Myeongjin Kim1, Jinho Park2, Minsoo Kang3, Jin Young Kim4, Seung Woo Lee2. 1. Department of Hydrogen & Renewable Energy, Kyungpook National University, 80 Daehakro, Bukgu, Daegu 41566, Republic of Korea. 2. G. W. Woodruff School of Mechanical Engineering, Georgia Institute of Technology, Atlanta, Georgia 30332, United States. 3. School of Materials Science and Engineering, Georgia Institute of Technology, Atlanta, Georgia 30332, United States. 4. Fuel Cell Research Center, Korea Institute of Science and Technology (KIST), Hwarang-ro 14-gil 5, Seongbuk-gu, Seoul 02792, Republic of Korea.
Abstract
The design of active and stable electrocatalysts for oxygen evolution reaction is a key enabling step toward efficient utilization of renewable energy. Along with efforts to develop high-performance electrocatalysts for oxygen evolution reaction, pyrochlore oxides have emerged as highly active and stable materials that function as catalysts as well as conductive supports for hybrid catalysts. The compositional flexibility of pyrochlore oxide provides many opportunities to improve electrocatalytic performance by manipulating material structures and properties. In this Outlook, we first discuss the recent advances in developing metallic pyrochlore oxides as oxygen evolution catalysts, along with elucidation of their reaction mechanisms, and then introduce an emerging area of using pyrochlore oxides as conductive supports to design hybrid catalysts to further improve the OER activity. Finally, the remaining challenges and emerging opportunities for pyrochlore oxides as electrocatalysts and conductive supports are discussed.
The design of active and stable electrocatalysts for oxygen evolution reaction is a key enabling step toward efficient utilization of renewable energy. Along with efforts to develop high-performance electrocatalysts for oxygen evolution reaction, pyrochlore oxides have emerged as highly active and stable materials that function as catalysts as well as conductive supports for hybrid catalysts. The compositional flexibility of pyrochlore oxide provides many opportunities to improve electrocatalytic performance by manipulating material structures and properties. In this Outlook, we first discuss the recent advances in developing metallic pyrochlore oxides as oxygen evolution catalysts, along with elucidation of their reaction mechanisms, and then introduce an emerging area of using pyrochlore oxides as conductive supports to design hybrid catalysts to further improve the OER activity. Finally, the remaining challenges and emerging opportunities for pyrochlore oxides as electrocatalysts and conductive supports are discussed.
Toward
a clean and sustainable energy infrastructure, large-scale
energy conversion and storage technologies that can enable efficient
utilization of renewable energy are essential. To this end, hydrogen
production through the electrochemical water splitting process has
been considered as a key technology for storing renewable energy in
the form of chemical fuels.[1,2] In water electrolyzers,
hydrogen is generated through the reduction of two protons at the
cathode; however, the overall efficiency is determined by the slow
kinetics of the oxygen evolution reaction (OER), which is the four-proton,
four-electron oxidation of water, at the anode.[3,4] Thus,
the development of more active and durable OER catalysts has a direct
impact on device efficiency and cost-effectiveness.[2,3,5−12]Substantial efforts have been devoted to the study of various
metaloxides, including rutile, spinel, perovskite, rock salt, and bixbyite
transition metal oxides, in order to find more efficient catalysts
for the OER and to elucidate the reaction mechanisms.[2,4−9,11−14] However, under harsh acidic conditions,
candidates for these catalysts are limited to noble metal oxides,
such as IrO2, RuO2, their solid solutions, Ir-
