Two-Dimensional Iron Tungstate: A Ternary Oxide Layer With Honeycomb Geometry
Author(s) -
Sascha Pomp,
David Kuhness,
Giovanni Barcaro,
Luca Sementa,
Venu Mankad,
Alessandro Fortunelli,
Martin Sterrer,
F. P. Netzer,
S. Surnev
Publication year - 2016
Publication title -
the journal of physical chemistry c
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.401
H-Index - 289
eISSN - 1932-7455
pISSN - 1932-7447
DOI - 10.1021/acs.jpcc.6b01086
Subject(s) - density functional theory , materials science , x ray photoelectron spectroscopy , scanning tunneling microscope , tungstate , ferromagnetism , monolayer , antiferromagnetism , ternary operation , crystallography , stoichiometry , condensed matter physics , chemistry , nanotechnology , computational chemistry , nuclear magnetic resonance , physics , computer science , metallurgy , programming language
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.
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