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dc.contributor.authorRizzo, Daniel J.
dc.contributor.authorShabani, Sara
dc.contributor.authorJessen, Bjarke S.
dc.contributor.authorZhang, Jin
dc.contributor.authorMcLeod, Alexander S.
dc.contributor.authorRubio Verdú, Carmen
dc.contributor.authorRuta, Francesco L.
dc.contributor.authorCothrine, Matthew
dc.contributor.authorYan, Jiaqiang
dc.contributor.authorMandrus, David G.
dc.contributor.authorNagler, Stephen E.
dc.contributor.authorRubio Secades, Angel
dc.contributor.authorHone, James
dc.contributor.authorDean, Cory R.
dc.contributor.authorPasupathy, Abhay N.
dc.contributor.authorBasov, Dmitri N.
dc.date.accessioned2022-05-26T07:50:28Z
dc.date.available2022-05-26T07:50:28Z
dc.date.issued2022
dc.identifier.citationNano Letters 22 (5) : 1946-1953 (2022)es_ES
dc.identifier.issn1530-6992
dc.identifier.urihttp://hdl.handle.net/10810/56737
dc.description.abstract[EN] The ability to create nanometer-scale lateral p-n junctions is essential for the next generation of two-dimensional (2D) devices. Using the charge-transfer heterostructure graphene/alpha-RuCl3, we realize nanoscale lateral p-n junctions in the vicinity of graphene nanobubbles. Our multipronged experimental approach incorporates scanning tunneling microscopy (STM) and spectroscopy (STS) and scattering-type scanning near-field optical microscopy (s-SNOM) to simultaneously probe the electronic and optical responses of nanobubble p-n junctions. Our STM/STS results reveal that p-n junctions with a band offset of 0.6 eV can be achieved with widths of 3 nm, giving rise to electric fields of order 108 V/m. Concurrent s-SNOM measurements validate a point-scatterer formalism for modeling the interaction of surface plasmon polaritons (SPPs) with nanobubbles. Ab initio density functional theory (DFT) calculations corroborate our experimental data and reveal the dependence of charge transfer on layer separation. Our study provides experimental and conceptual foundations for generating p-n nanojunctions in 2D materials.es_ES
dc.description.sponsorshipResearch at Columbia University was supported as part of the Energy Frontier Research Center on Programmable Quantum Materials funded by the U.S. Department of Energy (DOE), Office of Science, Basic Energy Sciences (BES), under Award No DE-SC0019443. Plasmonic nano-imaging at Columbia University was supported by the U.S. Department of Energy (DOE), Office of Science, Basic Energy Sciences (BES), under Award No DE-SC0018426. J.Z. and A.R. were supported by the European Research Council (ERC-2015-AdG694097), the Cluster of Excellence “Advanced Imaging of Matter” (AIM) EXC 2056-390715994, funding by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) under RTG 2247, Grupos Consolidados (IT1249-19), and SFB925 “Light induced dynamics and control of correlated quantum systems”. J.Z. and A.R. would like to acknowledge Nicolas Tancogne-Dejean and Lede Xian for fruitful discussions and also acknowledge support by the Max Planck Institute-New York City Center for Non-Equilibrium Quantum Phenomena. The Flatiron Institute is a division of the Simons Foundation. J.Z. acknowledges funding received from the European Union Horizon 2020 research and innovation programme under Marie Skłodowska-Curie Grant Agreement 886291 (PeSD-NeSL). STM support was provided by the National Science Foundation via Grant DMR-2004691. C.R.-V. acknowledges funding from the European Union Horizon 2020 research and innovation programme under the Marie Skłodowska-Curie Grant Agreement 844271. D.G.M. acknowledges support from the Gordon and Betty Moore Foundation’s EPiQS Initiative, Grant GBMF9069. J.Q.Y. was supported by the U.S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division. S.E.N. acknowledges support from the U.S. Department of Energy, Office of Science, Basic Energy Sciences, Division of Scientific User Facilities. Work at University of Tennessee was supported by NSF Grant 180896.es_ES
dc.language.isoenges_ES
dc.publisherAmerican Chemical Societyes_ES
dc.relationinfo:eu-repo/grantAgreement/EC/H2020/886291es_ES
dc.relationinfo:eu-repo/grantAgreement/EC/H2020/844271es_ES
dc.rightsinfo:eu-repo/semantics/openAccesses_ES
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/3.0/es/*
dc.subjectscanning tunneling microscopyes_ES
dc.subjectscanning tunneling spectroscopyes_ES
dc.subjectscanning near-field optical microscopyes_ES
dc.subjectplasmonses_ES
dc.subjecttwo-dimensional materialses_ES
dc.subjectcharge transferes_ES
dc.titleNanometer-Scale Lateral p–n Junctions in Graphene/α-RuCl3 Heterostructureses_ES
dc.typeinfo:eu-repo/semantics/articlees_ES
dc.rights.holder© 2022 The Authors. Published by American Chemical Society. Attribution-NonCommercial-NoDerivatives 4.0 International (CC BY-NC-ND 4.0)es_ES
dc.rights.holderAtribución-NoComercial-SinDerivadas 3.0 España*
dc.relation.publisherversionhttps://pubs.acs.org/doi/10.1021/acs.nanolett.1c04579es_ES
dc.identifier.doi10.1021/acs.nanolett.1c04579
dc.contributor.funderEuropean Commission
dc.departamentoesPolímeros y Materiales Avanzados: Física, Química y Tecnologíaes_ES
dc.departamentoeuPolimero eta Material Aurreratuak: Fisika, Kimika eta Teknologiaes_ES


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© 2022 The Authors. Published by American Chemical Society. 
Attribution-NonCommercial-NoDerivatives 4.0 International (CC BY-NC-ND 4.0)
Except where otherwise noted, this item's license is described as © 2022 The Authors. Published by American Chemical Society. Attribution-NonCommercial-NoDerivatives 4.0 International (CC BY-NC-ND 4.0)