Hexagonal Aln: Dimensional-Crossover Band-Gap Transition
| dc.contributor.author | Bacaksız, Cihan | |
| dc.contributor.author | Şahin, Hasan | |
| dc.contributor.author | Özaydın, H. Duygu | |
| dc.contributor.author | Horzum, Şeyda | |
| dc.contributor.author | Senger, Ramazan Tugrul | |
| dc.contributor.author | Peeters, François M. | |
| dc.coverage.doi | 10.1103/PhysRevB.91.085430 | |
| dc.date.accessioned | 2017-07-19T08:44:32Z | |
| dc.date.available | 2017-07-19T08:44:32Z | |
| dc.date.issued | 2015 | |
| dc.description.abstract | Motivated by a recent experiment that reported the successful synthesis of hexagonal (h) AlN [Tsipas, Appl. Phys. Lett. 103, 251605 (2013)APPLAB0003-695110.1063/1.4851239], we investigate structural, electronic, and vibrational properties of bulk, bilayer, and monolayer structures of h-AlN by using first-principles calculations. We show that the hexagonal phase of the bulk h-AlN is a stable direct-band-gap semiconductor. The calculated phonon spectrum displays a rigid-layer shear mode at 274 cm-1 and an Eg mode at 703 cm-1, which are observable by Raman measurements. In addition, single-layer h-AlN is an indirect-band-gap semiconductor with a nonmagnetic ground state. For the bilayer structure, AA′-type stacking is found to be the most favorable one, and interlayer interaction is strong. While N-layered h-AlN is an indirect-band-gap semiconductor for N=1-9, we predict that thicker structures (N≥10) have a direct band gap at the Γ point. The number-of-layer-dependent band-gap transitions in h-AlN is interesting in that it is significantly different from the indirect-to-direct crossover obtained in the transition-metal dichalcogenides. | en_US |
| dc.description.sponsorship | Flemish Science Foundation (FWO-Vl); Methusalem foundation of the Flemish government; TUBITAK Project (114F397); FWO Pegasus Long Marie Curie Fellowship | en_US |
| dc.identifier.citation | Bacaksız, C., Şahin, H., Özaydın, H.D., Horzum, Ş., Senger, R.T., and Peeters, F.M. (2015). Hexagonal AlN: Dimensional-crossover-driven band-gap transition. Physical Review B - Condensed Matter and Materials Physics, 91(8). doi:10.1103/PhysRevB.91.085430 | en_US |
| dc.identifier.doi | 10.1103/PhysRevB.91.085430 | |
| dc.identifier.doi | 10.1103/PhysRevB.91.085430 | en_US |
| dc.identifier.issn | 1098-0121 | |
| dc.identifier.issn | 1550-235X | |
| dc.identifier.issn | 1098-0121 | |
| dc.identifier.scopus | 2-s2.0-84924084572 | |
| dc.identifier.uri | https://doi.org/10.1103/PhysRevB.91.085430 | |
| dc.identifier.uri | https://hdl.handle.net/11147/5959 | |
| dc.language.iso | en | en_US |
| dc.publisher | American Physical Society | en_US |
| dc.relation | info:eu-repo/grantAgreement/TUBITAK/MFAG/114F397 | en_US |
| dc.relation.ispartof | Physical Review B - Condensed Matter and Materials Physics | en_US |
| dc.rights | info:eu-repo/semantics/openAccess | en_US |
| dc.subject | Graphene | en_US |
| dc.subject | Hexagonal AlN | en_US |
| dc.subject | Phonon spectrum | en_US |
| dc.subject | Semiconductor surfaces | en_US |
| dc.subject | Adsorbate structure | en_US |
| dc.title | Hexagonal Aln: Dimensional-Crossover Band-Gap Transition | en_US |
| dc.type | Article | en_US |
| dspace.entity.type | Publication | |
| gdc.author.institutional | Bacaksız, Cihan | |
| gdc.author.institutional | Özaydın, H. Duygu | |
| gdc.author.institutional | Senger, Ramazan Tugrul | |
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| gdc.description.department | İzmir Institute of Technology. Physics | en_US |
| gdc.description.issue | 8 | en_US |
| gdc.description.publicationcategory | Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
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| gdc.description.volume | 91 | en_US |
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| gdc.oaire.keywords | Condensed Matter - Materials Science | |
| gdc.oaire.keywords | Hexagonal AlN | |
| gdc.oaire.keywords | Semiconductor surfaces | |
| gdc.oaire.keywords | Phonon spectrum | |
| gdc.oaire.keywords | Materials Science (cond-mat.mtrl-sci) | |
| gdc.oaire.keywords | FOS: Physical sciences | |
| gdc.oaire.keywords | Graphene | |
| gdc.oaire.keywords | Adsorbate structure | |
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