Engineering Multiple GHz Mechanical Modes in Optomechanical Crystal Cavities

[EN] Optomechanical crystal cavities (OMCCs) are fundamental nanostructures for a wide range of phenomena and applications. Usually, optomechanical interaction in such OMCCs is limited to a single optical mode and a unique mechanical mode. In this sense, eliminating the single-mode constraint¿for in...

Descripción completa

Detalles Bibliográficos
Autores: Mercadé, Laura|||0000-0002-4994-7727, Ortiz-Fernández, Raúl|||0000-0002-4998-0201, Grau-Martínez, Alberto|||0000-0002-2411-1317, Griol Barres, Amadeu, Martínez, Alejandro|||0000-0001-5448-0140, Navarro-Urrios, Daniel
Tipo de recurso: artículo
Fecha de publicación:2023
País:España
Institución:Universitat Politècnica de València (UPV)
Repositorio:RiuNet. Repositorio Institucional de la Universitat Politécnica de Valéncia
Idioma:inglés
OAI Identifier:oai:riunet.upv.es:10251/212720
Acceso en línea:https://riunet.upv.es/handle/10251/212720
Access Level:acceso abierto
Palabra clave:Optomechanics
Nanophotonics
Cavity resonator
FISICA APLICADA
TEORÍA DE LA SEÑAL Y COMUNICACIONES
Descripción
Sumario:[EN] Optomechanical crystal cavities (OMCCs) are fundamental nanostructures for a wide range of phenomena and applications. Usually, optomechanical interaction in such OMCCs is limited to a single optical mode and a unique mechanical mode. In this sense, eliminating the single-mode constraint¿for instance, by adding more mechanical modes¿should enable more complex physical phenomena, giving rise to a context of multimode optomechanical interaction. However, a general method to produce in a controlled way multiple mechanical modes with large coupling rates in OMCCs is still missing. In this work, we present a route to confine multiple GHz mechanical modes coupled to the same optical field with similar optomechanical coupling rates¿up to 400 kHz¿by OMCC engineering. In essence, we increase the number of unit cells (consisting of a silicon nanobrick perforated by circular holes with corrugations at both its sides) in the adiabatic transition between the cavity center and the mirror region. Remarkably, the mechanical modes in our cavities are located within a full phononic band gap, which is a key requirement to achieve ultrahigh mechanical Q factors at cryogenic temperatures. The multimode behavior in a full phononic band gap and the easiness of realization using standard silicon nanotechnology make our OMCCs highly appealing for applications in the classical and quantum realms.