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. 2025 Jul;12(25):e2500516.
doi: 10.1002/advs.202500516. Epub 2025 Apr 2.

Active Sites-Enriched Hierarchical Weyl Semimetal WTe2 Nanowire Arrays for Highly Efficient Hydrogen Evolution Reaction

Affiliations

Active Sites-Enriched Hierarchical Weyl Semimetal WTe2 Nanowire Arrays for Highly Efficient Hydrogen Evolution Reaction

Hyeonkyeong Kim et al. Adv Sci (Weinh). 2025 Jul.

Abstract

Weyl semimetal tungsten ditelluride (WTe2), characterized by its high conductivity and robust topological surface state, possesses promising catalytic properties for electrochemical reactions. However, the synthesis of well-defined WTe2 nanostructures has faced challenges, hindering their practical applications. This study introduces a new method for synthesizing Weyl semimetal WTe2 nanowire arrays grown vertically on conductive carbon cloth. Through a selective synthesis process, WTe2 and core-shell semiconductor-semimetal WO3- x-WTe2 nanowires are successfully fabricated via tellurization of WO2.9 nanowires. To gain a comprehensive understanding of the structural, chemical, and catalytic properties of these nanowires, WO2.9 nanowires are gradually converted to WO3- x-WTe2 and WTe2 nanowires. The hierarchical structure of the WTe2 nanowires greatly increases the number of active sites and promotes efficient charge transfer, resulting in exceptional electrochemical catalytic performance. In the hydrogen evolution reaction, WTe2 nanowire arrays exhibit an exceptionally low Tafel slope of 49 mV dec-1, as well as remarkable stability under both high and low current densities. These exceptional properties highlight the potential of WTe2 nanowire arrays as highly effective electrochemical catalysts. It is expected that this facile synthesis approach will pave the way for the fabrication of well-structured Weyl semimetal nanowires, enabling further exploration of their intriguing properties and promising applications.

Keywords: catalysis; core–shell; transition metal dichalcogenide; transition metal oxide; tungsten ditelluride; tungsten oxide; water splitting.

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Conflict of interest statement

The authors declare no conflict of interest.

Figures

Figure 1
Figure 1
a) Schematic of the experimental setup for synthesizing WTe2 NW arrays and core–shell WO3− x –WTe2 NW arrays via a two‐step synthesis process. b) Growth pathways of WO3− x –WTe2 NWs and WTe2 NWs on CC.
Figure 2
Figure 2
a) Optical image of the Au‐deposited CC, WO2.9 NWs/CC, and WTe2 NWs/CC. b,c) Low‐magnification SEM images of WO2.9 NW arrays. d) High‐magnification SEM image of the white square region indicated in (c). e,f) Low‐magnification SEM images of WTe2 NW arrays. g) High‐magnification SEM image of the white square region indicated in (f).
Figure 3
Figure 3
a) XRD patterns and b) Raman spectra of WO2.9 NWs, core–shell WO3− x –WTe2 NWs, and WTe2 NWs. XPS spectra for c) W 4f and d) Te 3d regions of the as‐synthesized NWs.
Figure 4
Figure 4
TEM images, STEM images, and EDS element maps of a,b) WO2.9 NWs, c,d) core–shell WO3− x –WTe2 NWs (tellurization for 30 min), and e,f) WTe2 NWs, respectively. The structures of tungsten oxide compounds. The W─W distances g) between two corner‐sharing [WO6]‐octahedra, h) between two edge‐sharing [WO6]‐octahedra, and i) between a [WO6]‐octahedra and a bipyramidal pentagonal column. j–l) The structures of monoclinic WO3, WO2.9, and WO2.72. W is shown in blue, O in red.
Figure 5
Figure 5
Electrochemical performance of WTe2 NWs and core–shell WO3− x –WTe2 NWs at different tellurization times. a) LSV polarization curves, b) Tafel plots, c) Nyquist plots, and d) correlation between current density and scan rate for the catalysts. e) LSV polarization curves of WTe2 NWs before and after 1500 HER cycles, with the inset showing an SEM image of WTe2 NWs post‐HER. f) Stability test of WTe2 NWs at a current density of 500 mA cm−2.

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