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Abstract
High-harmonic generation (HHG) has been established as an indispensable tool in
optical spectroscopy. This effect arises for instance upon illumination of a
noble gas with sub-picosecond laser pulses at focussed intensities significantly
greater than 1012W/cm2. HHG provides a coherent light source in the extreme
ultraviolet (XUV) spectral region, which is of importance in inner shell photo
ionization of many atoms and molecules. Additionally, it intrinsically features
light fields with unique temporal properties. Even in its simplest realization,
XUV bursts of sub-femtosecond pulse lengths are released. More sophisticated
schemes open the path to attosecond physics by offering single pulses of less
than 100 attoseconds duration.
Resonant optical antennas are important tools for coupling and enhancing
electromagnetic fields on scales below their free-space wavelength. In a special
application, placing field-enhancing plasmonic nano antennas at the interaction
site of an HHG experiment has been claimed to boost local laser field strengths,
from insufficient initial intensities to sufficient values. This was achieved
with the use of arrays of bow-tie-shaped antennas of ∼ 100nm in length. However,
the feasibility of this concept depends on the vulnerability of these
nano-antennas to the still intense driving laser light.We show, by looking at a
set of exemplary metallic structures, that the threshold fluence Fth of
laser-induced damage (LID) is a greatly limiting factor for the proposed and
tested schemes along these lines.We present our findings in the context of work
done by other groups, giving an assessment of the feasibility and effectiveness
of the proposed scheme.
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