Doping‐Induced Enhancement of Hydrogen Evolution at MoS<sub>2</sub> Electrodes

Rate theory and DFT calculations of hydrogen evolution reaction (HER) on MoS<sub>2</sub> with Co, Ni and Pt impurities show the significance of dihydrogen (H<sub>2</sub>*) complex where both hydrogen atoms are interacting with the surface. Stabilization of such a complex affects the competing Volmer-Heyrovsky (direct H<sub>2</sub> release) and Volmer-Tafel (H<sub>2</sub>* intermediate) pathways. The resulting evolution proceeds with a very small overpotential for all dopants ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:semantics><mml:mi>η</mml:mi> <mml:annotation>${\eta }$</mml:annotation> </mml:semantics> </mml:math> =0.1 to 0.2 V) at 25 % edge substitution, significantly reduced from the already low <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:semantics><mml:mi>η</mml:mi> <mml:annotation>${\eta }$</mml:annotation> </mml:semantics> </mml:math> =0.27 V for the undoped edge. At full edge substitution, Co-MoS<sub>2</sub> remains highly active ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:semantics><mml:mi>η</mml:mi> <mml:annotation>${\eta }$</mml:annotation> </mml:semantics> </mml:math> =0.18 V) while Ni- and Pt-MoS<sub>2</sub> are deactivated ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:semantics><mml:mi>η</mml:mi> <mml:annotation>${\eta }$</mml:annotation> </mml:semantics> </mml:math> =0.4 to 0.5 V) due to unfavorable interaction with H<sub>2</sub>*. Instead of the single S-vacancy, the site of intrinsic activity in the basal plane was found to be the undercoordinated central Mo-atom in threefold S-vacancy configurations, enabling hydrogen evolution with <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:semantics><mml:mi>η</mml:mi> <mml:annotation>${\eta }$</mml:annotation> </mml:semantics> </mml:math> =0.52 V via a H<sub>2</sub>* intermediate. The impurity atoms interact favorably with the intrinsic sulfur vacancies on the basal plane, stabilizing but simultaneously deactivating the triple vacancy configuration. The calculated shifts in overpotential are consistent with reported measurements, and the dependence on doping level may explain variations in experimental observations.

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Journal
ChemPhysChem
Published
2024-08-23
DOI
https://doi.org/10.1002/cphc.202400349
Citations
3
Primary Topic
Electrocatalysts for Energy Conversion
Type
article
Field-Weighted Citation Impact
0.31

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article

Doping‐Induced Enhancement of Hydrogen Evolution at MoS2 Electrodes

Hannes Jónsson, Jaakko Akola, Sander Ø. Hanslin
3 citations
ChemPhysChem
Electrocatalysts for Energy Conversion
0.31
article

Doping‐Induced Enhancement of Hydrogen Evolution at MoS2 Electrodes

Hannes Jónsson, Jaakko Akola, Sander Ø. Hanslin
article en
3 citations

Abstract

Rate theory and DFT calculations of hydrogen evolution reaction (HER) on MoS<sub>2</sub> with Co, Ni and Pt impurities show the significance of dihydrogen (H<sub>2</sub>*) complex where both hydrogen atoms are interacting with the surface. Stabilization of such a complex affects the competing Volmer-Heyrovsky (direct H<sub>2</sub> release) and Volmer-Tafel (H<sub>2</sub>* intermediate) pathways. The resulting evolution proceeds with a very small overpotential for all dopants ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:semantics><mml:mi>η</mml:mi> <mml:annotation>${\eta }$</mml:annotation> </mml:semantics> </mml:math> =0.1 to 0.2 V) at 25 % edge substitution, significantly reduced from the already low <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:semantics><mml:mi>η</mml:mi> <mml:annotation>${\eta }$</mml:annotation> </mml:semantics> </mml:math> =0.27 V for the undoped edge. At full edge substitution, Co-MoS<sub>2</sub> remains highly active ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:semantics><mml:mi>η</mml:mi> <mml:annotation>${\eta }$</mml:annotation> </mml:semantics> </mml:math> =0.18 V) while Ni- and Pt-MoS<sub>2</sub> are deactivated ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:semantics><mml:mi>η</mml:mi> <mml:annotation>${\eta }$</mml:annotation> </mml:semantics> </mml:math> =0.4 to 0.5 V) due to unfavorable interaction with H<sub>2</sub>*. Instead of the single S-vacancy, the site of intrinsic activity in the basal plane was found to be the undercoordinated central Mo-atom in threefold S-vacancy configurations, enabling hydrogen evolution with <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:semantics><mml:mi>η</mml:mi> <mml:annotation>${\eta }$</mml:annotation> </mml:semantics> </mml:math> =0.52 V via a H<sub>2</sub>* intermediate. The impurity atoms interact favorably with the intrinsic sulfur vacancies on the basal plane, stabilizing but simultaneously deactivating the triple vacancy configuration. The calculated shifts in overpotential are consistent with reported measurements, and the dependence on doping level may explain variations in experimental observations.

ChemPhysChemVol. 25(20)
University of Iceland (IS), Tampere University (FI), Norwegian University of Science and Technology (NO)
Academy of Finland
Clean water and sanitation
Openalex Percentile: Top 53%
Electrocatalysts for Energy Conversion
0.31
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