or Ru-based perovskites, and Ruddlesden–Popper phases.[15−21] RuO2 represents the most active electrocatalyst for the
acidic OER, but the dissolution rate of Ru is somewhat faster than
Ir in acidic environments.[16,22] IrO2 exhibits
a higher stability than RuO2 and good activity in acidic
medium, but its cost is more than 10 times that of RuO2.[23] Therefore, various strategies have
been attempted to enhance the activity and stability of the Ru- and
Ir-based catalysts under acidic conditions by engineering their size,
shape, or elemental composition or employing stable substrate materials.[4,8,14,16,24−26] However, the high cost
of Ru and Ir still limits the large-scale application of proton exchange
membrane water electrolyzers.[25]The
crystal family of pyrochlore is a complex oxide with a general
formula of A2B2O7−δ of
which A is usually an alkaline-earth or rare-earth element and B is
a transition metal.[15] Recently, iridium
and ruthenium pyrochlore oxides, A2B2O7−δ (B = Ir or Ru), have risen as promising alternatives to binary RuO2 and IrO2oxides because of the low content of
noble metal, high activity, and stability under both alkaline and
acidic conditions.[15,22,23,27−38] Based on its crystal structure, the formula of pyrochlore oxides
also can be described as (A2B2O6O′)
or [A2O′][B2O6] with two types
of oxygen, consisting of a network of corner-sharing BO6 octahedra with A and O′ atoms occupying interstitial sites
(A2O′) (Figure ).[28] Thus, the O anion connects
two building blocks to form a network between the A- and B-site cations,
while the O′ anion links only to the A-site cations in the
form of A–O′–A.[28] It
is known that oxygen vacancies are generally formed preferentially
at the interstitial O′ sites rather than at the O sites.[38] Thanks to the compositional flexibility of the
A and B sites to manipulate their wide spectrum of properties, including
electrical, magnetic, dielectric, optical, and electrocatalytic properties,
pyrochlores have been used in a variety of applications, such as ionic/electrical
conductors, anode materials for solid electrolyte fuel cells, radioactive
waste immobilization, high-temperature thermal barrier coatings, photocatalysts,
electrocatalysts for oxygen reduction reaction (ORR), and OER.[39−41] In particular, pyrochlore oxides with metallic conduction behavior
are attractive candidates for OER catalysts due to their high conductivity,
fast charge transfer through the oxygen vacancies, and structural
stability. In addition, the ability to substitute different ions into
the A- and B-site elements while maintaining the same crystal structure
provides another powerful strategy to tune the concentration of oxygen
vacancies and electronic structures, and thus the OER activity and
stability.
Figure 1
Unit cell structure of A2B2O7 (left)
showing the A2O′ chains (middle) and corner shared
octahedral BO6 structures (right). Color code: A (teal),
B (gray), and O (red).[28] Images reproduced
with permission from ref (28). Copyright 2017 American Chemical Society.
Unit cell structure of A2B2O7 (left)
showing the A2O′ chains (middle) and corner shared
octahedral BO6 structures (right). Color code: A (teal),
B (gray), and O (red).[28] Images reproduced
with permission from ref (28). Copyright 2017 American Chemical Society.In this Outlook, we first briefly summarize the recent advances
in designing metallic pyrochlore oxides as OER catalysts through composition
control of A- and B-site cations, along with elucidation of their
OER mechanisms and structure–mechanism–performance relationship.
Then, we introduce a new approach using metallic pyrochlore oxides
as conductive supports to design hybrid catalysts using the in situ exsolution method, highlighting the synergetic effects
between catalyst and support to enhance the OER activity. Finally,
we discuss the remaining challenges and emerging opportunities of
pyrochlore oxides as electrocatalysts and conductive supports.
