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Optical super‐resolution using higher harmonics and different acquisition modes in an aperture tapping SNOM
Author(s) -
Longo Giovanni,
Girasole Marco,
Pompeo Giuliano,
Cricenti Antonio
Publication year - 2010
Publication title -
physica status solidi (b)
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.51
H-Index - 109
eISSN - 1521-3951
pISSN - 0370-1972
DOI - 10.1002/pssb.200983934
Subject(s) - optics , signal (programming language) , modulation (music) , near field scanning optical microscope , harmonics , materials science , noise (video) , laser , wavelength , oscillation (cell signaling) , optical microscope , physics , acoustics , computer science , quantum mechanics , image (mathematics) , programming language , biology , genetics , scanning electron microscope , voltage , artificial intelligence
Scanning near field optical microscopy (SNOM) is a well‐established technique to obtain a sub‐wavelength resolution optical characterization, together with nanometer‐scale topography images, on any kind of biological or non‐biological sample. Recently we have modified a classical SNOM unit to work in the tapping modality, ensuring stability, versatility and good optical resolution and signal to noise ratio. Exploiting the vertical tip movement, in particular, we were able to access two different optical detection modes: light modulation, which can be obtained by a mechanical chopper or by electronically switching the laser on and off; gap modulation in which the tip's vertical oscillation is used to produce, itself, a modulation of the collected light. Several biological and non‐biological samples have been investigated and the data reveal that, despite the signal collected in gap‐modulation is at least one order of magnitude smaller than in laser‐modulation, resolution, and signal‐to‐noise ratio in the gap‐modulated images is preferable. On the other hand, the higher intensity of the laser‐modulation signal allows to deconvolve the optical information at higher harmonics of the tip oscillation frequency. This is a well‐known procedure used in the apertureless‐SNOM setup to enhance the near‐field contribution of the scattered light and reduce the noise content. The interesting results obtained in this Aperture setup are described and commented.