Strain Mapping and Phase Evolution in Single Palladium Nanoparticles During Electrochemical Hydrogen Absorption
Frédéric Maillard a, Clément Atlan a b c, Corentin Chatelier b c, Apinya Ngoipala d, Kyle Olson a b c, Arnaud Viola a, Ewen Bellec b c, Michael Grimes b c, Minaam Qamar e, Matous Mrovec e, Steven Leake c, Tobias Schülli c, Joël Eymery b, Matthias Vandichel d, Marie-Ingrid Richard b c
a Univ. Grenoble Alpes, Univ. Savoie Mont Blanc, CNRS, Grenoble INP, LEPMI, 38000, Grenoble, France, Rue de la Piscine, 113, Saint-Martin-d'Hères, France
b Univ. Grenoble Alpes, CEA, IRIG-MEM, 38000 Grenoble, France
c ESRF - The European Synchrotron, Avenue des Martyrs, 71, Grenoble, France
d School of Chemical Sciences and Chemical Engineering, Bernal Institute, University of Limerick, Limerick, V94 T9PX Ireland
e Interdisciplinary Centre for Advanced Materials Simulation (ICAMS), Ruhr-Universität Bochum, Bochum, 44780 Germany
Proceedings of MATSUS Fall 2025 Conference (MATSUSFall25)
E3 ElectroCATalyst in action: REAl-time Characterization Techniques - #EcatReact
València, Spain, 2025 October 20th - 24th
Organizers: Kavita Kumar and Angus Pedersen
Invited Speaker, Frédéric Maillard, presentation 072
Publication date: 21st July 2025

Palladium hydrides (PdHx) are a model system for studying phase transitions and hydrogen (H) absorption in materials. Well-studied in the gas phase, they are also relevant in electrochemistry, particularly electrocatalysis, where the H:Pd ratio can be controlled though electrochemical potential. PdHx hydrides exhibit a slightly expanded lattice at low H content (x < 0.05), known as the α-phase, which transforms into a lattice-expanded β-phase at higher H content. While wide-angle X-ray scattering can be used to monitor the in situ absorption of H into commercial Pd nanoparticles (NPs) 3.6 nm in size [1] as well as related phenomena such as H trapping, crucial aspects of the mechanism and kinetics of PdHx formation remain elusive. Specifically, it is unclear whether the α- and β-phases coexist, and if the Pd NPs undergo isotropic H insertion, following a core-shell model, or if preferential H absorption pathways exist, as suggested by a spherical cap model. Furthermore, the small size of the facets makes it difficult to determine the distribution of strain fields across single NP.

In this study, employing Bragg Coherent X-ray Diffraction Imaging (BCDI) and focusing on the 111 Bragg reflection, we obtained information on the morphology, projected strain, displacement fields, and d-spacing of single 300 nm Pd NPs at various electrode potentials relevant to H adsorption, H absorption, and H2 evolution [2]. We examined changes in lattice constants for both α and β phases and reconstructed individual Pd NPs in each individual phase. The reconstructions revealed a continuous increase in the Pd lattice parameter, indicating an isotropic expansion of the NP. Additionally, we observed heterogeneous strain in the reconstructed Pd NPs, with tensile strain accumulating on the {111} and {100} facets, while the lattice in the edges and corners of the atoms appeared compressed. Finally, we will show how BCDI can be used to gain insights into H absorption/desorption mechanism and kinetics.

Figure 1. Diagram showing the in situ cell used to reconstruct a single nanoparticle in 3D under potential control from diffraction images.

This project has received funding from the European Union’s Horizon 2020 research and innovation program under grant agreement HERMES No. 952184 and grant agreement CARINE No. 818823.

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