Metallic
Pyrochlore Oxides as Oxygen Evolution Reaction Catalysts
Bismuth (Bi) and lead (Pb) pyrochlores have been identified as
metallic conductors.[42,43] It was first suggested that the
metallic behavior of Pb2Ru2O7−δ is due to the significant mixing between Ru 4d, Pb 6s, and Pb 6p
bands.[43−45] Later, Hsu and co-workers showed that the Pb 6s band
was unlikely to contribute to the metallic behavior, but the metallic
conductivity of Bi2Ru2O7 and Pb2Ru2O6.5 was due to the mixing of unoccupied
Pb (or Bi) 6p and Ru 4d bands via the ligand oxygen 2p states. In
general, the metallic vs semiconductor behavior of ruthenium pyrochlores
(A2Ru2O7−δ) can be determined
by the Mott–Hubbard mechanism of electron localization.[46] Since the width of the t2g-block
bands of A2Ru2O7−δ increases
as the Ru–O–Ru bond angle increases, the structure exhibits
metallic behavior when the Ru–O–Ru bond angle is larger
than 133°.[46] In addition, there is
a strong linear relationship between the ionic radius of the A-cation
and the Ru–O–Ru bond angle, explaining the metallic
behavior of ruthenium pyrochlores with large size cations such as
Bi, Pb, and Tl.[46] Such metallic conductivity
of pyrochlore oxides allows the preparation of self-supported electrodes
without the use of conductive carbon support, simplifying membrane
electrode assembly in water electrolyzers.[38] Motivated by this highly conductive behavior, metallic pyrochlores,
A2B2O7−δ (A = Bi, Pb,
Tl, B = Ru, Ir) have been actively investigated as OER catalysts under
both alkaline and acidic conditions.[22,27,38,47−52]Ramani and co-workers synthesized conductive pyrochlore oxides
(A2B2O7−δ, A = Pb or
Bi and B = Ru, Ir or Os) using solid-state methods and compared their
OER activities in 0.1 M KOH.[38] They correlated
the OER activity trend (ruthenate pyrochlores > iridatepyrochlores
> osmate pyrochlores) with the bonding strength between the B-site
cation and the oxygen species based on the conventional OER mechanism
established by density functional theory (DFT) calculations on metaloxides.[3,9,13] Based on a
single descriptor, the oxygen adsorption energy on the catalyst surface,
the conventional OER mechanism follows the Sabatier principle: the
best catalyst binds oxygen on its surface neither too weakly nor too
strongly.[3,9,13] Among binary
oxides, RuO2 and Co3O4 exhibit the
lowest theoretical overpotentials because of their optimal binding
energy of oxygen (Figure a).[3,13] Based on this mechanism, they
employed the calculated d-band center and adsorbate (s or p)–metal
d-coupling matrix element squared, Vad2,[53] to explain the high activity
of ruthenate pyrochlores through their optimum interaction with oxygen
intermediates.[38]
Figure 2
(a) Activity trends toward
oxygen evolution for binary oxides.[13] (b) Ex situ normalized O K-edge
XANES total electron yield mode spectra of the highly crystalline
pyrochlore oxides (A2Ru2O7–, A = Pb and Sm).[35] (c)
Linear scan voltammogram curves showing the OER activities of pyrochlore
oxides and RuO2 in 0.1 M KOH.[35] (d) Specific OER activity of pyrochlore oxides at η = 300
mV in 0.1 M HClO4.[33] (e, f)
