Beilstein J. Nanotechnol.2012,3, 674–683, doi:10.3762/bjnano.3.77
with a parabolic mirror based confocal microscope where the sample is scanned through the laser focus. By employing higherorderlasermodes (azimuthally and radially polarised laser beams), we can excite the Fischer patterns using either a pure in-plane (x,y) electric field or a strongly z-directional
orderlasermodes have been reported so far.
Here we present the investigation of gold nano-triangle Fischer patterns with a custom built confocal microscope. The use of higherorderlasermodes allows for the tuning of the polarisation in the laser focus so that it can be either perpendicular to the
described previously [21][22]. The Gaussian beam of a helium-neon laser (λ = 632.8 nm) is transformed by a mode converter to generate higherorderlasermodes: either a radially or an azimuthally polarised donut mode [23][24]. This mode is then focused onto the sample surface by a parabolic mirror of high
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Figure 1:
Focusing higher order laser modes with a parabolic mirror. (a) A sketch illustrating how a radial m...