Oxide perovskites have attracted great interest as materials for energy conversion due to their stability and structural tunability. La-based perovskites of 3d-transition metals have demonstrated excellent activities as electrocatalysts in water oxidation. Herein, we report the synthesis route to La-based perovskites using an environmentally friendly deep eutectic solvent (DES) consisting of choline chloride and malonic acid. The DES route affords phase-pure crystalline materials on a gram scale and results in perovskites with high electrocatalytic activity for oxygen evolution reaction. A convenient, fast, and scalable synthesis proceeds via assisted metathesis at a lower temperature as compared to traditional solid-state methods. Among LaCoO3, LaMn0.5Ni0.5O3, and LaMnO3 perovskites prepared via the DES route, LaCoO3 was established to be the best-performing electrocatalyst for water oxidation in alkaline medium at 0.25 mg cm-2 mass loading. LaCoO3 exhibits current densities of 10, 50, and 100 mA cm-2 at respective overpotentials of approximately 390, 430, and 470 mV, respectively, and features a Tafel slope of 55.8 mV dec-1. The high activity of LaCoO3 as compared to the other prepared perovskites is attributed to the high concentration of oxygen vacancies in the LaCoO3 lattice, as observed by high-resolution transmission electron microscopy. An intrinsically high concentration of O vacancies in the LaCoO3 synthesized via the DES route is ascribed to the reducing atmosphere attained upon thermal decomposition of the DES components. These findings will contribute to the preparation of highly active perovskites for various energy applications.
Oxide perovskites have attracted great interest as materials for energy conversion due to their stability and structural tunability. La-based perovskites of 3d-transition metals have demonstrated excellent activities as electrocatalysts in water oxidation. Herein, we report the synthesis route to La-based perovskites using an environmentally friendly deep eutectic solvent (DES) consisting of choline chloride and malonic acid. The DES route affords phase-pure crystalline materials on a gram scale and results in perovskites with high electrocatalytic activity for oxygen evolution reaction. A convenient, fast, and scalable synthesis proceeds via assisted metathesis at a lower temperature as compared to traditional solid-state methods. Among LaCoO3, LaMn0.5Ni0.5O3, and LaMnO3 perovskites prepared via the DES route, LaCoO3 was established to be the best-performing electrocatalyst for water oxidation in alkaline medium at 0.25 mg cm-2 mass loading. LaCoO3 exhibits current densities of 10, 50, and 100 mA cm-2 at respective overpotentials of approximately 390, 430, and 470 mV, respectively, and features a Tafel slope of 55.8 mV dec-1. The high activity of LaCoO3 as compared to the other prepared perovskites is attributed to the high concentration of oxygen vacancies in the LaCoO3 lattice, as observed by high-resolution transmission electron microscopy. An intrinsically high concentration of O vacancies in the LaCoO3 synthesized via the DES route is ascribed to the reducing atmosphere attained upon thermal decomposition of the DES components. These findings will contribute to the preparation of highly active perovskites for various energy applications.
