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dc.contributor.authorAbidi, El Hadj
dc.contributor.authorKhan, Ayaz H.
dc.contributor.authorDelgado Notario, Juan Antonio 
dc.contributor.authorClericò, Vito 
dc.contributor.authorCalvo Gallego, Jaime 
dc.contributor.authorTaniguchi, Takashi
dc.contributor.authorWatanabe, Kenji
dc.contributor.authorOtsuji, Taiichi
dc.contributor.authorVelázquez Pérez, Jesús Enrique 
dc.contributor.authorMeziani, Yahya Moubarak 
dc.date.accessioned2025-01-22T11:20:29Z
dc.date.available2025-01-22T11:20:29Z
dc.date.issued2024
dc.identifier.citationAbidi, E.; Khan, A.; Delgado-Notario, J.A.; Clericó, V.; Calvo-Gallego, J.; Taniguchi, T.; Watanabe, K.; Otsuji, T.; Velázquez, J.E.; Meziani, Y.M. Terahertz Detection by Asymmetric Dual Grating Gate Bilayer Graphene FETs with Integrated Bowtie Antenna. Nanomaterials 2024, 14, 383. https://doi.org/10.3390/nano14040383es_ES
dc.identifier.issn2079-4991
dc.identifier.urihttp://hdl.handle.net/10366/162266
dc.description.abstract[EN]An asymmetric dual-grating gate bilayer graphene-based field effect transistor (ADGG-GFET) with an integrated bowtie antenna was fabricated and its response as a Terahertz (THz) detector was experimentally investigated. The device was cooled down to 4.5 K, and excited at different frequencies (0.15, 0.3 and 0.6 THz) using a THz solid-state source. The integration of the bowtie antenna allowed to obtain a substantial increase in the photocurrent response (up to 8 nA) of the device at the three studied frequencies as compared to similar transistors lacking the integrated antenna (1 nA). The photocurrent increase was observed for all the studied values of the bias voltage applied to both the top and back gates. Besides the action of the antenna that helps the coupling of THz radiation to the transistor channel, the observed enhancement by nearly one order of magnitude of the photoresponse is also related to the modulation of the hole and electron concentration profiles inside the transistor channel by the bias voltages imposed to the top and back gates. The creation of local n and p regions leads to the formation of homojuctions (𝑛𝑝 , 𝑝𝑛 or 𝑝𝑝+) along the channel that strongly affects the overall photoresponse of the detector. Additionally, the bias of both back and top gates could induce an opening of the gap of the bilayer graphene channel that would also contribute to the photocurrent.es_ES
dc.format.mimetypeapplication/pdf
dc.language.isoenges_ES
dc.publisherMDPIes_ES
dc.titleTerahertz Detection by Asymmetric Dual Grating Gate Bilayer Graphene FETs with Integrated Bowtie Antennaes_ES
dc.typeinfo:eu-repo/semantics/articlees_ES
dc.relation.publishversionhttps://doi.org/10.3390/nano14040383es_ES
dc.identifier.doi10.3390/nano14040383
dc.relation.projectIDPID2021-126483OB-I00es_ES
dc.relation.projectIDPID2022-136869NB-C33es_ES
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses_ES
dc.identifier.essn2079-4991
dc.journal.titleNanomaterialses_ES
dc.volume.number14es_ES
dc.issue.number4es_ES
dc.page.initial383es_ES
dc.type.hasVersioninfo:eu-repo/semantics/publishedVersiones_ES


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