O K-edge XAS and the normalized intensity of the prepeak around 528
eV.[33] Images reproduced with permission
from refs (13, 35), and (33). Copyright 2011 WILEY-VCH,
2017 The Royal Society of Chemistry, 2018 WILEY-VCH.
(a) Activity trends toward
oxygen evolution for binary oxides.[13] (b) Ex situ normalized O K-edge
XANES total electron yield mode spectra of the highly crystalline
pyrochlore oxides (A2Ru2O7–, A = Pb and Sm).[35] (c)
Linear scan voltammogram curves showing the OER activities of pyrochloreoxides and RuO2 in 0.1 M KOH.[35] (d) Specific OER activity of pyrochlore oxides at η = 300
mV in 0.1 M HClO4.[33] (e, f)
O K-edge XAS and the normalized intensity of the prepeak around 528
eV.[33] Images reproduced with permission
from refs (13, 35), and (33). Copyright 2011 WILEY-VCH,
2017 The Royal Society of Chemistry, 2018 WILEY-VCH.Current understanding of transition metal oxide-based OER
catalysts
suggests that increasing the covalency of the transition metal (TM)–O
bond can lower the energy associated with O–O bond formation,[6,54,55] which is often considered as
the rate-determining step for the conventional OER mechanism.[9,13] Therefore, the effects of the covalency of the TM–O bonds
on the OER activities have been studied for Ru and Irpyrochlore oxides.[33,35] Cho and co-workers reported that the covalency of Ru–O bonds
of ruthenate pyrochlores affected the ORR and OER activities by comparing
the X-ray absorption near edge structure (XANES) spectra of the insulating
Sm2Ru2O7 and metallic Pb2Ru2O6.5.[35] The degree
of covalency of Ru–O bonds on the surface of the pyrochloreoxides was quantified based on the O K-edge XANES spectra at total
electron yield mode (Figure b) with the equation of absorbance/(holeeg + 1/4holet2g).[35] The higher covalency value
of metallic Pb2Ru2O6.5 (0.65) than
that of insulating Sm2Ru2O7 (0.39)
strengthened was correlated with the higher OER activity of Pb2Ru2O6.5 compared to Sm2Ru2O7 in 0.1 M KOH (Figure c). In addition, Shang et al. studied the
electronic structures of a series of pyrochlore iridates (R2Ir2O7) with different sizes of rare earth cations
(R = Ho < Tb < Gd < Nd < Pr) in correlation with their
OER activities under acidic conditions.[33] The OER activity of iridatepyrochlores in 0.1 M HClO4 gradually increased with the R ionic radius (Figure d).[33] In particular,
Pr2Ir2O7 showed considerably enhanced
activity and stability compared to the benchmark IrO2.[33] Such enhanced activity of Pr2Ir2O7 was attributed to the improved electrical conductivity
and the enhancement of Ir–O bond covalency. They showed that
increasing R ionic radius weakens the effective electron correlations
in these iridatepyrochlore oxides via the chemical pressure effect,
inducing an insulator–semimetal–metal transition.[33] The O K-edge XANES spectra (Figure e) were used to evaluate the
strength of Ir 5d–O 2p orbital hybridization in these oxides.[33] The prepeak intensity at ∼528 eV, which
is associated with the transition from the O 1s core level to the
unoccupied O 2p states hybridized with Ir 5d t2g orbitals,
was compared as an indicator of the metal–oxygen orbital hybridization
(Figure f).[33] The normalized intensity of the prepeak clearly
increased with increasing the ionic radius of R, indicating the enhanced
the Ir 5d–O 2p hybridization through the reduced electron correlations
(Figure f). These
results suggest that increasing the Ir–O covalency by adjusting
the ionic radius of the A-site cation can be an effective strategy
to enhance the OER activity of iridatepyrochlores.Taking into
account that numerous pyrochlore oxides can be generated
from various combinations of A-site and B-site components, the computation-based
screening process is critical to identify the ideal structure and
property of pyrochlore having superior catalytic activity and stability.
Schmidt and co-workers first employed a computational method to investigate
a series of lanthanidepyrochlore oxides (A2B2O7, A = La, Ce, Pr, Nd, Sm, Gd, or Yb and B = Ir or Ru)
as OER catalyst candidates.[31] Specifically,
the phase diagrams, Pourbaix diagrams (potential vs pH), band energy
diagrams, and projected density of states (PDOS) were calculated for
these pyrochlore oxides to investigate their phase stability, electrochemical
stability, conductivity, and Ir 5d or Ru 4d–O 2p hybridization,
respectively (Figure ).[31] Using the calculated phase diagram
(Figure a) and total
energy (eV/atoms) for these pyrochlores, it was possible to predict
whether materials could be synthesized. In addition, the calculated
Pourbaix diagrams were used to determine whether materials will dissociate
at the pH and electrochemical potential values under OER conditions.
