam.univ-mrs.fr<br />

In 1961, Kazuo Suzuki found out by X-ray diffraction experiments that a new phase is created in NaCl<br />

crystals if the crystals are doped with divalent impurity ions (e.g., with Cd2+ or Mg2+) [1]. In this so-called<br />

Suzuki phase, the positive divalent impurities and sodium vacancies are arranged in an highly ordered atomic<br />

lattice, which is twice as large as the one <strong>of</strong> pure NaCl. In real crystals, the Suzuki phase can be found in<br />

cubic precipitates, which are embedded in the NaCl matrix. Thanks to recent noncontact AFM experiments,<br />

the surfaces <strong>of</strong> Suzuki precipitates on NaCl(001) could be precisely characterized in ultrahigh vacuum [2-4].<br />

Basically two types <strong>of</strong> surface regions exist on NaCl:Cd2+(001) [2]: surface regions <strong>of</strong> pure NaCl and<br />

regions <strong>of</strong> Suzuki precipitates, which cover partially the (001) surface <strong>of</strong> the crystal. It has been shown by<br />

atomic resolution imaging, that the precipitates are indeed embedded in the NaCl matrix and that both types<br />

<strong>of</strong> surface regions are atomically flat [3]. Each ionic species in the atomic<br />

Suzuki structure can be unambiguously identified by just imaging [3, 4]. Kelvin probe force microscopy has<br />

further shown, that the precipitates carry a net negative surface charge, which is due to the negative sodium<br />

vacancies [3].<br />

Despite many attractive properties <strong>of</strong> Suzuki surfaces like the interesting nano-structuring at the nanometer<br />

scale and the presence <strong>of</strong> negative cation vacancies on the surface, Suzuki surfaces have not yet been used as<br />

a substrate surface for nano-objects like molecules or metal clusters. In this contribution the Suzuki surface<br />

36

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