Perovskites
with a general formula of ABO3± have
attracted great interest for energy-related applications
due to their structural flexibility and stability. Particularly, La-based
perovskites, LaTO3 (T = 3d late-transition metal), have
demonstrated high electrocatalytic activity for oxygen evolution reaction
(OER),[1,2] which is crucial for rechargeable metal–air
batteries as well as water electrolysis. However, overcoming slow
kinetics caused by multi-electron transfer remains a great challenge
and requires a large overpotential.[3]To design a cost-effective and high-performance electrocatalyst
for OER, substantial efforts have been made to understand the reaction
mechanism and ideally to recognize effective activity descriptors.[4−6] Shao-Horn and co-workers have identified several descriptors relevant
to the OER activity of perovskites,[6] namely
the number of d electrons, charge-transfer energy (covalency), and
optimal eg orbital occupancy. Additionally, structural
factors, such as metal–oxygen–metal bond angles, were
found to be relevant. Oxygen vacancies, VO, have also been shown to play a key role in the OER activity of
perovskite oxide catalysts.[7−11]Deep eutectic solvents (DESs) are emerging green solvents
that
are inexpensive, non-toxic, and biodegradable,[12] rendering them interesting media for sustainable synthesis
of functional materials. They can be prepared by mixing a hydrogen-bond
donor and acceptor (typically quaternary ammonium salt choline chloride)
in a desired molar ratio.[13] Due to the
formation of a eutectic, the melting point of the mixture is lowered
as compared to its individual components.We have previously
shown that the DES synthesis route facilitates
the preparation of complex oxides with mixed-valent states of metal
cations,[14,15] giving access to mixed-valent ternary Zn
and Cu vanadates. The reduced metal centers V4+ and Cu+ were found to modify electronic structures and optical properties
of the resultant vanadates. This DES route, giving access to complex
oxides with VO, prompted us to target
green synthesis of perovskite electrocatalysts for alkaline OER.Herein, we present a convenient, scalable, and green DES route
to La-based perovskite oxides, LaTO3 (T = Mn, Mn/Ni, or
Co), comprising dissolution of metal salts and binary metal oxides
in environmentally benign solvents followed by heat treatment under
air. The resultant materials were tested as electrocatalysts for water
oxidation in alkaline medium, and LaCoO3 was found to exhibit
the best catalytic activity among the prepared perovskites. High-resolution
transmission electron microscopy (HRTEM) studies were carried out
to gain insights into the structures, and a plausible reaction mechanism
is discussed.
Results and Discussion
We developed
a green DES synthesis route for LaCoO3,
LaMn0.5Ni0.5O3, and LaMnO3 perovskites due to the expected high electrocatalytic activity of
these materials in alkaline OER.[5,16,17] The DES of choice was a eutectic mixture of malonic acid (mp 135–137
°C) as the hydrogen-bond donor and choline chloride (mp 302 °C)
as the hydrogen-bond acceptor mixed in a 1:1 molar ratio. The resulting
eutectic mixture has a melting point of 10 °C. The binary precursors
manganese oxide Mn2O3 and metal salts (LaCl3, NiCl2, and CoCl2) were dissolved in
this medium at 70 °C. The produced solutions were then calcined
at moderate temperatures of 200–400 °C in an open crucible
under air to remove NH3(g) and HCl(g) side products
stemming from the decomposition of the DES resulting in semi-amorphous
solids. Upon further calcination at 900–1000 °C, the leftover
hydrocarbon was removed via combustion, resulting in the crystallization
of the target perovskites.As determined by powder X-ray diffraction
(PXRD), our DES route
provides phase-pure perovskites LaCoO3, LaMn0.5Ni0.5O3, and LaMnO3 (Figure ). Structural parameters from
Rietveld refinement are summarized in Figure S1 and Table S1.
Figure 1
Collected PXRD and calculated reference patterns of DES-derived
perovskites.
Collected PXRD and calculated reference patterns of DES-derived
perovskites.The PXRD patterns of LaTO3 (T = Mn, Co) indicate a rhombohedral
crystal structure with the space group R3̅c.