For example, the Pourbaix diagram of Gd2Ir2O7 pyrochlore shows that this material does not dissolve when
contacted with water under OER conditions (Figure b).[31] Moreover,
the band structure diagram of Gd2Ir2O7 shows that the material can be considered conductive because some
bands intersect at the Fermi level (Figure c).[31] The PDOS
shows that, for most pyrochlore candidates, the valence band is formed
by the Ir or Ru d-orbitals hybridized with the O 2p orbitals and the
Ir or Ru d-orbitals also contribute to the conduction band, which
is sometimes hybridized with the A-site element f-orbitals (Figure d).[31] Based on these systematic screening processes, only a few
materials (A2B2O7, A = Nd, Gd, or
Yb and B = Ir or Ru) were identified for the synthesis and testing
as OER catalysts.[31] Yb2Ir2O7 and the ruthenate pyrochlores (Nd2Ru2O7, Gd2Ru2O7, and Yb2Ru2O7) exhibited higher
OER activity and stability in 0.1 M HClO4 compared to the
IrO2 catalyst (Figure e).[31] The OER activity of
iridate or ruthenate pyrochlore series generally increased with decreasing
size of the A-site cation (Figure f).[31] It is interesting
to note that this trend is the opposite of other pyrochlore iridate
systems (R2Ir2O7, R = Ho, Tb, Gd,
Nd, and Pr, Figure d).[33] Despite the opposite trend of these
two studies,[31,33] controlling the A-site ion in
Ir or Ru pyrochlore oxides suggests an effective strategy in creating
stable, conductive, highly active, and stable OER catalysts.
Figure 3
(a) Phase diagram,
(b) Pourbaix diagram, (c) band structure diagram,
and (d) PDOS diagram for Gd2Ir2O7.[31] (e) Measured OER activities for the
Ru and Ir pyrochlore series in 0.1 M HClO4 and (f) average
specific activity of the pyrochlore oxides as a function of the unit
cell parameter.[31] Images reproduced with
permission from ref (31). Copyright 2019 American Chemical Society.
(a) Phase diagram,
(b) Pourbaix diagram, (c) band structure diagram,
and (d) PDOS diagram for Gd2Ir2O7.[31] (e) Measured OER activities for the
Ru and Irpyrochlore series in 0.1 M HClO4 and (f) average
specific activity of the pyrochlore oxides as a function of the unit
cell parameter.[31] Images reproduced with
permission from ref (31). Copyright 2019 American Chemical Society.
Metal
Substitution for Pyrochlore Oxides
Metal cation substitution
is the most popular strategy to tune
the electronic structure of metal oxides by controlling the oxidation
state of the metal and the concentration of oxygen vacancy (OV). This
strategy has also been actively adopted to enhance the OER activity
of pyrochlore oxides, with a particular focus on pyrochlore-type yttriumruthenate (Y2Ru2O7−δ). Yang and co-workers first showed that phase-pure Y2Ru2O7−δ exhibited significantly
enhanced OER activity and stability over conventional RuO2 electrocatalysts in 0.1 M HClO4.[28] Later, the same group introduced porous Y2[Ru1.6Y0.4]O7−δ through the partial
substitution of Ru4+ with Y3+ cations, demonstrating
the improved OER activity compared to Y2Ru2O7−δ (Figure a).[30] The enhanced activity
of Y2[Ru1.6Y0.4]O7−δ was attributed to both the high surface area of the porous material
and the introduced oxygen lattice defects that are formed by the mixed
oxidation state of Ru4+/5+ through partial substitution
by Y3+ on the B-site.[30] Specifically,
they suggested that the oxygen-deficient pyrochlore structure can
lower the band energy and strengthen the covalent bond between the
Ru 4d band and the O 2p band, which is beneficial for OER performance.[30]
Figure 4
(a) OER activity comparison of porous Y2[Ru1.6Y0.4]O7−δ, Y2Ru2O7−δ, and RuO2 electrocatalysts
in 0.1 M HClO4 by Tafel plots.[30] (b) The relationships between OER overpotential (at 10 mA cm–2) in 0.5 M H2SO4 and OV concentration
for Y2–BaRuO7−δ (x = 0, 0.1,
0.15, 0.25, 0.4).[32] (c) Tafel plots of
Y1.8M0.2Ru2O7−δ measured in 1 N H2SO4.[34] (d) Scaling between OV content expressed as OV/OL ratio and enthalpies of MO formation, ΔfH°.[34] (e) Relation between the OER activity of Y1.8M0.2Ru2O7−δ and OV/OL ratio.[34] (f) PDOS on Ru 4d and O 2p states of Y1.8Cu0.2Ru2O7. PDOS on O 2p states of surface terminated
oxygen atoms (Osurf) are shaded.[34] (g) Schematic rigid band diagram for Y1.8Fe0.2Ru2O7 and Y1.8Cu0.2Ru2O7 visualizing an upshift of the O 2p band center.[34] (h) Scaling between specific OER activity and
O 2p band center position for Y1.8M0.2Ru2O7−δ.[34] Images reproduced with permission from refs (30, 32), and (34). Copyright 2018 Wiley-VCH, 2020 American Chemical Society.
