Switchable optically active schottky barrier in La_(0.7)Sr(0.3)MnO_3/BaTiO_3/ITO ferroelectric tunnel junction

One of the most desirable attributes of non-volatile memories and memristors is a fast and non-destructive read out of their resistive state. Prototypical ferroelectric (FE) memories use the bulk photovoltaic response associated to the polarization of FE films to address this requirement by opticall...

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Detalles Bibliográficos
Autores: Rivera Calzada, Alberto Carlos, Gallego Toledo, Fernando, Kalcheim, Yoav, Salev, Pavel, Valle, Javier del, Tenreiro Villar, Isabel, León Yebra, Carlos, Santamaría Sánchez-Barriga, Jacobo, Schuller, Ivan K.
Tipo de recurso: artículo
Fecha de publicación:2021
País:España
Institución:Universidad Complutense de Madrid (UCM)
Repositorio:Docta Complutense
Idioma:inglés
OAI Identifier:oai:docta.ucm.es:20.500.14352/8157
Acceso en línea:https://hdl.handle.net/20.500.14352/8157
Access Level:acceso abierto
Palabra clave:538.9
Nonvolatile memory
Electroresistance
Films
Transition
Nanoscale
Ferroelectric tunnel junctions
Optical resistive sensing
Photovoltaic effect
Resistive switching
Schottky barrier
Física de materiales
Física del estado sólido
2211 Física del Estado Sólido
Descripción
Sumario:One of the most desirable attributes of non-volatile memories and memristors is a fast and non-destructive read out of their resistive state. Prototypical ferroelectric (FE) memories use the bulk photovoltaic response associated to the polarization of FE films to address this requirement by optically sensing binary memory cells. A more advanced type of non-volatile memories is FE tunnel junctions (FTJs). They feature resistive state ratios R_High/R_Low up to 10^6, with a continuum of resistive states accessible, making them promising candidates for neuromorphic computing applications. A novel approach is presented to achieve the optical sensing of the resistive state in a La_(0.7)Sr_(0.3)MnO_3/BaTiO_3/ITO FTJ, by using the Schottky barrier forming in the La_(0.7)Sr_(0.3)MnO_3/BaTiO_3/ITO interface to dramatically enhance the optical response of the 5 nm BaTiO3 (BTO) barrier. Illumination with UV light exceeding the BTO bandgap through the top transparent ITO electrode generates a photovoltaic response in the R_High state, with an open circuit voltage V_oc of 400 mV at 20 K, enabling the optical sensing of the resistive state. In the R_Low state, the Schottky barrier is removed and the photoresponse disappears.

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