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Published May 21, 2014 | Supplemental Material
Journal Article Open

Dendritic Assembly of Gold Nanoparticles during Fuel-Forming Electrocatalysis

Abstract

We observe the dendritic assembly of alkanethiol-capped gold nanoparticles on a glassy carbon support during electrochemical reduction of protons and CO₂. We find that the primary mechanism by which surfactant-ligated gold nanoparticles lose surface area is by taking a random walk along the support, colliding with their neighbors, and fusing to form dendrites, a type of fractal aggregate. A random walk model reproduces the fractal dimensionality of the dendrites observed experimentally. The rate at which the dendrites form is strongly dependent on the solubility of the surfactant in the electrochemical double layer under the conditions of electrolysis. Since alkanethiolate surfactants reductively desorb at potentials close to the onset of CO₂ reduction, they do not poison the catalytic activity of the gold nanoparticles. Although catalyst mobility is typically thought to be limited for room-temperature electrochemistry, our results demonstrate that nanoparticle mobility is significant under conditions at which they electrochemically catalyze gas evolution, even in the presence of a high surface area carbon and binder. A careful understanding of the electrolyte- and polarization-dependent nanoparticle aggregation kinetics informs strategies for maintaining catalyst dispersion during fuel-forming electrocatalysis.

Additional Information

© 2014 American Chemical Society. Received 14 March 2014. Published online 9 May 2014. Published in issue 21 May 2014. We thank David Grauer for conducting XPS measurements and Virginia Altoe, David Barton, Brandon Beberwyck, Trevor Ewers, Eric Granlund, Kendra Kuhl, Li-Chiang Lin, Matt Lucas, Pete Nickias, Fadekemi Oba, and Rachel Segalman for useful discussions and experimental assistance. This work was supported by the Dow Chemical Co. under contract 20120984. SEM was conducted at the Molecular Foundry, supported by the Office of Science, Basic Energy Sciences, of the U.S. Department of Energy (DOE) under contract DE-AC02-05CH11231. K.M. acknowledges the support of the U.S. DOE Office of Science Graduate Fellowship. Y.S. acknowledges the Miller Institute for Basic Research in Science for a postdoctoral fellowship. A.P.A. was supported by the U.S. DOE under contract DE-AC02-05CH11231. The authors declare no competing financial interest.

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