(a) OER activity comparison of porous Y2[Ru1.6Y0.4]O7−δ, Y2Ru2O7−δ, and RuO2 electrocatalysts
in 0.1 M HClO4 by Tafel plots.[30] (b) The relationships between OER overpotential (at 10 mA cm–2) in 0.5 M H2SO4 and OV concentration
for Y2–BaRuO7−δ (x = 0, 0.1,
0.15, 0.25, 0.4).[32] (c) Tafel plots of
Y1.8M0.2Ru2O7−δ measured in 1 N H2SO4.[34] (d) Scaling between OV content expressed as OV/OL ratio and enthalpies of MO formation, ΔfH°.[34] (e) Relation between the OER activity of Y1.8M0.2Ru2O7−δ and OV/OL ratio.[34] (f) PDOS on Ru 4d and O 2p states of Y1.8Cu0.2Ru2O7. PDOS on O 2p states of surface terminated
oxygen atoms (Osurf) are shaded.[34] (g) Schematic rigid band diagram for Y1.8Fe0.2Ru2O7 and Y1.8Cu0.2Ru2O7 visualizing an upshift of the O 2p band center.[34] (h) Scaling between specific OER activity and
O 2p band center position for Y1.8M0.2Ru2O7−δ.[34] Images reproduced with permission from refs (30, 32), and (34). Copyright 2018 Wiley-VCH, 2020 American Chemical Society.Due to the n-type semiconducting property, phase-pure
Y2Ru2O7−δ (YRO) shows
low electrical
conductivity. Brambilla and co-workers have shown that A-site doping
of YRO with Zn2+ (Y1.85Zn0.15Ru2O7−δ) can increase the conductivity
by 2 orders of magnitude compared to undoped YRO at room temperature.[56] In addition, previous studies have shown that
doping the A-site of pyrochlores with 2+ cation can lead to a hole
doping effect with an increased concentration of disordered oxygen
vacancies (OVs).[56−58] Motivated by these doping effects, Wang and co-workers
have reported a series of A-site-doped YRO pyrochlores (Y2–ARuO7−δ, A= Zn,[23] Ca,[59] Ba,[32] and Mg[60]) as highly active and stable OER catalysts. The substitution of
2+ cation at the A-site of YRO enables the formation of OVs and mixed
valences of Ru5+/4+, which significantly alters the electronic
structure and conductivity. Figure b shows the strong correlation between the OV concentration
of Y2–BaRuO7−δ (x = 0, 0.1,
015, 0.25, and 0.4) and their OER activities in 0.5 M H2SO4.[32] They explain that a
higher OV concentration in the catalysts can provide more adsorption
sites for the OER intermediates.[32] Moreover,
the hole-doping effect caused by the A-site doping of YRO catalysts
can enhance conductivity, generate multivalence of Ru5+/4+, and alter the electronic band structure, which can all benefit
the OER activity.[32]Since the metal
substitution can cause several structural changes,
including OV concentration, conductivity, and electronic band structure,
it is critical to evaluate the contribution of each variable to the
OER activity and stability. To answer this important question, Müller
and co-workers have studied model pyrochlores of Y1.8M0.2Ru2O7−δ (M = Cu, Co,
Ni, Fe, and Y) as OER catalysts in acid.[34] Using a moderate level of A-site substitution, the oxidation state
of Ru was maintained unchanged within the series, which is intended
to study the individual effect of the M substituent on the OER activity.[34] Similar Tafel slopes (52–63 mV/dec) of
all prepared pyrochlores indicate the same rate-limiting step (Figure c), but the specific
OER activity of Y1.8Cu0.2Ru2O7−δ at 1.50 V vs reversible hydrogen electrode
(RHE) in 1 N H2SO4 is more than 1 order of magnitude
higher than Y1.8Fe0.2Ru2O7−δ.[34] The concentration of surface OVs in
the pyrochlore was calculated based on the ratio of OV (oxygen
vacancy)/OL (lattice oxygen) through O 1s core level X-ray
photoelectron spectroscopy (XPS) spectra. The calculated concentration
