Coexisting commensurate and incommensurate charge ordered phases in CoO

Abstract The subtle interplay of strong electronic correlations in a distorted crystal lattice often leads to the evolution of novel emergent functionalities in the strongly correlated materials (SCM). Here, we unravel such unprecedented commensurate (COM) and incommensurate (ICOM) charge ordered (C...

Full description

Bibliographic Details
Main Authors: Devendra Negi, Deobrat Singh, Rajeev Ahuja, Peter A. van Aken
Format: Article
Language:English
Published: Nature Portfolio 2021-09-01
Series:Scientific Reports
Online Access:https://doi.org/10.1038/s41598-021-98739-6
_version_ 1830412259440984064
author Devendra Negi
Deobrat Singh
Rajeev Ahuja
Peter A. van Aken
author_facet Devendra Negi
Deobrat Singh
Rajeev Ahuja
Peter A. van Aken
author_sort Devendra Negi
collection DOAJ
description Abstract The subtle interplay of strong electronic correlations in a distorted crystal lattice often leads to the evolution of novel emergent functionalities in the strongly correlated materials (SCM). Here, we unravel such unprecedented commensurate (COM) and incommensurate (ICOM) charge ordered (CO) phases at room temperature in a simple transition-metal mono-oxide, namely CoO. The electron diffraction pattern unveils a COM ( $$q_{1}$$ q 1 = $$\frac{1}{2}(1,1,{\bar{1}})$$ 1 2 ( 1 , 1 , 1 ¯ ) and ICOM ( $$q_{2}=0.213(1,1,{\bar{1}})$$ q 2 = 0.213 ( 1 , 1 , 1 ¯ ) ) periodic lattice distortion. Transmission electron microscopy (TEM) captures unidirectional and bidirectional stripe patterns of charge density modulations. The widespread phase singularities in the phase-field of the order parameter (OP) affirms the abundant topological disorder. Using, density functional theory (DFT) calculations, we demystify the underlying electronic mechanism. The DFT study shows that a cation disordering ( $$\mathrm {Co}_{1-\textit{x}}\mathrm {O}, \text {with }{} \textit{x} = 4.17 \%$$ Co 1 - x O , with x = 4.17 % ) stabilizes Jahn-Teller (JT) distortion and localized aliovalent $$\mathrm {Co}^{3+}$$ Co 3 + states in CoO. Therefore, the lattice distortion accompanied with mixed valence states ( $$\mathrm {Co}^{3+}, \mathrm {Co}^{2+}$$ Co 3 + , Co 2 + ) states introduces CO in CoO. Our findings offer an electronic paradigm to engineer CO to exploit the associated electronic functionalities in widely available transition-metal mono-oxides.
first_indexed 2024-12-20T20:04:14Z
format Article
id doaj.art-8606e978a0e54a10bac5859af8f47b7b
institution Directory Open Access Journal
issn 2045-2322
language English
last_indexed 2024-12-20T20:04:14Z
publishDate 2021-09-01
publisher Nature Portfolio
record_format Article
series Scientific Reports
spelling doaj.art-8606e978a0e54a10bac5859af8f47b7b2022-12-21T19:27:58ZengNature PortfolioScientific Reports2045-23222021-09-011111810.1038/s41598-021-98739-6Coexisting commensurate and incommensurate charge ordered phases in CoODevendra Negi0Deobrat Singh1Rajeev Ahuja2Peter A. van Aken3Stuttgart Center for Electron Microscopy, Max Planck Institute for Solid State ResearchCondensed Matter Theory Group, Materials Theory Division, Department of Physics and Astronomy, Uppsala UniversityCondensed Matter Theory Group, Materials Theory Division, Department of Physics and Astronomy, Uppsala UniversityStuttgart Center for Electron Microscopy, Max Planck Institute for Solid State ResearchAbstract The subtle interplay of strong electronic correlations in a distorted crystal lattice often leads to the evolution of novel emergent functionalities in the strongly correlated materials (SCM). Here, we unravel such unprecedented commensurate (COM) and incommensurate (ICOM) charge ordered (CO) phases at room temperature in a simple transition-metal mono-oxide, namely CoO. The electron diffraction pattern unveils a COM ( $$q_{1}$$ q 1 = $$\frac{1}{2}(1,1,{\bar{1}})$$ 1 2 ( 1 , 1 , 1 ¯ ) and ICOM ( $$q_{2}=0.213(1,1,{\bar{1}})$$ q 2 = 0.213 ( 1 , 1 , 1 ¯ ) ) periodic lattice distortion. Transmission electron microscopy (TEM) captures unidirectional and bidirectional stripe patterns of charge density modulations. The widespread phase singularities in the phase-field of the order parameter (OP) affirms the abundant topological disorder. Using, density functional theory (DFT) calculations, we demystify the underlying electronic mechanism. The DFT study shows that a cation disordering ( $$\mathrm {Co}_{1-\textit{x}}\mathrm {O}, \text {with }{} \textit{x} = 4.17 \%$$ Co 1 - x O , with x = 4.17 % ) stabilizes Jahn-Teller (JT) distortion and localized aliovalent $$\mathrm {Co}^{3+}$$ Co 3 + states in CoO. Therefore, the lattice distortion accompanied with mixed valence states ( $$\mathrm {Co}^{3+}, \mathrm {Co}^{2+}$$ Co 3 + , Co 2 + ) states introduces CO in CoO. Our findings offer an electronic paradigm to engineer CO to exploit the associated electronic functionalities in widely available transition-metal mono-oxides.https://doi.org/10.1038/s41598-021-98739-6
spellingShingle Devendra Negi
Deobrat Singh
Rajeev Ahuja
Peter A. van Aken
Coexisting commensurate and incommensurate charge ordered phases in CoO
Scientific Reports
title Coexisting commensurate and incommensurate charge ordered phases in CoO
title_full Coexisting commensurate and incommensurate charge ordered phases in CoO
title_fullStr Coexisting commensurate and incommensurate charge ordered phases in CoO
title_full_unstemmed Coexisting commensurate and incommensurate charge ordered phases in CoO
title_short Coexisting commensurate and incommensurate charge ordered phases in CoO
title_sort coexisting commensurate and incommensurate charge ordered phases in coo
url https://doi.org/10.1038/s41598-021-98739-6
work_keys_str_mv AT devendranegi coexistingcommensurateandincommensuratechargeorderedphasesincoo
AT deobratsingh coexistingcommensurateandincommensuratechargeorderedphasesincoo
AT rajeevahuja coexistingcommensurateandincommensuratechargeorderedphasesincoo
AT peteravanaken coexistingcommensurateandincommensuratechargeorderedphasesincoo