Terahertz displacive excitation of a coherent Raman-active phonon in V2O3

Nonlinear processes involving frequency-mixing of light fields set the basis for ultrafast coherent spectroscopy of collective modes in solids. In certain semimetals and semiconductors, generation of coherent phonon modes can occur by a displacive force on the lattice at the difference-frequency mix...

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Detalles Bibliográficos
Autores: Giorgianni, Flavio|||0000-0002-3810-4222, Udina, Mattia, Cea, Tommaso, Paris, Eugenio|||0000-0002-3418-8828, Caputo, Marco, Radovic, Milan|||0000-0003-4042-9648, Boie, Larissa|||0000-0002-1991-3980, Sakai, Joe|||0000-0001-7688-0655, Schneider, Christof W., Johnson, Steven Lee
Tipo de recurso: artículo
Fecha de publicación:2022
País:España
Institución:Universitat Autònoma de Barcelona
Repositorio:Dipòsit Digital de Documents de la UAB
Idioma:inglés
OAI Identifier:oai:ddd.uab.cat:266369
Acceso en línea:https://ddd.uab.cat/record/266369
https://dx.doi.org/urn:doi:10.1038/s42005-022-00882-7
Access Level:acceso abierto
Palabra clave:Coherent phonons
Coherent spectroscopies
Collective modes
Frequency mixing
Light fields
Nonlinear process
Phonon mode
Raman-active phonon
Tera Hertz
Ultra-fast
Descripción
Sumario:Nonlinear processes involving frequency-mixing of light fields set the basis for ultrafast coherent spectroscopy of collective modes in solids. In certain semimetals and semiconductors, generation of coherent phonon modes can occur by a displacive force on the lattice at the difference-frequency mixing of a laser pulse excitation on the electronic system. Here, as a low-frequency counterpart of this process, we demonstrate that coherent phonon excitations can be induced by the sum-frequency components of an intense terahertz light field, coupled to intraband electronic transitions. This nonlinear process leads to charge-coupled coherent dynamics of Raman-active phonon modes in the strongly correlated metal VO. Our results show an alternative up-conversion pathway for the optical control of Raman-active modes in solids mediated by terahertz-driven electronic excitation.