Please use this identifier to cite or link to this item: https://doi.org/10.1038/s41598-018-34903-9
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dc.titleCurvature induced quantum phase transitions in an electron-hole system
dc.contributor.authorSiu, Z.B
dc.contributor.authorChang, J.-Y
dc.contributor.authorTan, S.G
dc.contributor.authorJalil, M.B.A
dc.contributor.authorChang, C.-R
dc.date.accessioned2020-10-20T03:24:39Z
dc.date.available2020-10-20T03:24:39Z
dc.date.issued2018
dc.identifier.citationSiu, Z.B, Chang, J.-Y, Tan, S.G, Jalil, M.B.A, Chang, C.-R (2018). Curvature induced quantum phase transitions in an electron-hole system. Scientific Reports 8 (1) : 16497. ScholarBank@NUS Repository. https://doi.org/10.1038/s41598-018-34903-9
dc.identifier.issn20452322
dc.identifier.urihttps://scholarbank.nus.edu.sg/handle/10635/177806
dc.description.abstractIn this work, we study the effect of introducing a periodic curvature on nanostructures, and demonstrate that the curvature can lead to a transition from a topologically trivial state to a non-trivial state. We first present the Hamiltonian for an arbitrarily curved nanostructure, and introduce a numerical scheme for calculating the bandstructure of a periodically curved nanostructure. Using this scheme, we calculate the bandstructure for a sinusoidally curved two-dimensional electron gas. We show that the curvature can lead to a partner switching reminiscent of a topological phase transition at the time reversal invariant momenta. We then study the Bernevig-Hughes-Zhang (BHZ) Hamiltonian for a two-dimensional quantum well. We show that introducing a curvature can lead to the emergence of topological surface states. © 2018, The Author(s).
dc.rightsAttribution 4.0 International
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/
dc.sourceUnpaywall 20201031
dc.typeArticle
dc.contributor.departmentELECTRICAL AND COMPUTER ENGINEERING
dc.description.doi10.1038/s41598-018-34903-9
dc.description.sourcetitleScientific Reports
dc.description.volume8
dc.description.issue1
dc.description.page16497
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