Exploring the electronic and magnetic properties of new metal halides from bulk to two-dimensional monolayer: RuX3 (X = Br, I)

buir.contributor.authorErsan, Fatih
buir.contributor.authorKadıoğlu, Yelda
dc.citation.epage119en_US
dc.citation.spage111en_US
dc.citation.volumeNumber476en_US
dc.contributor.authorErsan, Fatihen_US
dc.contributor.authorVatansever, E.en_US
dc.contributor.authorSarikurt, S.en_US
dc.contributor.authorYüksel, Y.en_US
dc.contributor.authorKadıoğlu, Yeldaen_US
dc.contributor.authorOzaydin, H.en_US
dc.contributor.authorAktürk, O. Ü.en_US
dc.contributor.authorAkıncı, Ü.en_US
dc.contributor.authorAktürk, E.en_US
dc.date.accessioned2020-02-05T05:28:38Z
dc.date.available2020-02-05T05:28:38Z
dc.date.issued2018
dc.departmentDepartment of Physicsen_US
dc.description.abstractTheoretical and experimental studies present that metal halogens in MX3 forms can show very interesting electronic and magnetic properties in their bulk and monolayer phases. Many MX3 materials have layered structures in their bulk phases, while RuBr3 and RuI3 have one-dimensional chains in plane. In this paper, we show that these metal halogens can also form two-dimensional layered structures in the bulk phase similar to other metal halogens, and cleavage energy values confirm that the monolayers of RuX3 can be possible to be synthesized. We also find that monolayers of RuX3 prefer ferromagnetic spin orientation in the plane for Ru atoms. Their ferromagnetic ground state, however, changes to antiferromagnetic zigzag state after U is included. Calculations using PBE + U with SOC predict indirect band gap of 0.70 eV and 0.32 eV for the optimized structure of RuBr3 and RuI3, respectively. Calculation based on the Monte Carlo simulations reveal interesting magnetic properties of RuBr3, such as large Curie temperature against RuI3, both in bulk and monolayer cases. Moreover, as a result of varying exchange couplings between neighboring magnetic moments, magnetic properties of RuBr3 and RuI3 can undergo drastic changes from bulk to monolayer. We hope our findings can be useful to attempt to fabricate the bulk and monolayer of RuBr3 and RuI3.en_US
dc.description.provenanceSubmitted by Onur Emek (onur.emek@bilkent.edu.tr) on 2020-02-05T05:28:38Z No. of bitstreams: 1 Bilkent-research-paper.pdf: 268963 bytes, checksum: ad2e3a30c8172b573b9662390ed2d3cf (MD5)en
dc.description.provenanceMade available in DSpace on 2020-02-05T05:28:38Z (GMT). No. of bitstreams: 1 Bilkent-research-paper.pdf: 268963 bytes, checksum: ad2e3a30c8172b573b9662390ed2d3cf (MD5) Previous issue date: 2018en
dc.embargo.release2021-04-15
dc.identifier.doi10.1016/j.jmmm.2018.12.032en_US
dc.identifier.issn0304-8853
dc.identifier.urihttp://hdl.handle.net/11693/53062
dc.language.isoEnglishen_US
dc.publisherElsevieren_US
dc.relation.isversionofhttps://dx.doi.org/10.1016/j.jmmm.2018.12.032en_US
dc.source.titleJournal of Magnetism and Magnetic Materialsen_US
dc.subjectMonolayer RuBr3 and RuI3en_US
dc.subjectMagnetic propertiesen_US
dc.subjectDensity functional theoryen_US
dc.subjectMonte Carlo methoden_US
dc.titleExploring the electronic and magnetic properties of new metal halides from bulk to two-dimensional monolayer: RuX3 (X = Br, I)en_US
dc.typeArticleen_US

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