Optomechanical gigahertz oscillator made of a two photon absorption free piezoelectric III/V semiconductor
Inès Ghorbel,
François Swiadek,
Rui Zhu,
Daniel Dolfi,
Gaëlle Lehoucq,
Aude Martin,
Grégory Moille,
Loïc Morvan,
Rémy Braive,
Sylvain Combrié,
Alfredo De Rossi
Affiliations
Inès Ghorbel
Thales Research and Technology, 1 Avenue Augustin Fresnel, 91767 Palaiseau, France
François Swiadek
Thales Research and Technology, 1 Avenue Augustin Fresnel, 91767 Palaiseau, France
Rui Zhu
Centre de Nanosciences et de Nanotechnologies, CNRS, Université Paris-Sud, Université Paris-Saclay, C2N, 10, Boulevard Thomas Gobert, 91120 Palaiseau, France
Daniel Dolfi
Thales Research and Technology, 1 Avenue Augustin Fresnel, 91767 Palaiseau, France
Gaëlle Lehoucq
Thales Research and Technology, 1 Avenue Augustin Fresnel, 91767 Palaiseau, France
Aude Martin
Thales Research and Technology, 1 Avenue Augustin Fresnel, 91767 Palaiseau, France
Grégory Moille
Thales Research and Technology, 1 Avenue Augustin Fresnel, 91767 Palaiseau, France
Loïc Morvan
Thales Research and Technology, 1 Avenue Augustin Fresnel, 91767 Palaiseau, France
Rémy Braive
Centre de Nanosciences et de Nanotechnologies, CNRS, Université Paris-Sud, Université Paris-Saclay, C2N, 10, Boulevard Thomas Gobert, 91120 Palaiseau, France
Sylvain Combrié
Thales Research and Technology, 1 Avenue Augustin Fresnel, 91767 Palaiseau, France
Alfredo De Rossi
Thales Research and Technology, 1 Avenue Augustin Fresnel, 91767 Palaiseau, France
Oscillators in the gigahertz frequency range are key building blocks for telecommunication and positioning applications. Operating directly in the gigahertz while keeping high frequency stability and compactness is still an up-to-date challenge. Optomechanical crystals have demonstrated gigahertz frequency modes, thus gathering prerequisite features for using them as oscillators. Here, we report on the demonstration, in ambient atmospheric conditions, of an optomechanical crystal based on the concept of bichromatic lattice. It is made of InGaP, a low loss and TPA-free piezoelectric material, which makes it valuable for optomechanics. Self-sustained oscillations directly at 3 GHz are routinely achieved with a low optical power threshold of 40 μW and a short-term linewidth narrowed down to 100 Hz in agreement with phase noise measurements (−110 dBc/Hz at 1 MHz from the carrier) for free running optomechanical oscillators.