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Electric field-induced second-order nonlinear optical effects in silicon waveguides
Electric field-induced second-order nonlinear optical effects in silicon waveguides
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Electric field-induced second-order nonlinear optical effects in silicon waveguides
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Electric field-induced second-order nonlinear optical effects in silicon waveguides
Electric field-induced second-order nonlinear optical effects in silicon waveguides
Journal Article

Electric field-induced second-order nonlinear optical effects in silicon waveguides

2017
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Overview
The symmetry of crystalline silicon inhibits a second-order optical nonlinear susceptibility, χ (2) , in complementary metal–oxide–semiconductor-compatible silicon photonic platforms. However, χ (2) is required for important processes such as phase-only modulation, second-harmonic generation (SHG) and sum/difference frequency generation. Here, we break the crystalline symmetry by applying direct-current fields across p–i–n junctions in silicon ridge waveguides and induce a χ (2) proportional to the large χ (3) of silicon. The obtained χ (2) is first used to perturb the permittivity (the direct-current Kerr effect) and achieve phase-only modulation. Second, the spatial distribution of χ (2) is altered by periodically patterning p–i–n junctions to quasi-phase-match pump and second-harmonic modes and realize SHG. We measure a maximum SHG efficiency of P 2 ω / P ω 2  = 13 ± 0.5% W −1 at λ ω  = 2.29 µm and with field-induced χ (2)  = 41 ± 1.5 pm V –1 . We expect such field-induced χ (2) in silicon to lead to a new class of complex integrated devices such as carrier-envelope offset frequency stabilizers, terahertz generators, optical parametric oscillators and chirp-free modulators. The application of d.c. fields across p–i–n junctions in silicon ridge waveguides leads to crystal symmetry breaking. This induces a second-order optical nonlinear susceptibility that enables phase-only modulation and second-harmonic generation with an efficiency of ∼13% W –1 at 2.29 µm.