TO6 octahedra are slightly tilted, namely rotated about
the threefold rotation axis as compared to a cubic perovskite (Figure S2). The tilt angles (4.697° for
Mn and[18] 5.3565° for Co[19]) are small due to the large ionic radius of
12-coordinated trivalent La.[20] A significantly
larger unit cell volume of LaMnO3 cf. LaCoO3 arises from the greater ionic radius of high-spin Mn3+ cf. Co3+ in the octahedral environment (Table S1).The PXRD pattern of LaMn0.5Ni0.5O3 is indexed in a monoclinic unit cell (P21/c, Figure S3a,b), although
the possibility of a rhombohedral polymorph (R3̅, Figure S3c,d) present as a minor phase cannot
be ruled out due to the similarity of the PXRD patterns. Moreover,
the structural transition from a low-temperature monoclinic phase
to a high-temperature rhombohedral phase occurs at room temperature
according to Blasco and co-workers.[21] Notably,
there are two distinct T–O (T = Mn, Ni) distances: 1.902 Å,
which is typical for Mn4+ in metal oxides and 2.025 Å,
which is characteristic of Ni2+.[21] As a result, the different octahedral environments introduce significant
distortion in the perovskite structure and create two crystallographically
independent B-sites. Neutron diffraction studies have revealed that
there is a site preference for Mn and Ni cations in both polymorphs,
classifying LaMn0.5Ni0.5O3 as a double
perovskite with a nominal formula La2MnNiO6.[21,22]As compared to traditional solid-state synthesis methods,[23,24] the DES methodology reported here provides rapid access to perovskite
materials without the need of intermediate regrinding/reheating efforts
or reaction temperatures >1000 °C. The DES protocol
not
only facilitates homogeneous mixing of metal cations in the solution
but also favors the formation of reactive intermediates. Specifically,
a labile ternary intermediate, LaOCl, was found to form at ≥400
°C (Figure S4), which further reacts
with binary metal oxides (Mn3O4, NiO, or Co3O4) at 900 °C or 1000 °C to form the
respective perovskites. According to the literature, these findings
suggest that our synthesis follows an assisted metathesis reaction
pathway. In particular, Todd and co-workers reported synthesis of
YMnO3 via assisted metathesis.[25,26] The reaction between Mn2O3, YCl3·6H2O, and Li2CO3 can proceed
according toin which
binary oxides react at 600 °C,
or according towhich is an example of metathesis reaction.[25,26] The latter reaction is faster and stabilizes metastable orthorhombic
YMnO3 at a lower temperature of 500 °C because of
reactive ternary intermediates yttrium oxochloride YOCl and lithium
manganese oxide LiMnO2.[25,26] Considering
that our DES route does not require multiple grinding steps or reheating
at elevated temperatures, we conclusively prove that LaOCl is a kinetically
labile intermediate in the DES synthesis of La-based perovskite oxides
(Figure S4), similar to the assisted metathesis
reaction pathway in the reported synthesis of YMnO3.Next, we investigated the electrocatalytic activity of the newly
synthesized perovskites in alkaline OER. To facilitate the preparation
of the electrocatalytic inks and to increase the surface area for
improved OER activity, the materials were ball-milled into fine powders.
Notably, the ball-milling process does not result in structural changes
in the materials but slightly decreases the average crystallite size
(Table S2) and induces strain. The ball-milled
perovskites were then formulated as inks in ethanol-containing conductive
Nafion ionomer as a binder,[27] and the ink
was deposited onto the Ni foam current collector. More details on
the anode fabrication and electrochemical testing can be found in
the Supporting Information. Experimentally,
the perovskites were found to demonstrate the best OER properties
at 0.25 mg cm–2 mass loading (Figure S5). In addition, the perovskites required prolonged
activation via cyclic voltammetry (CV) for about 700 cycles to achieve
steady-state conditions (Figure S6), after
which the materials exhibit constant OER performance.Figure and Table S3 summarize the electrochemical water
oxidation properties in 1.0 M NaOH of DES-synthesized, ball-milled
LaCoO3, LaMn0.5Ni0.5O3, and LaMnO3 electrocatalysts supported on Ni foam, in
comparison with the standard reference IrO2 electrocatalyst
supported on Ni foam as well as pure Ni foam. High electrocatalytic
performance was observed for all prepared electrocatalysts (Figure a). LaCoO3 affords the most favorable apparent OER properties based on the
geometric area, with current densities j of 10, 50,
and 100 mA cm–2 reached at overpotentials η
of around 390 (η10), 430 (η50),
and 470 (η100) mV, respectively (Table S3). Notably, both Mn-containing perovskites, LaMnO3 and LaMn0.5Ni0.5O3, have
comparable OER properties, while exhibiting higher OER overpotentials
as compared to the best-performing LaCoO3 electrocatalyst
(Figure a, Table S3). The shallow Tafel slope b = 55.8 mV dec–1 was estimated for LaCoO3, while LaMnO3 and LaMn0.5Ni0.5O3 demonstrate slightly higher values of b =
65.8 mV dec–1 and b = 60.3 mV dec–1, respectively (Figure b, Table S3).
