Cargando…

Atomic-Scale Structure of the Hematite α-Fe(2)O(3)(11̅02) “R-Cut” Surface

[Image: see text] The α-Fe(2)O(3)(11̅02) surface (also known as the hematite r-cut or (012) surface) was studied using low-energy electron diffraction (LEED), X-ray photoelectron spectroscopy (XPS), ultraviolet photoelectron spectroscopy (UPS), scanning tunneling microscopy (STM), noncontact atomic...

Descripción completa

Detalles Bibliográficos
Autores principales: Kraushofer, Florian, Jakub, Zdenek, Bichler, Magdalena, Hulva, Jan, Drmota, Peter, Weinold, Michael, Schmid, Michael, Setvin, Martin, Diebold, Ulrike, Blaha, Peter, Parkinson, Gareth S.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2017
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5823487/
https://www.ncbi.nlm.nih.gov/pubmed/29492182
http://dx.doi.org/10.1021/acs.jpcc.7b10515
_version_ 1783301893437521920
author Kraushofer, Florian
Jakub, Zdenek
Bichler, Magdalena
Hulva, Jan
Drmota, Peter
Weinold, Michael
Schmid, Michael
Setvin, Martin
Diebold, Ulrike
Blaha, Peter
Parkinson, Gareth S.
author_facet Kraushofer, Florian
Jakub, Zdenek
Bichler, Magdalena
Hulva, Jan
Drmota, Peter
Weinold, Michael
Schmid, Michael
Setvin, Martin
Diebold, Ulrike
Blaha, Peter
Parkinson, Gareth S.
author_sort Kraushofer, Florian
collection PubMed
description [Image: see text] The α-Fe(2)O(3)(11̅02) surface (also known as the hematite r-cut or (012) surface) was studied using low-energy electron diffraction (LEED), X-ray photoelectron spectroscopy (XPS), ultraviolet photoelectron spectroscopy (UPS), scanning tunneling microscopy (STM), noncontact atomic force microscopy (nc-AFM), and ab initio density functional theory (DFT)+U calculations. Two surface structures are stable under ultrahigh vacuum (UHV) conditions; a stoichiometric (1 × 1) surface can be prepared by annealing at 450 °C in ≈10(–6) mbar O(2), and a reduced (2 × 1) reconstruction is formed by UHV annealing at 540 °C. The (1 × 1) surface is close to an ideal bulk termination, and the undercoordinated surface Fe atoms reduce the surface bandgap by ≈0.2 eV with respect to the bulk. The work function is measured to be 5.7 ± 0.2 eV, and the VBM is located 1.5 ± 0.1 eV below E(F). The images obtained from the (2 × 1) reconstruction cannot be reconciled with previously proposed models, and a new “alternating trench” structure is proposed based on an ordered removal of lattice oxygen atoms. DFT+U calculations show that this surface is favored in reducing conditions and that 4-fold-coordinated Fe(2+) cations at the surface introduce gap states approximately 1 eV below E(F). The work function on the (2 × 1) termination is 5.4 ± 0.2 eV.
format Online
Article
Text
id pubmed-5823487
institution National Center for Biotechnology Information
language English
publishDate 2017
publisher American Chemical Society
record_format MEDLINE/PubMed
spelling pubmed-58234872018-02-26 Atomic-Scale Structure of the Hematite α-Fe(2)O(3)(11̅02) “R-Cut” Surface Kraushofer, Florian Jakub, Zdenek Bichler, Magdalena Hulva, Jan Drmota, Peter Weinold, Michael Schmid, Michael Setvin, Martin Diebold, Ulrike Blaha, Peter Parkinson, Gareth S. J Phys Chem C Nanomater Interfaces [Image: see text] The α-Fe(2)O(3)(11̅02) surface (also known as the hematite r-cut or (012) surface) was studied using low-energy electron diffraction (LEED), X-ray photoelectron spectroscopy (XPS), ultraviolet photoelectron spectroscopy (UPS), scanning tunneling microscopy (STM), noncontact atomic force microscopy (nc-AFM), and ab initio density functional theory (DFT)+U calculations. Two surface structures are stable under ultrahigh vacuum (UHV) conditions; a stoichiometric (1 × 1) surface can be prepared by annealing at 450 °C in ≈10(–6) mbar O(2), and a reduced (2 × 1) reconstruction is formed by UHV annealing at 540 °C. The (1 × 1) surface is close to an ideal bulk termination, and the undercoordinated surface Fe atoms reduce the surface bandgap by ≈0.2 eV with respect to the bulk. The work function is measured to be 5.7 ± 0.2 eV, and the VBM is located 1.5 ± 0.1 eV below E(F). The images obtained from the (2 × 1) reconstruction cannot be reconciled with previously proposed models, and a new “alternating trench” structure is proposed based on an ordered removal of lattice oxygen atoms. DFT+U calculations show that this surface is favored in reducing conditions and that 4-fold-coordinated Fe(2+) cations at the surface introduce gap states approximately 1 eV below E(F). The work function on the (2 × 1) termination is 5.4 ± 0.2 eV. American Chemical Society 2017-12-08 2018-01-25 /pmc/articles/PMC5823487/ /pubmed/29492182 http://dx.doi.org/10.1021/acs.jpcc.7b10515 Text en Copyright © 2017 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 Kraushofer, Florian
Jakub, Zdenek
Bichler, Magdalena
Hulva, Jan
Drmota, Peter
Weinold, Michael
Schmid, Michael
Setvin, Martin
Diebold, Ulrike
Blaha, Peter
Parkinson, Gareth S.
Atomic-Scale Structure of the Hematite α-Fe(2)O(3)(11̅02) “R-Cut” Surface
title Atomic-Scale Structure of the Hematite α-Fe(2)O(3)(11̅02) “R-Cut” Surface
title_full Atomic-Scale Structure of the Hematite α-Fe(2)O(3)(11̅02) “R-Cut” Surface
title_fullStr Atomic-Scale Structure of the Hematite α-Fe(2)O(3)(11̅02) “R-Cut” Surface
title_full_unstemmed Atomic-Scale Structure of the Hematite α-Fe(2)O(3)(11̅02) “R-Cut” Surface
title_short Atomic-Scale Structure of the Hematite α-Fe(2)O(3)(11̅02) “R-Cut” Surface
title_sort atomic-scale structure of the hematite α-fe(2)o(3)(11̅02) “r-cut” surface
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5823487/
https://www.ncbi.nlm.nih.gov/pubmed/29492182
http://dx.doi.org/10.1021/acs.jpcc.7b10515
work_keys_str_mv AT kraushoferflorian atomicscalestructureofthehematiteafe2o31102rcutsurface
AT jakubzdenek atomicscalestructureofthehematiteafe2o31102rcutsurface
AT bichlermagdalena atomicscalestructureofthehematiteafe2o31102rcutsurface
AT hulvajan atomicscalestructureofthehematiteafe2o31102rcutsurface
AT drmotapeter atomicscalestructureofthehematiteafe2o31102rcutsurface
AT weinoldmichael atomicscalestructureofthehematiteafe2o31102rcutsurface
AT schmidmichael atomicscalestructureofthehematiteafe2o31102rcutsurface
AT setvinmartin atomicscalestructureofthehematiteafe2o31102rcutsurface
AT dieboldulrike atomicscalestructureofthehematiteafe2o31102rcutsurface
AT blahapeter atomicscalestructureofthehematiteafe2o31102rcutsurface
AT parkinsongareths atomicscalestructureofthehematiteafe2o31102rcutsurface