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Two-Dimensional Iron Tungstate: A Ternary Oxide Layer With Honeycomb Geometry
[Image: see text] The exceptional physical properties of graphene have sparked tremendous interests toward two-dimensional (2D) materials with honeycomb structure. We report here the successful fabrication of 2D iron tungstate (FeWO(x)) layers with honeycomb geometry on a Pt(111) surface, using the...
Autores principales: | , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2016
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4838946/ https://www.ncbi.nlm.nih.gov/pubmed/27110319 http://dx.doi.org/10.1021/acs.jpcc.6b01086 |
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author | Pomp, S. Kuhness, D. Barcaro, G. Sementa, L. Mankad, V. Fortunelli, A. Sterrer, M. Netzer, F. P. Surnev, S. |
author_facet | Pomp, S. Kuhness, D. Barcaro, G. Sementa, L. Mankad, V. Fortunelli, A. Sterrer, M. Netzer, F. P. Surnev, S. |
author_sort | Pomp, S. |
collection | PubMed |
description | [Image: see text] The exceptional physical properties of graphene have sparked tremendous interests toward two-dimensional (2D) materials with honeycomb structure. We report here the successful fabrication of 2D iron tungstate (FeWO(x)) layers with honeycomb geometry on a Pt(111) surface, using the solid-state reaction of (WO(3))(3) clusters with a FeO(111) monolayer on Pt(111). The formation process and the atomic structure of two commensurate FeWO(x) phases, with (2 × 2) and (6 × 6) periodicities, have been characterized experimentally by combination of scanning tunneling microscopy (STM), low-energy electron diffraction (LEED), X-ray photoelectron spectroscopy (XPS), and temperature-programmed desorption (TPD) and understood theoretically by density functional theory (DFT) modeling. The thermodynamically most stable (2 × 2) phase has a formal FeWO(3) stoichiometry and corresponds to a buckled Fe(2+)/W(4+) layer arranged in a honeycomb lattice, terminated by oxygen atoms in Fe–W bridging positions. This 2D FeWO(3) layer has a novel structure and stoichiometry and has no analogues to known bulk iron tungstate phases. It is theoretically predicted to exhibit a ferromagnetic electronic ground state with a Curie temperature of 95 K, as opposed to the antiferromagnetic behavior of bulk FeWO(4) materials. |
format | Online Article Text |
id | pubmed-4838946 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2016 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-48389462016-04-22 Two-Dimensional Iron Tungstate: A Ternary Oxide Layer With Honeycomb Geometry Pomp, S. Kuhness, D. Barcaro, G. Sementa, L. Mankad, V. Fortunelli, A. Sterrer, M. Netzer, F. P. Surnev, S. J Phys Chem C Nanomater Interfaces [Image: see text] The exceptional physical properties of graphene have sparked tremendous interests toward two-dimensional (2D) materials with honeycomb structure. We report here the successful fabrication of 2D iron tungstate (FeWO(x)) layers with honeycomb geometry on a Pt(111) surface, using the solid-state reaction of (WO(3))(3) clusters with a FeO(111) monolayer on Pt(111). The formation process and the atomic structure of two commensurate FeWO(x) phases, with (2 × 2) and (6 × 6) periodicities, have been characterized experimentally by combination of scanning tunneling microscopy (STM), low-energy electron diffraction (LEED), X-ray photoelectron spectroscopy (XPS), and temperature-programmed desorption (TPD) and understood theoretically by density functional theory (DFT) modeling. The thermodynamically most stable (2 × 2) phase has a formal FeWO(3) stoichiometry and corresponds to a buckled Fe(2+)/W(4+) layer arranged in a honeycomb lattice, terminated by oxygen atoms in Fe–W bridging positions. This 2D FeWO(3) layer has a novel structure and stoichiometry and has no analogues to known bulk iron tungstate phases. It is theoretically predicted to exhibit a ferromagnetic electronic ground state with a Curie temperature of 95 K, as opposed to the antiferromagnetic behavior of bulk FeWO(4) materials. American Chemical Society 2016-03-24 2016-04-14 /pmc/articles/PMC4838946/ /pubmed/27110319 http://dx.doi.org/10.1021/acs.jpcc.6b01086 Text en Copyright © 2016 American Chemical Society This is an open access article published under a Creative Commons Attribution (CC-BY) License (http://pubs.acs.org/page/policy/authorchoice_ccby_termsofuse.html) , which permits unrestricted use, distribution and reproduction in any medium, provided the author and source are cited. |
spellingShingle | Pomp, S. Kuhness, D. Barcaro, G. Sementa, L. Mankad, V. Fortunelli, A. Sterrer, M. Netzer, F. P. Surnev, S. Two-Dimensional Iron Tungstate: A Ternary Oxide Layer With Honeycomb Geometry |
title | Two-Dimensional Iron Tungstate: A Ternary Oxide Layer
With Honeycomb Geometry |
title_full | Two-Dimensional Iron Tungstate: A Ternary Oxide Layer
With Honeycomb Geometry |
title_fullStr | Two-Dimensional Iron Tungstate: A Ternary Oxide Layer
With Honeycomb Geometry |
title_full_unstemmed | Two-Dimensional Iron Tungstate: A Ternary Oxide Layer
With Honeycomb Geometry |
title_short | Two-Dimensional Iron Tungstate: A Ternary Oxide Layer
With Honeycomb Geometry |
title_sort | two-dimensional iron tungstate: a ternary oxide layer
with honeycomb geometry |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4838946/ https://www.ncbi.nlm.nih.gov/pubmed/27110319 http://dx.doi.org/10.1021/acs.jpcc.6b01086 |
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