A new
concept for second-harmonic generation (SHG) in an optical
nanocircuit is proposed. We demonstrate both theoretically and experimentally
that the symmetry of an optical mode alone is sufficient to allow
SHG even in centro-symmetric structures made of centro-symmetric material.
The concept is realized using a plasmonic two-wire transmission-line
(TWTL), which simultaneously supports a symmetric and an antisymmetric
mode. We first confirm that emission of second-harmonic light into
the symmetric mode of the waveguide is symmetry-allowed when the fundamental
excited waveguide modes are either purely symmetric or antisymmetric.
We further switch the emission into the antisymmetric mode when a
controlled mixture of the fundamental modes is excited simultaneously.
Our results open up a new degree of freedom into the designs of nonlinear
optical components and should pave a new avenue toward multifunctional
nanophotonic circuitry.
The plasmon resonance of a metal nanoparticle increases the optical field amplitude in and around the particle with respect to the incoming wave. In consequence, optical effects that are nonlinear in their field amplitude profit from this increased field. In general, a plasmonic structure can react nonlinearly by itself and it can also enhance the effect of the nonlinearity in its environment, which we consider as plasmonic nanoantenna. In this paper, we review third-order nonlinear effects such as third-harmonic generation, pump-probe spectroscopy, coherent anti-Stokes Raman scattering and four-wave mixing of and near plasmonic nanostructures. All these processes are described by very similar equations for the nonlinear polarization, but the underling physics differs.
We present a fluorescent emitter (rhodamine B) coupled to a dielectric or metallic interface as well as a metallic cavity to study their radiative decay processes. Supported by finite-difference time-domain (FDTD) simulations, we correlate the non-radiative and radiative decay rates with the absorption and scattering cross section efficiencies, respectively. On a single particle level, we use atomic force microscopy (AFM), scanning electron microscopy (SEM), scattering spectroscopy, fluorescence life time imaging (FLIM) and time-correlated single photon counting (TCSPC) to evaluate the enhanced fluorescence decay at the same location. With this study, we show a colloidal gain material, which can be integrated into lattices using existing directed self-assembled methods to study their coherent energy transfer.
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