Charge-transfer properties and electron dynamics in ferromagnetic <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi>CoS</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:math>

We investigated the element-specific electronic structure and charge-carrier dynamics of a single-crystal ferromagnet <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:msub><a:mi>CoS</a:mi><a:mn>2</a:mn></a:msub></a:math> with complementary x-ray spectroscopy techniques. Hard x-ray photoemission (HAXPES) is used to provide crucial information on the bulk electronic structure and chemical bonding in <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:msub><b:mi>CoS</b:mi><b:mn>2</b:mn></b:msub></b:math> that is compared against the isoelectronic paramagnet <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:msub><c:mi>CoSe</c:mi><c:mn>2</c:mn></c:msub></c:math>. The Co <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"><d:mrow><d:mn>1</d:mn><d:mi>s</d:mi></d:mrow></d:math> core-level line shows several satellite features for <e:math xmlns:e="http://www.w3.org/1998/Math/MathML"><e:msub><e:mi>CoS</e:mi><e:mn>2</e:mn></e:msub></e:math>, showing explicit charge-transfer processes and local screening of the core hole by S ligands, whereas no such features are observed in <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"><f:msub><f:mi>CoSe</f:mi><f:mn>2</f:mn></f:msub></f:math>. The satellite structures indicate the electronic configuration of divalent <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"><g:msup><g:mrow><g:mi>Co</g:mi></g:mrow><g:mrow><g:mn>2</g:mn><g:mo>+</g:mo></g:mrow></g:msup></g:math> as a combination of <h:math xmlns:h="http://www.w3.org/1998/Math/MathML"><h:mrow><h:msup><h:mi>d</h:mi><h:mn>8</h:mn></h:msup><h:mi mathvariant="normal">Ḻ</h:mi></h:mrow></h:math> and <j:math xmlns:j="http://www.w3.org/1998/Math/MathML"><j:mrow><j:msup><j:mi>d</j:mi><j:mn>9</j:mn></j:msup><j:msup><j:mi mathvariant="normal">Ḻ</j:mi><j:mn>2</j:mn></j:msup></j:mrow></j:math> in addition to the nominal ionic <l:math xmlns:l="http://www.w3.org/1998/Math/MathML"><l:msup><l:mrow><l:mi>d</l:mi></l:mrow><l:mn>7</l:mn></l:msup></l:math> state, where <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"><m:mi mathvariant="normal">Ḻ</m:mi></m:math> represents an S <o:math xmlns:o="http://www.w3.org/1998/Math/MathML"><o:mrow><o:mn>3</o:mn><o:mi>p</o:mi></o:mrow></o:math> hole. We employ resonant Auger spectroscopy across the S <p:math xmlns:p="http://www.w3.org/1998/Math/MathML"><p:mi>K</p:mi></p:math>-edge for <q:math xmlns:q="http://www.w3.org/1998/Math/MathML"><q:msub><q:mi>CoS</q:mi><q:mn>2</q:mn></q:msub></q:math> to obtain electron delocalization times to adjacent Co atomic sites. The fast carrier dynamics are attributed to strongly screened Coulomb interactions and hence a facile carrier delocalization. The strong hybridization formed between the Co <r:math xmlns:r="http://www.w3.org/1998/Math/MathML"><r:mrow><r:mn>3</r:mn><r:mi>d</r:mi></r:mrow></r:math> and S <s:math xmlns:s="http://www.w3.org/1998/Math/MathML"><s:mrow><s:mn>3</s:mn><s:mi>p</s:mi></s:mrow></s:math> states with pronounced charge-transfer character reflects a self-doped system with a finite density <t:math xmlns:t="http://www.w3.org/1998/Math/MathML"><t:mi>n</t:mi></t:math> of holes at the sulfur site (<u:math xmlns:u="http://www.w3.org/1998/Math/MathML"><u:msup><u:mi mathvariant="normal">Ḻ</u:mi><u:mi>n</u:mi></u:msup></u:math>), in line with recent models that indicate a negative charge-transfer energy for <w:math xmlns:w="http://www.w3.org/1998/Math/MathML"><w:msub><w:mi>CoS</w:mi><w:mn>2</w:mn></w:msub></w:math>. In addition to HAXPES data, we also report on experimental and theoretical <x:math xmlns:x="http://www.w3.org/1998/Math/MathML"><x:mi>L</x:mi></x:math>-edge x-ray absorption and x-ray magnetic circular dichroism data for <y:math xmlns:y="http://www.w3.org/1998/Math/MathML"><y:msub><y:mi>CoS</y:mi><y:mn>2</y:mn></y:msub></y:math> that demonstrate multiconfiguration effects in the excitation process. To enable a direct comparison of the experimental spectra, we used density functional theory calculations to obtain the projected density of states to describe the ground-state electronic structure. The existence of fast carrier dynamics and strong charge-transfer properties, demonstrated in this study, highlights the unique nature of <z:math xmlns:z="http://www.w3.org/1998/Math/MathML"><z:msub><z:mi>CoS</z:mi><z:mn>2</z:mn></z:msub></z:math> with a wide potential in topological spintronics applications and integration in energy-related device platforms.

