Coherent nonlinear microscopy (CNM) is widely used in three-dimensional imaging
of transparent samples, particularly for biological tissues [1]. Examples for
parametric and label free CNM processes are second harmonic generation (SHG)
and third harmonic generation (THG). However, working under far off-resonant
excitation conditions usually leads to low optical conversion efficiencies.
Hence, the typically low signals may lead to a bad signal-to-noise ratio and
low image contrast. There are several approaches to enhance the signal yield in
CNM, e.g. using dispersion to optimize the phase-matching integral [2]. One
promising concept is the “Enhancement of Second-Order Nonlinear-Optical Signals
by Optical Stimulation” [3]. The basic idea is to stimulate a nonlinear signal
by already “seeding” with some radiation at the harmonic frequency. The
previous and first demonstration of the concept for SHG yielded signal
enhancements more than 10 in a biologically relevant medium. We present
strong enhancements of third harmonic generation by optical stimulation in a
microscopy setup. The effect is most pronounced at low laser intensity and weak
nonlinear susceptibilities, making it suitable in harmonic microscopy.
[1] S. Yue, M.N. Slipchenko, J.-X. Cheng, “Multimodal nonlinear optical
microscopy”, Laser Photon. Rev. 5, 496–512 (2011).
[2] Christian Stock, Kaloyan Zlatanov, and Thomas Halfmann,
“Dispersion-enhanced third-harmonic microscopy”, Optics Communications Vol.
393, 289-293 (2017).
[3] A. J. Goodman and W. A. Tisdale, “Enhancement of Second-Order
Nonlinear-Optical Signals by Optical Stimulation”, Phys. Rev. Lett. 114,
183902 (2015).
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