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...
Autores principales: | , , , , , , , , , , |
---|---|
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 |