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Journal
Physical review. B./Physical review. B
Published
2025-10-14
DOI
https://doi.org/10.1103/vg4c-h785
Citations
1
Primary Topic
Heusler alloys: electronic and magnetic properties
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article
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article

Charge-transfer properties and electron dynamics in ferromagnetic <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi>CoS</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:math>

Anna Delin, Å. Edström, Fredrik O. L. Johansson, Martin Pavelka et al.
1 citations
Physical review. B./Physical review. B
Heusler alloys: electronic and magnetic properties
0.43
article

Charge-transfer properties and electron dynamics in ferromagnetic <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi>CoS</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:math>

Anna Delin, Å. Edström, Fredrik O. L. Johansson, Martin Pavelka, Anirudha Ghosh, Anwesha Chakraborty, Mahmoud Abdel‐Hafiez, Dibya Phuyal, Debjani Karmakar, Olle Eriksson, A. N. Vasiliev, Д. А. Чареев
article en
1 citations

Abstract

We investigated the element-specific electronic structure and charge-carrier dynamics of a single-crystal ferromagnet <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:msub><a:mi>CoS</a:mi><a:mn>2</a:mn></a:msub></a:math> with complementary x-ray spectroscopy techniques. Hard x-ray photoemission (HAXPES) is used to provide crucial information on the bulk electronic structure and chemical bonding in <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:msub><b:mi>CoS</b:mi><b:mn>2</b:mn></b:msub></b:math> that is compared against the isoelectronic paramagnet <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:msub><c:mi>CoSe</c:mi><c:mn>2</c:mn></c:msub></c:math>. The Co <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"><d:mrow><d:mn>1</d:mn><d:mi>s</d:mi></d:mrow></d:math> core-level line shows several satellite features for <e:math xmlns:e="http://www.w3.org/1998/Math/MathML"><e:msub><e:mi>CoS</e:mi><e:mn>2</e:mn></e:msub></e:math>, showing explicit charge-transfer processes and local screening of the core hole by S ligands, whereas no such features are observed in <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"><f:msub><f:mi>CoSe</f:mi><f:mn>2</f:mn></f:msub></f:math>. The satellite structures indicate the electronic configuration of divalent <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"><g:msup><g:mrow><g:mi>Co</g:mi></g:mrow><g:mrow><g:mn>2</g:mn><g:mo>+</g:mo></g:mrow></g:msup></g:math> as a combination of <h:math xmlns:h="http://www.w3.org/1998/Math/MathML"><h:mrow><h:msup><h:mi>d</h:mi><h:mn>8</h:mn></h:msup><h:mi mathvariant="normal">Ḻ</h:mi></h:mrow></h:math> and <j:math xmlns:j="http://www.w3.org/1998/Math/MathML"><j:mrow><j:msup><j:mi>d</j:mi><j:mn>9</j:mn></j:msup><j:msup><j:mi mathvariant="normal">Ḻ</j:mi><j:mn>2</j:mn></j:msup></j:mrow></j:math> in addition to the nominal ionic <l:math xmlns:l="http://www.w3.org/1998/Math/MathML"><l:msup><l:mrow><l:mi>d</l:mi></l:mrow><l:mn>7</l:mn></l:msup></l:math> state, where <m:math xmlns:m="http://www.w3.org/1998/Math/MathML"><m:mi mathvariant="normal">Ḻ</m:mi></m:math> represents an S <o:math xmlns:o="http://www.w3.org/1998/Math/MathML"><o:mrow><o:mn>3</o:mn><o:mi>p</o:mi></o:mrow></o:math> hole. We employ resonant Auger spectroscopy across the S <p:math xmlns:p="http://www.w3.org/1998/Math/MathML"><p:mi>K</p:mi></p:math>-edge for <q:math xmlns:q="http://www.w3.org/1998/Math/MathML"><q:msub><q:mi>CoS</q:mi><q:mn>2</q:mn></q:msub></q:math> to obtain electron delocalization times to adjacent Co atomic sites. The fast carrier dynamics are attributed to strongly screened Coulomb interactions and hence a facile carrier delocalization. The strong hybridization formed between the Co <r:math xmlns:r="http://www.w3.org/1998/Math/MathML"><r:mrow><r:mn>3</r:mn><r:mi>d</r:mi></r:mrow></r:math> and S <s:math xmlns:s="http://www.w3.org/1998/Math/MathML"><s:mrow><s:mn>3</s:mn><s:mi>p</s:mi></s:mrow></s:math> states with pronounced charge-transfer character reflects a self-doped system with a finite density <t:math xmlns:t="http://www.w3.org/1998/Math/MathML"><t:mi>n</t:mi></t:math> of holes at the sulfur site (<u:math xmlns:u="http://www.w3.org/1998/Math/MathML"><u:msup><u:mi mathvariant="normal">Ḻ</u:mi><u:mi>n</u:mi></u:msup></u:math>), in line with recent models that indicate a negative charge-transfer energy for <w:math xmlns:w="http://www.w3.org/1998/Math/MathML"><w:msub><w:mi>CoS</w:mi><w:mn>2</w:mn></w:msub></w:math>. In addition to HAXPES data, we also report on experimental and theoretical <x:math xmlns:x="http://www.w3.org/1998/Math/MathML"><x:mi>L</x:mi></x:math>-edge x-ray absorption and x-ray magnetic circular dichroism data for <y:math xmlns:y="http://www.w3.org/1998/Math/MathML"><y:msub><y:mi>CoS</y:mi><y:mn>2</y:mn></y:msub></y:math> that demonstrate multiconfiguration effects in the excitation process. To enable a direct comparison of the experimental spectra, we used density functional theory calculations to obtain the projected density of states to describe the ground-state electronic structure. The existence of fast carrier dynamics and strong charge-transfer properties, demonstrated in this study, highlights the unique nature of <z:math xmlns:z="http://www.w3.org/1998/Math/MathML"><z:msub><z:mi>CoS</z:mi><z:mn>2</z:mn></z:msub></z:math> with a wide potential in topological spintronics applications and integration in energy-related device platforms.

Physical review. B./Physical review. BVol. 112(16)
Uppsala University (SE), Ural Federal University (RU), Bhabha Atomic Research Centre (IN), University of Potsdam (DE), Lomonosov Moscow State University (RU), Homi Bhabha National Institute (IN), Helmholtz-Zentrum Berlin für Materialien und Energie (DE), University of Sharjah (AE), Institute of Experimental Mineralogy (RU), Swedish e-Science Research Centre (SE), MAX IV Laboratory (SE), Moscow State University (TJ), Fayoum University (EG), KTH Royal Institute of Technology (SE)
Openalex Percentile: Top 35%
Heusler alloys: electronic and magnetic properties
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