Figure 2
Anodic polarization
curves (a), Tafel (b), Nyquist (c), and chronopotentiometric
(d) plots for Ni foam-supported perovskites and reference IrO2, all recorded in 1 M NaOH at room temperature with a mass
loading of 0.25 mg cm–2. The inset in (c) shows
an equivalent electrical circuit model used to fit the Nyquist plots.
Anodic polarization
curves (a), Tafel (b), Nyquist (c), and chronopotentiometric
(d) plots for Ni foam-supported perovskites and reference IrO2, all recorded in 1 M NaOH at room temperature with a mass
loading of 0.25 mg cm–2. The inset in (c) shows
an equivalent electrical circuit model used to fit the Nyquist plots.Notably, significant capacitive currents were observed
for perovskites
between approximately 1.40 and 1.55 V in Figure a, which could be indicative of a variation
in the electrochemically active surface area (ECSA) of the electrocatalysts.
To investigate how the intrinsic OER activities of LaCoO3, LaMn0.5Ni0.5O3, and LaMnO3 materials compare, the activity data in Figure a were normalized to the measured
double-layer capacitance Cdl (Figure S7, Table S3). Assuming that all the perovskites
have a similar specific capacitance, Cp, and neglecting the contribution of cation intercalation into the
material, ECSA can be inferred to be proportional to Cdl. From the resultant normalized data shown in Figure S8, one can conclude that the intrinsic
activity of LaCoO3 (per unit ECSA) is higher than that
of LaMn0.5Ni0.5O3 and LaMnO3, and thus, its better performance is not simply related to its higher
ECSA.To gain insights into the OER kinetics assuming aqueous
electrochemical
assembly,[28] electrochemical impedance spectroscopy
experiments were carried out on a stable electrocatalytic system at
≈η10, as illustrated by the Nyquist plots
(Figure c). Experimental
data were fitted using an equivalent circuit model (Figure c, inset) accounting for a
resistor, which is in series with parallel combination of a resistor
and a constant phase element. Specifically, the resistor Rs is the Ohmic resistance from the electrolyte and all
contacts. The time constant R1–CPE1
is associated with the interfacial resistance from electron transport
between the electrocatalyst and Ni foam current collector, while the
time constant Rct–CPE2 is the charge-transfer resistance (Rct) at the catalyst–electrolyte interface.[29] Importantly, shallow Rct values typically reflect faster charge-transfer
kinetics.[29] The analysis of the obtained
semi-circles (Figure c) as well as derived parameters (Table S3) reveals fastest charge-transfer kinetics over the anode/electrolyte
interface in the case of Ni foam-supported LaCoO3, as reflected
by its smallest Rct = 2.1692 Ω,
compared to Ni foam-supported LaMn0.5Ni0.5O3 (Rct = 2.6762 Ω) and LaMnO3 (Rct = 2.7260 Ω).Interestingly, we observed that the CV curves of the perovskites
feature pre-oxidation peaks at potentials lower than their respective
OER onsets (Figures a, S5, and S6). The trend of the pre-oxidation
peak potential, LaCoO3 (1.51 V) > LaMnO3 ≈
LaMn0.5Ni0.5O3 (1.48 V), agrees well
with that of charge-transfer resistance Rct, LaCoO3 < LaMnO3 ≈ LaMn0.5Ni0.5O3 (Table S3). These observed pre-oxidation peaks are characteristic of Co3+/Co4+ and Mn3+/Mn4+ redox
couples in the respective perovskites, indicating oxidation of the
electrocatalysts during alkaline OER.Having established that
LaCoO3 demonstrates excellent
OER properties, we further investigated if this electrocatalyst can
generate a stable current during alkaline OER. To this end, the anode
