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Research Article

Depolarization effects in tip‐enhanced Raman spectroscopy

A. Merlen

Corresponding Author

E-mail address:merlen@univ.tln.fr

Université du Sud Toulon Var, IM2NP, Bâtiment R, BP 20132, F83957 La Garde Cedex, France

CNRS, IM2NP (UMR 6242) France

Université du Sud Toulon Var, IM2NP, Bâtiment R, BP 20132, F83957 La Garde Cedex, France.
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J. C. Valmalette

Université du Sud Toulon Var, IM2NP, Bâtiment R, BP 20132, F83957 La Garde Cedex, France

CNRS, IM2NP (UMR 6242) France

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P. G. Gucciardi

CNR Istituto per i Processi ChimicoFisici, sez. Messina, Salita Sperone Contrada Papardo, I98158 Messina, Italy

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M. Lamy de la Chapelle

Laboratoire de Chimie, Structure et Propriétés des Biomatériaux et d'Agents Thérapeutiques, UFR SMBH, Université Paris 13, 74 rue Marcel Cachin, 93017 Bobigny, France

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A. Frigout

LPICM, Ecole Polytechnique, CNRS, 91128 Palaiseau, France

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R. Ossikovski

LPICM, Ecole Polytechnique, CNRS, 91128 Palaiseau, France

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First published: 21 September 2009
Cited by: 25

Abstract

Tip‐enhanced Raman spectroscopy has proven to be a promising technique for stress/strain mapping of silicon‐based semiconductor devices on the nanometer scale. Field enhancement factors of up to 104 have been reported and a spatial resolution down to 20 nm has been claimed through exploiting far‐field suppression techniques based on an appropriate choice of the excitation/detection polarization states. In this paper, we show that depolarization of light due to scattering from the tip plays a key role in the selective enhancement of the one‐phonon optical mode peak at 520 cm−1 with respect to the two‐phonon ones. The spatial confinement of the selective enhancement has been studied by means of approach curves, and its dependence on the excitation wavelength and power further explored. Conclusions on the physical nature of the enhancement (depolarization‐ or plasmonic‐based) are presented. Copyright © 2009 John Wiley & Sons, Ltd.

Number of times cited: 25

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