7 research outputs found
Rambutan-Like FeCO<sub>3</sub> Hollow Microspheres: Facile Preparation and Superior Lithium Storage Performances
Rambutan-like FeCO<sub>3</sub> hollow
microspheres were prepared
via a facile and economic one-step hydrothermal method. The structure
and morphology evolution mechanism was disclosed through time-dependent
experiments. After undergoing the symmetric inside-out Ostwald ripening,
the resultants formed microporous/nanoporous constructions composed
of numerous one-dimensional (1D) nanofiber building blocks. Tested
as anode materials of Li-ion batteries, FeCO<sub>3</sub> hollow microspheres
presented attractive electrochemical performances. The capacities
were over 1000 mAh g<sup>–1</sup> for initial charge, ∼880
mAh g<sup>–1</sup> after 100 cycles at 50 mA g<sup>–1</sup>, and ∼710 mAh g<sup>–1</sup> after 200 cycles at 200
mA g<sup>–1</sup>. The 1D nanofiber assembly and hollow interior
endow this material efficient contact with electrolyte, short Li<sup>+</sup> diffusion paths, and sufficient void spaces to accommodate
large volume variation. The cost-efficient FeCO<sub>3</sub> with rationally
designed nanostructures is a promising anode candidate for Li-ion
batteries
Co<sub>2</sub>(OH)<sub>2</sub>CO<sub>3</sub> Nanosheets and CoO Nanonets with Tailored Pore Sizes as Anodes for Lithium Ion Batteries
Co<sub>2</sub>(OH)<sub>2</sub>CO<sub>3</sub> nanosheets were prepared and initially tested as anode materials
for Li ion batteries. Benefiting from hydroxide and carbonate, the
as-prepared sample delivered a high reversible capacity of 800 mAh
g<sup>–1</sup> after 200 cycles at 200 mA g<sup>–1</sup> and long-cycling capability of 400 mAh g<sup>–1</sup> even
at 1 A g<sup>–1</sup>. Annealed in Ar, monoclinic Co<sub>2</sub>(OH)<sub>2</sub>CO<sub>3</sub> nanosheets were transformed into cubic
CoO nanonets with rich pores. The pore size had apparent influence
on the high-rate performances of CoO. CoO with appropriate pore sizes
exhibited greatly enhanced Li storage performances, stable capacity
of 637 mAh g<sup>–1</sup> until 200 cycles at 1 A g<sup>–1</sup>. More importantly, after many fast charge–discharge cycles,
the highly porous nanonets were still maintained. Our results indicate
that Co<sub>2</sub>(OH)<sub>2</sub>CO<sub>3</sub> nanosheets and highly
porous CoO nanonets are both promising candidate anode materials for
high-performance Li ion batteries
Mechanistic Insights into Surface Chemical Interactions between Lithium Polysulfides and Transition Metal Oxides
The
design and development of materials for electrochemical energy storage
and conversion devices requires fundamental understanding of chemical
interactions at electrode/electrolyte interfaces. For Li–S
batteries that hold the promise for outperforming the current generation
of Li ion batteries, the interactions of lithium polysulfide (LPS)
intermediates with the electrode surface strongly influence the efficiency
and cycle life of the sulfur cathode. While metal oxides have been
demonstrated to be useful in trapping LPS, the actual binding modes
of LPS on 3d transition metal oxides and their dependence on the metal
element identity across the periodic table remain poorly understood.
Here, we investigate the chemical interactions between LPS and oxides
of Mn, Fe, Co, and Cu by combining X-ray photoelectron spectroscopy
and density functional theory calculations. We find that Li–O
interactions dominate LPS binding to the oxides (Mn<sub>3</sub>O<sub>4</sub>, Fe<sub>2</sub>O<sub>3</sub>, and Co<sub>3</sub>O<sub>4</sub>), with increasing strength from Mn to Fe to Co. For Co<sub>3</sub>O<sub>4</sub>, LPS binding also involves metal–sulfur interactions.
We also find that the metal oxides exhibit different binding preferences
for different LPS, with Co<sub>3</sub>O<sub>4</sub> binding shorter-chain
LPS more strongly than Mn<sub>3</sub>O<sub>4</sub>. In contrast to
the other oxides, CuO undergoes intense reduction and dissolution
reactions upon interaction with LPS. The reported findings are thus
particularly relevant to the design of LPS/oxide interfaces for high-performance
Li–S batteries
Surface Chemistry in Cobalt Phosphide-Stabilized Lithium–Sulfur Batteries
Chemistry
at the cathode/electrolyte interface plays an important
role for lithium–sulfur batteries in which stable cycling of
the sulfur cathode requires confinement of the lithium polysulfide
intermediates and their fast electrochemical conversion on the electrode
surface. While many materials have been found to be effective for
confining polysulfides, the underlying chemical interactions remain
poorly understood. We report a new and general lithium polysulfide-binding
mechanism enabled by surface oxidation layers of transition-metal
phosphide and chalcogenide materials. We for the first time find that
CoP nanoparticles strongly adsorb polysulfides because their natural
oxidation (forming Co–O–P-like species) activates the
surface Co sites for binding polysulfides via strong Co–S bonding.