was subjected to continuous stability testing by means of chronopotentiometry,
where LaCoO3 showed excellent long-term stability in 1
M NaOH electrolyte during the tested 100 h, affording reasonably steady
current density j of 10 and 100 mA cm–2 at overpotentials η of only ≈390 and 450 mV, respectively
(Figure d).The activity and stability of the synthesized perovskite electrocatalysts
were also compared to the standard platinum group metal reference
IrO2 electrocatalyst at the same mass loading of 0.25 mg
cm–2 (Figure ). Despite possible differences in the surface area between
LaCoO3 and IrO2, the perovskite can be deduced
to offer at least comparable OER properties to the significantly more
expensive and less abundant reference electrocatalyst. Overall, the
low OER overpotential, shallow Tafel slope, fast kinetics, and stable
long-term performance of DES-synthesized LaCoO3 (Figure , Table S3) highlight the potential of this material in electrolysis
applications.To rationalize the observed excellent activity
and stability of
our LaCoO3 in alkaline water oxidation, we carried out
detailed electron microscopy investigations of the material before
and after electrocatalytic testing. Figure S9 shows a representative z-contrast high-angle annular
dark-field scanning transmission electron microscopy (HAADF–STEM)
image of the sample after ball milling but before OER, together with
the corresponding energy-dispersive X-ray spectroscopy mapping in
the STEM mode (STEM–EDX). These images indicate that La, Co,
and O elements are uniformly distributed across the sub-μm-sized
LaCoO3 particles. Notably, neither N nor Cl elements are
present in the as-synthesized LaCoO3, confirming that DES
constituents are eliminated during combustion reaction. This contrasts
with the recent report about N doping into O sites in LaCoO3 prepared by annealing of the pristine oxide powder in the atmosphere
of ammonia gas.[30]Interestingly,
high-resolution HAADF–STEM and selected area
electron diffraction (SAED) analyses of LaCoO3 before OER
evidence the existence of a large number of oxygen vacancies, VO, in the sample (Figure ) clearly manifested in the HAADF–STEM
images by the presence of dark stripes in the Co–O layers. VO are also highlighted by the appearance of
weak superstructure spots in the respective SAED patterns, which are
attributed to the ordering of the dark stripes. The measurement of
the interlayer distances revealed the expansion of the La–La
distance from a typical 0.38 to 0.46 nm in the VO stripe. Both the appearance of dark contrast Co–O
layers and the increase in La–La distances can be attributed
to VO layers, as has been previously observed
in perovskite structures.[31−33] Such layers of VO change Co coordination from CoO6 octahedral
to CoO5 square pyramidal. The formation of VO in the DES-synthesized perovskites is consistent with
our previous studies,[14,15] where we used a DES route to
prepare mixed-valent ternary Zn and Cu vanadates (M2V2O7– and MV2O6–, M = Zn or Cu) and found annealing the reaction mixture to
intrinsically introduce VO.
Figure 3
Top panel:
representative [010] HAADF–STEM images of LaCoO3 after ball milling together with the corresponding SAED patterns
(insets) evidencing dark stripes of VO. White arrows in the magnified selection of the SAED pattern (right
top panel inset) indicate superstructure spots. Bottom panel: magnified
HRTEM image with an overlaid structural model and intensity line scan
profile showing periodic change of La–La distances from typical
0.38 nm to expanded 0.46 nm in VO stripes.
