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dc.contributor.authorAres García, Pablo 
dc.contributor.authorPakdel, Sahar
dc.contributor.authorPalacio, Irene
dc.contributor.authorPaz, Wendel S.
dc.contributor.authorRassekh, Maedeh
dc.contributor.authorRodríguez-San Miguel, David
dc.contributor.authorAballe, Lucía
dc.contributor.authorFoerster, Michael
dc.contributor.authorRuiz del Árbol, Nerea
dc.contributor.authorMartín-Gago, José Ángel
dc.contributor.authorZamora Abanades, Félix Juan 
dc.contributor.authorGómez Herrero, Julio 
dc.contributor.authorPalacios Burgos, Juan José 
dc.contributor.otherUAM. Departamento de Física de la Materia Condensadaes_ES
dc.contributor.otherUAM. Departamento de Química Inorgánicaes_ES
dc.date.accessioned2022-02-24T08:36:37Z
dc.date.available2022-02-24T08:36:37Z
dc.date.issued2021-09-01
dc.identifier.citationApplied Materials Today 24 (2021): 101132en_US
dc.identifier.issn2352-9407es_ES
dc.identifier.urihttp://hdl.handle.net/10486/700480
dc.description.abstractAntimonene -a single layer of antimony atoms- and its few layer forms are among the latest additions to the 2D mono-elemental materials family. Numerous predictions and experimental evidence of its remarkable properties including (opto)electronic, energetic or biomedical, among others, together with its robustness under ambient conditions, have attracted the attention of the scientific community. However, experimental evidence of its electrical properties is still lacking. Here, we characterized the electronic properties of mechanically exfoliated flakes of few-layer (FL) antimonene of different thicknesses (∼ 2–40 nm) through photoemission electron microscopy, kelvin probe force microscopy and transport measurements, which allows us to estimate a sheet resistance of ∼ 1200 Ω sq−1 and a mobility of ∼ 150 cm2V−1s−1 in ambient conditions, independent of the flake thickness. Alternatively, our theoretical calculations indicate that topologically protected surface states (TPSS) should play a key role in the electronic properties of FL antimonene, which supports our experimental findings. We anticipate our work will trigger further experimental studies on TPSS in FL antimonene thanks to its simple structure and significant stability in ambient environmentsen_US
dc.description.sponsorshipWe acknowledge financial support through the “Maríade Maeztu” Programme for Units of Excellence in R&D (CEX2018-000805-M), the Spanish MINECO through projects PCI2018-093081, FIS2016-80434-P, PID2019-109539GB-C43, PID2019- 106268GB-C31 and -C32, MAT2016-77608-C3-1-P and -3-P, MAT2013-46753-C2-2-P and MAT2017-85089-C2-1R, the EU Graphene Flagship funding (Graphene Flagship Core3 881603 and JTC2017/2D-Sb&Ge), the EU via the ERC-Synergy Program (GrantERC-2013-SYG-610256 NANOCOSMOS), the Comunidad Autónoma de Madrid through MAD2D-CM, S2018/NMT-4321 (NanomagCOST-CM) and the European StructuralFunds via FotoArt CM project (S2018/NMT-4367), and the Fundación Ramón Areces. S.P. acknowledges financial support by the VILLUM FONDEN via the Centre of Excellence for Dirac Materials (Grant No. 11744)en_US
dc.format.extent8 pag.es_ES
dc.format.mimetypeapplication/pdfes_ES
dc.language.isoenges_ES
dc.publisherElsevieren_US
dc.relation.ispartofApplied Materials Todayen_US
dc.rights© 2021 The Authorsen_US
dc.subject.otherAntimony atomsen_US
dc.subject.otherPhotoemission electron microscopyen_US
dc.subject.otherKelvin probe force microscopyen_US
dc.subject.otherElectronic propertiesen_US
dc.titleFew-layer antimonene electrical propertiesen_US
dc.typearticlees_ES
dc.subject.ecienciaFísicaes_ES
dc.relation.publisherversionhttps://doi.org/10.1016/j.apmt.2021.101132es_ES
dc.identifier.doi10.1016/j.apmt.2021.101132es_ES
dc.identifier.publicationfirstpage101132-1es_ES
dc.identifier.publicationlastpage101132-8es_ES
dc.identifier.publicationvolume24es_ES
dc.relation.projectIDGobierno de España. CEX2018-000805-Mes_ES
dc.relation.projectIDGobierno de España. PCI2018-093081es_ES
dc.relation.projectIDGobierno de España. FIS2016-80434-Pes_ES
dc.relation.projectIDGobierno de España. PID2019-109539GB-C43es_ES
dc.relation.projectIDGobierno de España. PID2019-106268GB-C31es_ES
dc.relation.projectIDGobierno de España. PID2019-106268GB-C32es_ES
dc.relation.projectIDGobierno de España. MAT2016-77608-C3-1-Pes_ES
dc.relation.projectIDGobierno de España. MAT2016-77608-C3-3-Pes_ES
dc.relation.projectIDGobierno de España. MAT2013-46753-C2-2-Pes_ES
dc.relation.projectIDGobierno de España. MAT2017-85089-C2-1-Res_ES
dc.relation.projectIDinfo:eu-repo/grantAgreement/EC/H2020/881603/EU//GrapheneCore3es_ES
dc.relation.projectIDinfo:eu-repo/grantAgreement/EC/FP7/610256/EU//NANOCOSMOSes_ES
dc.relation.projectIDComunidad de Madrid. S2013/MIT-3007/MAD2D-CMes_ES
dc.relation.projectIDComunidad de Madrid. S2018/NMT-4321/NanomagCOST-CMes_ES
dc.relation.projectIDComunidad de Madrid. S2018/NMT-4367-FotoArt-CMes_ES
dc.type.versioninfo:eu-repo/semantics/publishedVersiones_ES
dc.rights.ccReconocimientoes
dc.rights.accessRightsopenAccesses_ES
dc.authorUAMAres García, Pablo (260701)
dc.authorUAMGómez Herrero, Julio (260232)
dc.authorUAMPalacios Burgos, Juan José (262184)
dc.authorUAMZamora Abanades, Félix Juan (258846)
dc.authorUAMRodríguez San Miguel, David (265015)
dc.facultadUAMFacultad de Ciencias
dc.institutoUAMCentro de Investigación en Física de la Materia Condensada (IFIMAC)
dc.institutoUAMInstituto de Investigación Avanzada en Ciencias Químicas (IAdChem)


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