With a surface oxidation layer capable of confining polysulfides and
an inner core suitable for conducting electrons, the CoP nanoparticles
are thus a desirable candidate for stabilizing and improving the performance
of sulfur cathodes in lithium–sulfur batteries. We demonstrate
that sulfur electrodes that hold a high mass loading of 7 mg cm<sup>–2</sup> and a high areal capacity of 5.6 mAh cm<sup>–2</sup> can be stably cycled for 200 cycles. We further reveal that this
new surface oxidation-induced polysulfide-binding scheme applies to
a series of transition-metal phosphide and chalcogenide materials
and can explain their stabilizing effects for lithium–sulfur
batteries
Coupled Metal/Oxide Catalysts with Tunable Product Selectivity for Electrocatalytic CO<sub>2</sub> Reduction
One major challenge
to the electrochemical conversion of CO<sub>2</sub> to useful fuels
and chemical products is the lack of efficient catalysts that can
selectively direct the reaction to one desirable product and avoid
the other possible side products. Making use of strong metal/oxide
interactions has recently been demonstrated to be effective in enhancing
electrocatalysis in the liquid phase. Here, we report one of the first
systematic studies on composition-dependent influences of metal/oxide
interactions on electrocatalytic CO<sub>2</sub> reduction, utilizing
Cu/SnO<sub><i>x</i></sub> heterostructured nanoparticles
supported on carbon nanotubes (CNTs) as a model catalyst system. By
adjusting the Cu/Sn ratio in the catalyst material structure, we can
tune the products of the CO<sub>2</sub> electrocatalytic reduction
reaction from hydrocarbon-favorable to CO-selective to formic acid-dominant.
In the Cu-rich regime, SnO<sub><i>x</i></sub> dramatically
alters the catalytic behavior of Cu. The Cu/SnO<sub><i>x</i></sub>–CNT catalyst containing 6.2% of SnO<sub><i>x</i></sub> converts CO<sub>2</sub> to CO with a high faradaic efficiency
(FE) of 89% and a <i>j</i><sub>CO</sub> of 11.3 mA·cm<sup>–2</sup> at −0.99 V versus reversible hydrogen electrode,
in stark contrast to the Cu–CNT catalyst on which ethylene
and methane are the main products for CO<sub>2</sub> reduction. In
the Sn-rich regime, Cu modifies the catalytic properties of SnO<sub><i>x</i></sub>. The Cu/SnO<sub><i>x</i></sub>–CNT catalyst containing 30.2% of SnO<sub><i>x</i></sub> reduces CO<sub>2</sub> to formic acid with an FE of 77% and
a <i>j</i><sub>HCOOH</sub> of 4.0 mA·cm<sup>–2</sup> at −0.99 V, outperforming the SnO<sub><i>x</i></sub>–CNT catalyst which only converts CO<sub>2</sub> to formic
acid in an FE of 48%
Electroreduction of CO<sub>2</sub> Catalyzed by a Heterogenized Zn–Porphyrin Complex with a Redox-Innocent Metal Center
Transition-metal-based
molecular complexes are a class of catalyst
materials for electrochemical CO<sub>2</sub> reduction to CO that
can be rationally designed to deliver high catalytic performance.
One common mechanistic feature of these electrocatalysts developed
thus far is an electrogenerated reduced metal center associated with
catalytic CO<sub>2</sub> reduction. Here we report a heterogenized
zinc–porphyrin complex (zincÂ(II) 5,10,15,20-tetramesitylporphyrin)
as an electrocatalyst that delivers a turnover frequency as high as
14.4 site<sup>–1</sup> s<sup>–1</sup> and a Faradaic
efficiency as high as 95% for CO<sub>2</sub> electroreduction to CO
at −1.7 V vs the standard hydrogen electrode in an organic/water
mixed electrolyte. While the Zn center is critical to the observed
catalysis, in situ and operando X-ray absorption spectroscopic studies
reveal that it is redox-innocent throughout the potential range. Cyclic
voltammetry indicates that the porphyrin ligand may act as a redox
mediator. Chemical reduction of the zinc–porphyrin complex
further confirms that the reduction is ligand-based and the reduced
species can react with CO<sub>2</sub>. This represents the first example
of a transition-metal complex for CO<sub>2</sub> electroreduction
catalysis with its metal center being redox-innocent under working
conditions
Strong Metal–Phosphide Interactions in Core–Shell Geometry for Enhanced Electrocatalysis
Rational
design of multicomponent material structures with strong interfacial
interactions enabling enhanced electrocatalysis represents an attractive
but underdeveloped paradigm for creating better catalysts for important
electrochemical energy conversion reactions. In this work, we report
metal–phosphide core–shell nanostructures as a new model
electrocatalyst material system where the surface electronic states
of the shell phosphide and its interactions with reaction intermediates
can be effectively influenced by the core metal to achieve higher
catalytic activity. The strategy is demonstrated by the design and
synthesis of iron–iron phosphide (Fe@FeP) core–shell nanoparticles on
carbon nanotubes (CNTs) where we find that the electronic interactions
between the metal and the phosphide components increase the binding
strength of hydrogen adatoms toward the optimum. As a consequence,
the Fe@FeP/CNT material exhibits exceptional catalytic activity for
the hydrogen evolution reaction, only requiring overpotentials of
53–110 mV to reach catalytic current densities of 10–100
mA cm<sup>–2</sup>