Top panel:
representative [010] HAADF–STEM images of LaCoO3 after ball milling together with the corresponding SAED patterns
(insets) evidencing dark stripes of VO. White arrows in the magnified selection of the SAED pattern (right
top panel inset) indicate superstructure spots. Bottom panel: magnified
HRTEM image with an overlaid structural model and intensity line scan
profile showing periodic change of La–La distances from typical
0.38 nm to expanded 0.46 nm in VO stripes.Remarkably, to the best of our knowledge, there
are no studies
reporting the formation of VO in bulk
LaCoO3 prepared without doping of metal sites or any post-treatment
under reducing conditions, and so far, such examples have only been
reported in LaCoO3 films.[32,34] Even annealing
of pristine LaCoO3 in the reducing atmosphere of ammonium
gas does not induce the formation of VO, with HAADF–STEM of N-doped LaCoO3 indicating
a regular perovskite structure.[30] Most
notably, transmission electron microscopy (TEM), HAADF–STEM,
and SAED investigations of our LaCoO3 electrocatalyst after
stability testing at a constant current density of 10 mA cm–2 for 100 h (Figure d) clearly indicate that the VO are preserved
in the structure of spent LaCoO3 (Figure ).
Figure 4
Representative low-magnification [110] TEM and
[001] HAADF–STEM
(left panels) as well as high-resolution [001] HAADF–STEM (right
panel) images together with the corresponding SAED patterns (insets)
for LaCoO3 after alkaline OER stability testing at a constant
current density of 10 mA cm–2 for 100 h (Figure d), highlighting
that VO and their ordering have been preserved
in the structure.
Representative low-magnification [110] TEM and
[001] HAADF–STEM
(left panels) as well as high-resolution [001] HAADF–STEM (right
panel) images together with the corresponding SAED patterns (insets)
for LaCoO3 after alkaline OER stability testing at a constant
current density of 10 mA cm–2 for 100 h (Figure d), highlighting
that VO and their ordering have been preserved
in the structure.Interestingly, the high-resolution
HAADF–STEM and SAED study
of the LaMnO3 electrocatalyst with the lower electrocatalytic
activity for OER as compared to LaCoO3 showed no evidence
of VO (Figure ). Typical La–La distances of 0.39
nm were observed in the structure. We hypothesize that such a difference
in the VO formation between LaCoO3 and LaMnO3 can be attributed to the higher reduction
potential of Co3+/Co as compared to Mn3+/Mn,
affording greater stability of the +3 oxidation state for Mn in LaTO3 as compared to Co. Thus, partial reduction under the conditions
of our DES route is more likely to occur in the case of LaCoO3. Similarly, no evidence of VO was found in the case of LaMn0.5Ni0.5O3 (data not shown).
Figure 5
Left panel: Representative HAADF–STEM
images of LaMnO3 after ball milling, together with the
corresponding SAED
pattern (insets), evidencing the absence of VO in the material. White arrows indicate the typical La–La
distances of 0.39 nm. Right panel: HAADF–STEM image with simultaneously
collected STEM–EDX mappings of La, O, Mn, and their mixture,
indicating a homogeneous distribution of all the elements within the
sample.
Left panel: Representative HAADF–STEM
images of LaMnO3 after ball milling, together with the
corresponding SAED
pattern (insets), evidencing the absence of VO in the material. White arrows indicate the typical La–La
distances of 0.39 nm. Right panel: HAADF–STEM image with simultaneously
collected STEM–EDX mappings of La, O, Mn, and their mixture,
indicating a homogeneous distribution of all the elements within the
sample.For the LaCoO3 catalyst
reported herein, a plausible
electrocatalytic mode of action is consistent with lattice OER (LOER).[4,5] Although OER over perovskites or other oxides can proceed via a
conventional four-consecutive proton-coupled electron transfer mechanism
with metal cations as the catalytically active sites,[35] examples of alternative or simultaneously occurring LOER
mechanisms are increasingly reported in the literature.[36] In LOER, the oxidation of the lattice oxygen
of the electrocatalyst is accompanied by continuous dissolution–redeposition
of metal cations, which leads to O2 evolution.[37] The resultant VO, formed by the evolution of the lattice O, are then compensated
by OH– from the alkaline electrolyte,[38] affording stability to the electrocatalyst and
preventing collapse due to depletion in structural O. Furthermore,
the LOER mechanism has been demonstrated to be closely associated
with the presence of VO in perovskites.