of OV sites showed good correlations with the enthalpy of formation
of the binary oxides MO (Figure d) and the OER activity (Figure e).[34] These trends were explained by comparing the electronic
band structures of pyrochlores. The calculated density of states (DOS)
of Y1.8M0.2Ru2O7 showed
a substantial contribution of oxygen states to the bands near the
Fermi level (EF) (Figure f), indicating the high covalency of the
Ru–O bonds.[34] Transitioning the
substitution from Fe to Y, Ni, Co, and to Cu at the A-site shifted
the EF closer to the O 2p band center
and also decreased the energy gap between the Ru 4d and O 2p band
centers,[34] defined as charge transfer energy
from the previous study on perovskite catalysts.[61] As the EF moves down closer
to the O 2p states, the states below the EF show a greater oxygen character, indicating a higher covalency of
the Ru–O bond in Y1.8Cu0.2Ru2O7 compared to Y1.8Fe0.2Ru2O7 (Figure g).[34] A strong correlation between OV
concentration and O 2p band center relative to the EF was reported for perovskite catalysts.[62] Therefore, the upshift of the O 2p band center relative
to the EF can explain the higher concentration
of OV in Y1.8Cu0.2Ru2O7 (Figure g). In addition,
the OER activity of Y1.8M0.2Ru2O7 pyrochlores strongly correlated with the O 2p band center
relative to the EF computed for surface
O atoms (Figure h).[34] Therefore, the enhanced OER activity of Y1.8Cu0.2Ru2O7 was attributed
to the decreased energy gap between the O 2p states and the EF as well as the reduced charge transfer energy.
Understanding
of Oxygen Evolution Reaction Mechanisms on Pyrochlore
Oxides
The conventional OER mechanism of metal oxides is
derived from
that of metal catalysts, where the dominant parameter governing the
reaction overpotential is the binding strength of oxygenated adsorbates
(Figure , adsorbate
evolution mechanism (AEM)).[9,12,13,34] The scaling relationship between
adsorption energies of the oxygenated adsorbates defines a theoretical
minimum overpotential for the OER.[13] Recent
studies on metal oxide catalysts have suggested the possibility of
a different reaction mechanism based on the involvement of lattice
oxygens in the OER, the so-called lattice oxygen(-mediated) mechanism
(LOM, Figure ).[3,5,34,63−65] This LOM mechanism involves the oxidation of the
lattice oxygen (more precisely, the lattice O2– anions),
thus avoiding the scaling limitations of the conventional AEM.[3,34] Therefore, understanding the LOM mechanism on pyrochlore oxides
is important to improve the OER kinetics. Schmidt and co-workers first
investigated the contribution of the LOM mechanism on highly crystalline
pyrochlores (Yb2Ru2O7 and Gd2Ru2O7) by measuring the isotopic distribution
of the evolved oxygen in 18O-labeled water using differential
electrochemical mass spectrometry (DEMS).[31] Assuming that the surface of the pyrochlore is composed of solely 16O, the LOM mechanism can produce the 16O18O or 16O2 through the participation of the
pyrochlore lattice oxygen.[31] Two types
of molecular oxygen (18O2 with m/z of 36 and 16O18O with m/z of 34) were detected, but the ratio
of 16O18O (m/z = 34) was only 0.04, indicating the negligible contribution of the
LOM mechanism.[31] A recent study also showed
no involvement of the lattice oxygen on crystalline RuO2 films during OER, suggesting that the LOM mechanism can only be
involved with amorphous RuO2 or nanocrystalline phases
with undercoordinated edge sites.[66]
Figure 5
Schematic illustration
showing OER mechanisms under acidic conditions:
