Selective Orbital Imaging of Excited States with X-Ray Spectroscopy: The Example of α-MnS
Herein we show that nonresonant inelastic x-ray scattering involving an s core level is a powerful spectroscopic method to characterize the excited states of transition metal compounds. The spherical charge distribution of the s core hole allows the orientational dependence of the intensities of the...
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2021-01-01
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Series: | Physical Review X |
Online Access: | http://doi.org/10.1103/PhysRevX.11.011002 |
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doaj-8119911786f34b4d8523ba51bc156e652021-02-12T00:12:25ZengAmerican Physical SocietyPhysical Review X2160-33082021-01-0111101100210.1103/PhysRevX.11.011002Selective Orbital Imaging of Excited States with X-Ray Spectroscopy: The Example of α-MnSA. AmoreseB. LeedahlM. SundermannH. GretarssonZ. HuH.-J. LinC. T. ChenM. SchmidtH. BorrmannYu. GrinA. SeveringM. W. HaverkortL. H. TjengHerein we show that nonresonant inelastic x-ray scattering involving an s core level is a powerful spectroscopic method to characterize the excited states of transition metal compounds. The spherical charge distribution of the s core hole allows the orientational dependence of the intensities of the various spectral features to produce a spatial charge image of the associated multiplet states in a straightforward manner, thereby facilitating the identification of their orbital character. In addition, the s core hole does not add an extra orbital angular momentum component to the multiplet structure so that the well-established Sugano-Tanabe-Kamimura diagrams can be used for the analysis of the spectra. For α-MnS we observe the spherical charge density corresponding to its high-spin 3d^{5} (^{6}A_{1}) ground state configuration and we were able to selectively image its excited states and identify them as t_{2g} (^{5}T_{2}) and e_{g} (^{5}E) with an energy splitting 10Dq of 0.78 eV.http://doi.org/10.1103/PhysRevX.11.011002 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
A. Amorese B. Leedahl M. Sundermann H. Gretarsson Z. Hu H.-J. Lin C. T. Chen M. Schmidt H. Borrmann Yu. Grin A. Severing M. W. Haverkort L. H. Tjeng |
spellingShingle |
A. Amorese B. Leedahl M. Sundermann H. Gretarsson Z. Hu H.-J. Lin C. T. Chen M. Schmidt H. Borrmann Yu. Grin A. Severing M. W. Haverkort L. H. Tjeng Selective Orbital Imaging of Excited States with X-Ray Spectroscopy: The Example of α-MnS Physical Review X |
author_facet |
A. Amorese B. Leedahl M. Sundermann H. Gretarsson Z. Hu H.-J. Lin C. T. Chen M. Schmidt H. Borrmann Yu. Grin A. Severing M. W. Haverkort L. H. Tjeng |
author_sort |
A. Amorese |
title |
Selective Orbital Imaging of Excited States with X-Ray Spectroscopy: The Example of α-MnS |
title_short |
Selective Orbital Imaging of Excited States with X-Ray Spectroscopy: The Example of α-MnS |
title_full |
Selective Orbital Imaging of Excited States with X-Ray Spectroscopy: The Example of α-MnS |
title_fullStr |
Selective Orbital Imaging of Excited States with X-Ray Spectroscopy: The Example of α-MnS |
title_full_unstemmed |
Selective Orbital Imaging of Excited States with X-Ray Spectroscopy: The Example of α-MnS |
title_sort |
selective orbital imaging of excited states with x-ray spectroscopy: the example of α-mns |
publisher |
American Physical Society |
series |
Physical Review X |
issn |
2160-3308 |
publishDate |
2021-01-01 |
description |
Herein we show that nonresonant inelastic x-ray scattering involving an s core level is a powerful spectroscopic method to characterize the excited states of transition metal compounds. The spherical charge distribution of the s core hole allows the orientational dependence of the intensities of the various spectral features to produce a spatial charge image of the associated multiplet states in a straightforward manner, thereby facilitating the identification of their orbital character. In addition, the s core hole does not add an extra orbital angular momentum component to the multiplet structure so that the well-established Sugano-Tanabe-Kamimura diagrams can be used for the analysis of the spectra. For α-MnS we observe the spherical charge density corresponding to its high-spin 3d^{5} (^{6}A_{1}) ground state configuration and we were able to selectively image its excited states and identify them as t_{2g} (^{5}T_{2}) and e_{g} (^{5}E) with an energy splitting 10Dq of 0.78 eV. |
url |
http://doi.org/10.1103/PhysRevX.11.011002 |
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