For example, in La1–SrCoO3−δ, the existence of VO accelerates the dissolution of La/Sr via the
LOER mechanism, thus facilitating the in situ reconstruction of the
perovskite surface into a highly active CoO(OH) shell.[39] Accordingly, VO have
proven to be one of the main factors governing the activity of perovskites
in alkaline OER,[40] somewhat similar to
the field of solid oxide fuel cells.[41]In our study, dissolution of the surface La3+ occurs
upon OER, resulting in the segregation of a La- and O-containing phase
next to the well-isolated LaCoO3 particles as indicated
by STEM–EDX analysis (Figure S10) of LaCoO3 after OER stability testing for 100 h (Figure d). This is most
likely La(OH)3, formed by the precipitation of the as-leached
La3+ in NaOH electrolyte solution under anodic oxidation
conditions.[42] The surface of LaCoO3 could then be reconstructed in situ into a tiny Co-rich shell,
perhaps CoO(OH).[39] In our previous studies,
we clearly confirmed the in situ formation of active and stable shells
of Fe, Co, or Ni oxide/oxyhydroxide nanoparticles during OER over
various phosphide and boride pre-catalysts.[43−46] In sharp contrast, the formation
of such a Co oxide/oxyhydroxide shell was not observed by TEM on the
surface of our spent LaCoO3 (Figure ). As such, the process of the formation
of a Co-rich shell over our LaCoO3 may be rather dynamic
owing to the continuous dissolution–redeposition of Co.[39] Furthermore, the thus-formed Co-rich shell is
suggested to deliver O2 through anodic oxidation of lattice
O in LaCoO3. Most notably, the presence of a large number
of VO in LaCoO3 is proposed
to enhance its OER activity via high oxygen diffusivity,[7] thus affording efficient refilling of the evolved
lattice oxygen.[40,47] The fact that VO remain after 100 h of alkaline OER over our LaCoO3 (Figure )
indicates that there is a dynamic equilibrium state between electrolyte–surface–bulk
during OER.[39,40,48] Importantly, inductively coupled plasma optical emission spectroscopy
chemical analysis of the electrolyte after alkaline OER testing did
not reveal any traces of La, Ni, Co, or Mn but merely the presence
of 0.022 ppm of Pt admixture, which, most likely, stems from leaching
of the Pt wire counter electrode.Perovskites featuring oxygen
vacancies have been shown to be highly
active electrocatalysts for alkaline water oxidation. For example,
plasma treatment was used to introduce VO in PrBa0.5Sr0.5Co1.5Fe0.5O5+δ, resulting in highly active catalyst material
with b = 94 mV dec–1.[8] In another study, the four-layered perovskite
La5Ni3CoO13−δ, synthesized
through glycine nitrate combustion, was found to be enriched with
oxygen defects and showed exceptional electrocatalytic OER activity
(b = 35 mV dec–1).[49] Ce-doping of LaCoO3 was found to significantly
increase the concentration of VO as compared
to pristine LaCoO3, with La0.96Ce0.04CoO3−δ synthesized using a microwave/ultrasound-assisted
hydrothermal route (b = 80 mV dec–1), outperforming pure LaCoO3 (b = 124
mV dec–1) in alkaline OER.[9] The herein reported DES synthesis route provides a straightforward
approach to introduce VO in LaCoO3, placing the material with η10 = 390 mV
and b = 55.8 mV dec–1 among the
best of the state-of-the-art perovskite electrocatalysts for alkaline
water oxidation (Figure ).
