Recently, germanium selenide (GeSe) has emerged as a promising van der Waals semiconductor for photovoltaics, solar light harvesting, and water photoelectrolysis cells. Contrary to previous reports claiming perfect ambient stability based on experiments with techniques without surface sensitivity, here, by means of surface-science investigations and density functional theory, it is demonstrated that actually both: i) the surface of bulk crystals; and ii) atomically thin flakes of GeSe are prone to oxidation, with the formation of self-assembled germanium-oxide skin with sub-nanometric thickness. Surface oxidation leads to the decrease of the bandgap of stoichiometric GeSe and GeSe 1−x , while bandgap energy increases upon surface oxidation of Ge 1−x Se. Remarkably, the formation of a surface oxide skin on GeSe crystals plays a key role in the physicochemical mechanisms ruling photoelectrocatalysis: the underlying van der Waals semiconductor provides electron-hole pairs, while the germanium-oxide skin formed upon oxidation affords the active sites for catalytic reactions. The self-assembled germanium-oxide/germanium-selenide heterostructure with different bandgaps enables the activation of photocatalytic processes by absorption of light of different wavelengths, with inherently superior activity. Finally, it is discovered that, depending on the specific solvent-GeSe interaction, the liquid phase exfoliation of bulk crystals can induce the formation of Se nanowires.
Reduction
of Cu2O by hydrogen is a common preparation
step for heterogeneous catalysts; however, a detailed understanding
of the atomic reaction pathways is still lacking. Here, we investigate
the interaction of atomic hydrogen with the Cu2O(100):(3,0;1,1)
and Cu2O(111):(√3 × √3)R30° surfaces using scanning tunneling microscopy (STM), low-energy
electron diffraction, temperature-programmed desorption (TPD), and
X-ray photoelectron spectroscopy (XPS). The experimental results are
compared to density functional theory simulations. At 300 K, we identify
the most favorable adsorption site on the Cu2O(100) surface:
hydrogen atoms bind to an oxygen site located at the base of the atomic
rows intrinsic to the (3,0;1,1) surface. The resulting hydroxyl group
subsequently migrates to a nearby Cu trimer site. TPD analysis identifies
H2 as the principal desorption product. These observations
imply that H2 is formed through a disproportionation reaction
of surface hydroxyl groups. The interaction of H with the (111) surface
is more complex, including coordination to both Cu+ and
OCUS sites. STM and XPS analyses reveal the formation of
metallic copper clusters on the Cu2O surfaces after cycles
of hydrogen exposure and annealing. The interaction of the Cu clusters
with the substrate is notably different for the two surface terminations
studied: after annealing, the Cu clusters coalesce on the (100) termination,
and the (3,0;1,1) reconstruction is partially recovered. Clusters
formed on the (111) surface are less prone to coalescence, and the
(√3 × √3)R30° reconstruction
was not recovered by heat treatment, indicating a weaker Cu cluster
to support interaction on the (100) surface.
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