Nano-engineered high-confinement AlGaAs waveguide devices for nonlinear photonics

The combination of nonlinear and integrated photonics enables applications in telecommunication, metrology, spectroscopy, and quantum information science. Pioneer works in silicon-on-insulator (SOI) has shown huge potentials of integrated nonlinear photonics. However, silicon suffers two-photon absorption (TPA) in the telecom wavelengths around 1550 nm, which hampers its practical applications. To get a superior nonlinear performance, an ideal integrated waveguide platform should combine a high material nonlinearity, low material absorption (linear and nonlinear), a strong light confinement, and a mature fabrication technology. Aluminum gallium arsenide (AlGaAs) was identified as a promising candidate for nonlinear applications since 1994. It offers a large transparency window, a high refractive index (n≈3.3), a nonlinear index (n2) on the order of 10-17 m2W−1, and the ability to engineer the material bandgap to mitigate TPA. In spite of the high intrinsic nonlinearity, conventional deep-etched AlGaAs waveguides exhibit low effective nonlinearity due to the vertical low-index contrast. To take full advantage of the high intrinsic linear and nonlinear index of AlGaAs material, we reconstructed the conventional AlGaAs waveguide into a high index contrast layout that has been realized in the AlGaAs-on-insulator (AlGaAsOI) platform. We have demonstrated low loss waveguides with an ultra-high nonlinear coefficient and high Q microresonators in such a platform. Owing to the high confinement waveguide layout and state-of-the-art nanolithography techniques, the dispersion properties of the AlGaAsOI waveguide can be tailored efficiently and accurately by altering the waveguide shape or dimension, which enables various applications in signal processing and generation, which will be reviewed in this paper.

[1]  Li Qian,et al.  Compact highly-nonlinear AlGaAs waveguides for efficient wavelength conversion. , 2011, Optics express.

[2]  J. S. Aitchison,et al.  AlGaAs Below Half Bandgap:. the Silicon of Nonlinear Optical Materials , 1994 .

[3]  R.W. Boyd,et al.  Enhanced nonlinear optical phase response of an AlGaAs microring resonator , 2004, InternationalQuantum Electronics Conference, 2004. (IQEC)..

[4]  C. Richardson,et al.  Low propagation loss AlGaAs waveguides fabricated with plasma-assisted photoresist reflow. , 2014, Optics express.

[5]  L. Lanco,et al.  Toward an AlGaAs/AlOx near-infrared integrated optical parametric oscillator , 2014 .

[6]  R. Morandotti,et al.  Extremely high aspect ratio GaAs and GaAs/AlGaAs nanowaveguides fabricated using chlorine ICP etching with N2-promoted passivation , 2010, Nanotechnology.

[7]  Hao Hu,et al.  Characterization and Optimization of a High-Efficiency AlGaAs-On-Insulator-Based Wavelength Converter for 64- and 256-QAM Signals , 2017, Journal of Lightwave Technology.

[8]  T. Kippenberg,et al.  Microresonator based optical frequency combs , 2012, CLEO 2012.

[9]  E. Semenova,et al.  Low-loss high-confinement waveguides and microring resonators in AlGaAs-on-insulator. , 2016, Optics letters.

[10]  J. S. Aitchison,et al.  The nonlinear optical properties of AlGaAs at the half band gap , 1997 .

[11]  Francesco Da Ros,et al.  Broadband and efficient dual-pump four-wave-mixing in AlGaAs-on-insulator nano-waveguides , 2016, 2016 Conference on Lasers and Electro-Optics (CLEO).

[12]  Toshio Morioka,et al.  Single-source algaas frequency comb transmitter for 661 Tbit/s data transmission in a 30-core fiber , 2016, 2016 Conference on Lasers and Electro-Optics (CLEO).

[13]  I Cristiani,et al.  Nonlinear properties of AlGaAs waveguides in continuous wave operation regime. , 2014, Optics express.

[14]  Michal Lipson,et al.  Nonlinear silicon photonics , 2012, 2012 17th Opto-Electronics and Communications Conference.

[15]  Hao Hu,et al.  Supercontinuum generation in AlGaAs-on-insulator nano-waveguide at telecom wavelengths , 2016, 2016 Conference on Lasers and Electro-Optics (CLEO).

[16]  K. Yvind,et al.  AlGaAs-on-insulator nanowire with 750 nm FWM bandwidth, −9 dB CW conversion efficiency, and ultrafast operation enabling record Tbaud wavelength conversion , 2015, 2015 Optical Fiber Communications Conference and Exhibition (OFC).

[17]  A Taflove,et al.  Waveguide-coupled AlGaAs / GaAs microcavity ring and disk resonators with high f inesse and 21.6-nm f ree spectral range. , 1997, Optics letters.

[18]  E. Semenova,et al.  Efficient frequency comb generation in AlGaAs-on-insulator , 2016 .

[19]  I Favero,et al.  Large second-harmonic generation at 1.55 μmin oxidized AlGaAs waveguides. , 2011, Optics letters.

[20]  J. Matsuoka,et al.  Temperature dependence of refractive index of SiO2 glass , 1991 .

[21]  M. Sorel,et al.  Low-power continuous-wave four-wave mixing wavelength conversion in AlGaAs-nanowaveguide microresonators. , 2015, Optics letters.

[22]  T. Hänsch,et al.  Optical frequency metrology , 2002, Nature.

[23]  T. Murphy,et al.  Efficient continuous-wave four-wave mixing in bandgap-engineered AlGaAs waveguides. , 2014, Optics letters.