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      Chapter

      Tip-Enhanced Raman Spectroscopy: Principle and Instrumentation
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      Chapter

      Tip-Enhanced Raman Spectroscopy: Principle and Instrumentation

      DOI link for Tip-Enhanced Raman Spectroscopy: Principle and Instrumentation

      Tip-Enhanced Raman Spectroscopy: Principle and Instrumentation book

      Tip-Enhanced Raman Spectroscopy: Principle and Instrumentation

      DOI link for Tip-Enhanced Raman Spectroscopy: Principle and Instrumentation

      Tip-Enhanced Raman Spectroscopy: Principle and Instrumentation book

      ByJean-Christophe Valmalette
      BookHandbook of Enhanced Spectroscopy

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      Edition 1st Edition
      First Published 2015
      Imprint Jenny Stanford Publishing
      Pages 42
      eBook ISBN 9780429083150
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      ABSTRACT

      The nanoscale identification of molecules is a driving force for the

      knowledge in nanoscience and a key parameter in the further devel-

      opment of nanotechnology such as nanoelectronics, biotechnology,

      or green technology. Vibration of atoms in molecules provides

      valuable information on chemical species and is considered as a

      molecular “finger-print.” For example, vibration-based microscopy

      has recently shown the ability to track molecules in living tissues

      without the need for fluorescent labels [1, 2]. Furthermore,

      molecular vibrations or phonons in crystals are also sensitive to

      intrinsic perturbations (defects, plasmon-phonon coupling, etc.)

      and extrinsic perturbation (charge transfer, pressure, temperature,

      optical processes, etc.). Vibrations can be probed by only a limited

      number of techniques: infrared spectroscopy, inelastic neutron

      scattering, Raman scattering, and, more recently, inelastic scanning

      tunneling spectroscopy [3]. The last one “visualizes” the chemical

      nature of atoms and molecules on a surface but requires ultra-

      high vacuum (UHV) and very low temperature. The inelastic Raman

      scattering provides very rich information and does not require

      special sample preparation, but faces a low scattering cross section

      (10−31-10−26 cm2/molecule [4, 5]), and Abbe’s diffraction limited spatial resolution.

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