Please use this identifier to cite or link to this item: https://hdl.handle.net/10356/147882
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dc.contributor.authorHuang, Zumengen_US
dc.contributor.authorLiu, Yuandaen_US
dc.contributor.authorDini, Kévinen_US
dc.contributor.authorTan, Qinghaien_US
dc.contributor.authorLiu, Zhuojunen_US
dc.contributor.authorFang, Hanlinen_US
dc.contributor.authorLiu, Jinen_US
dc.contributor.authorLiew, Timothyen_US
dc.contributor.authorGao, Weiboen_US
dc.date.accessioned2021-04-14T06:36:22Z-
dc.date.available2021-04-14T06:36:22Z-
dc.date.issued2020-
dc.identifier.citationHuang, Z., Liu, Y., Dini, K., Tan, Q., Liu, Z., Fang, H., Liu, J., Liew, T. & Gao, W. (2020). Robust room temperature valley Hall effect of interlayer excitons. Nano Letters, 20(2), 1345-1351. https://dx.doi.org/10.1021/acs.nanolett.9b04836en_US
dc.identifier.issn1530-6984en_US
dc.identifier.urihttps://hdl.handle.net/10356/147882-
dc.description.abstractThe Berry curvature in the band structure of transition metal dichalcogenides (TMDs) introduces a valley-dependent effective magnetic field, which induces the valley Hall effect (VHE). Similar to the ordinary Hall effect, the VHE spatially separates carriers or excitons, depending on their valley index, and accumulates them at opposite sample edges. The VHE can play a key role in valleytronic devices, but previous observations of the VHE have been limited to cryogenic temperatures. Here, we report a demonstration of the VHE of interlayer excitons in a MoS2/WSe2 heterostructure at room temperature. We monitored the in-plane propagation of interlayer excitons through photoluminescence mapping and observed their spatial separation into two opposite transverse directions that depended on the valley index of the excitons. Our theoretical simulations reproduced the salient features of these observations. Our demonstration of the robust interlayer exciton VHE at room temperature, enabled by their intrinsically long lifetimes, will open up realistic possibilities for the development of opto-valleytronic devices based on TMD heterostructures.en_US
dc.description.sponsorshipMinistry of Education (MOE)en_US
dc.description.sponsorshipNational Research Foundation (NRF)en_US
dc.language.isoenen_US
dc.relationNRF-NRFF2015-03en_US
dc.relationNRF-CRP21-2018-0007en_US
dc.relationMOE2016-T2-2-077en_US
dc.relationMOE2016-T2-2-077en_US
dc.relationMOE2016-T3-1-006 (S)en_US
dc.relation.ispartofNano Lettersen_US
dc.relation.uri10.21979/N9/Q9MC8Wen_US
dc.rightsThis document is the Accepted Manuscript version of a Published Work that appeared in final form in Nano Letters, copyright © American Chemical Society after peer review and technical editing by the publisher. To access the final edited and published work see https://doi.org/10.1021/acs.nanolett.9b04836.en_US
dc.subjectScience::Physics::Optics and lighten_US
dc.titleRobust room temperature valley Hall effect of interlayer excitonsen_US
dc.typeJournal Articleen
dc.contributor.schoolSchool of Physical and Mathematical Sciencesen_US
dc.contributor.departmentPhysics and Applied Physicsen_US
dc.contributor.researchThe Photonics Instituteen_US
dc.contributor.researchCentre for Disruptive Photonic Technologies (CDPT)en_US
dc.identifier.doi10.1021/acs.nanolett.9b04836-
dc.identifier.issue2en_US
dc.identifier.volume20en_US
dc.identifier.spage1345en_US
dc.identifier.epage1351en_US
dc.subject.keywordsTMD Heterostructuresen_US
dc.subject.keywordsInterlayer Excitonsen_US
dc.description.acknowledgementWe acknowledge the support from the Singapore National Research Foundation (NRF-NRFF2015-03) and its Competitive Research Program (CRP Award NRF-CRP21-2018- 0007), Singapore Ministry of Education (MOE2016-T2-2- 077, MOE2016-T2-1-163, MOE2016-T3-1-006 (S)), and A*Star QTE programme. T.L. and K.D. were supported by the Singapore Ministry of Education (MOE2017-T2-1-001 and MOE2018-T3-1-002). The work done at Sun Yat-sen University was supported by the National Key R&D Program of China (2018YFA0306100), the National Natural Science Foundation of China (11874437), Guangzhou Science and Technology Project (201805010004) and the Natural Science Foundation of Guangdong (2018B030311027). We thank J. Kono for the helpful discussion.en_US
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