Figure 6
Comparison between the Tafel slopes as well as overpotentials required
for driving current density of 10 mA cm–2 for our
best-performing electrocatalyst, LaCoO3, and reported state-of-the-art
perovskite electrocatalysts for alkaline water oxidation.[8,9,49−54]
Comparison between the Tafel slopes as well as overpotentials required
for driving current density of 10 mA cm–2 for our
best-performing electrocatalyst, LaCoO3, and reported state-of-the-art
perovskite electrocatalysts for alkaline water oxidation.[8,9,49−54]
Conclusions
In summary, we have
prepared a series of La-containing perovskites
LaTO3 (T = Mn, Mn/Ni, or Co) using an
environmentally friendly DES synthesis route. DES synthesis enables
uniform mixing of metal precursors and the formation of labile intermediates,
while the unique reaction environment achieved upon DES calcination
facilitates formation of oxygen vacancies in the LaCoO3 structure. LaCoO3 was found to be a stable electrocatalyst
with OER activity among the best reported for perovskites. The high
activity was attributed to the presence of a large number of structural
oxygen vacancies as evidenced by electron microscopy. Further studies
that address a deeper understanding of the effect of oxygen vacancies
on OER over DES-derived perovskites, as well as the optimization of
their OER properties via nanostructuring, will be the subjects of
our future research efforts.
Experimental Section
Catalyst
Synthesis
The DES was prepared by mixing malonic
acid and choline chloride in a 1:1 molar ratio. The mixture was heated
in a beaker at 70 °C until it became liquid. Metal precursors
were added to the solvent and dissolved under vigorous stirring at
70 °C (0.7158 g of LaCl3 and 0.2304 g Mn2O3 in 87 g of the solvent for LaMnO3 | 0.5368
g of LaCl3, 0.0865 g Mn2O3, and 0.1418
g NiCl2 in 72.5 g of the solvent for LaMn0.5Ni0.5O3 | 0.6135 g of LaCl3 and 0.3248 g CoCl2 in 80.0
g of the solvent for LaCoO3). Afterward, the metal-precursor-containing
solution was transferred to a porcelain crucible for calcination (7
g of solution in a 30 mL crucible). The heat treatment was performed
in a box-type muffle furnace for all the samples. For all heat treatments,
a heating rate of 10 °C min–1 was used.For the synthesis of LaMnO3 and LaMn0.5Ni0.5O3, the precursor solution was heated at 230
°C for 2 h and then calcined at 900 °C for LaMnO3 or 1000 °C for LaMn0.5Ni0.5O3 in the span of 8.5 h. LaCoO3 was prepared by heating
the precursor solution at 300 °C for 2 h, followed by calcination
at 900 °C for 8.5 h. Calcination was conducted in an open crucible
under the air. Afterward, the samples were cooled to room temperature
by switching off the furnace.
Authors: Christoph Baeumer; Jiang Li; Qiyang Lu; Allen Yu-Lun Liang; Lei Jin; Henrique Perin Martins; Tomáš Duchoň; Maria Glöß; Sabrina M Gericke; Marcus A Wohlgemuth; Margret Giesen; Emily E Penn; Regina Dittmann; Felix Gunkel; Rainer Waser; Michal Bajdich; Slavomír Nemšák; J Tyler Mefford; William C Chueh Journal: Nat Mater Date: 2021-01-11 Impact factor: 43.841
Authors: Benworth B Hansen; Stephanie Spittle; Brian Chen; Derrick Poe; Yong Zhang; Jeffrey M Klein; Alexandre Horton; Laxmi Adhikari; Tamar Zelovich; Brian W Doherty; Burcu Gurkan; Edward J Maginn; Arthur Ragauskas; Mark Dadmun; Thomas A Zawodzinski; Gary A Baker; Mark E Tuckerman; Robert F Savinell; Joshua R Sangoro Journal: Chem Rev Date: 2020-12-14 Impact factor: 60.622
Authors: Dallas K Mann; Junyuan Xu; Natalia E Mordvinova; Vincent Yannello; Yasmine Ziouani; Noelia González-Ballesteros; Juliana P S Sousa; Oleg I Lebedev; Yury V Kolen'ko; Michael Shatruk Journal: Chem Sci Date: 2019-01-23 Impact factor: 9.825