adsorbate evolution mechanism (AEM) and lattice-oxygen-mediated mechanism
(LOM).[34] An image reproduced with permission
from ref (34). Copyright
2020 American Chemical Society.
Schematic illustration
showing OER mechanisms under acidic conditions:
adsorbate evolution mechanism (AEM) and lattice-oxygen-mediated mechanism
(LOM).[34] An image reproduced with permission
from ref (34). Copyright
2020 American Chemical Society.Although highly crystalline pyrochlores showed negligible involvement
of the lattice oxygen in the OER, the LOM mechanism may play a role
on the doped pyrochlores containing large amounts of oxygen vacancies.
Recent studies have also suggested an important role of OVs in the
LOM mechanism of perovskite catalysts.[3,67,68] In agreement with this suggestion, Müller
and co-workers hypothesized that the increased oxygen lability and
surface density of OV in pyrochlores favored the LOM mechanism, which
may increase the OER activity.[34] Using
model pyrochlores of Y1.8M0.2Ru2O7−δ (M = Cu, Co, Ni, and Fe), they suggested that
the enthalpy of formation (ΔfH°)
of the binary oxides MO (Fe2O3, CoO, NiO, and CuO) can be an important parameter to
understand the relationship between the surface oxygen lability and
the OER activity. The calculated ΔfH° of the binary oxides MO showed
a strong correlation with the density of OV site and the OER activity
of Y1.8M0.2Ru2O7 pyrochlores
(Figure d and e).
The less negative ΔfH° of MO indicates the weaker M–O bonds (i.e.,
less stable oxide) that can promote the removal of lattice oxygen
atoms. Therefore, Y1.8Cu0.2Ru2O7 with the smallest negative value of ΔfH° of MO showed the highest
concentration on OV and ultimately the highest OER activity.[34] These results indicate that ΔfH° of a bulk binary oxide can be a useful parameter
to understand the LOM mechanism in correlation with surface oxygen
lability and density of OV in pyrochlores.
Pyrochlore
Oxide Supports for Hybrid Catalysts
Carbon blacks, such as
Ketjenblack (AkzoNobel) and Vulcan (Cabot),
have been dominantly used as supports for electrocatalysts due to
their high electric conductivity (∼20 S/cm) and high surface
area (200–800 m2/g).[69,70] However, the
carbon black support is highly corroded under OER conditions, resulting
in the detachment of active catalytic materials from the support.[69−71] Although graphitized carbon is more durable than porous carbon black,
it still suffers from irreversible oxidation at high potential and
acidity.[69] Metal oxides have been considered
as alternative supports for OER, with enhanced conductivity through
metal doping.[69,72,73] In particular, metallic pyrochlore oxides, such as Pb2Ru2O7−δ, exhibit a high conductivity
of (2–5) × 103 S/cm.[45] For example, the recently reported conductive pyrochlore oxides
(A2B2O7−δ, A = Pb or
Bi and B = Ru, Ir, or Os) showed high conductivity in the range of
50–120 S/cm.[38] Additionally, A-site
doping of semiconducting YRO with Zn2+ or Ca2+ increases the conductivity to 0.1–50 S/cm.[56,74] Such high conductivity of pyrochlore oxides is sufficient to meet
the minimum electric conductivity requirement (∼0.1 S/cm)[69] for electrocatalytic support applications. In
addition to high electric conductivity, the synthesis of nanoscale
pyrochlore oxides is also important for both electrocatalyst and support
applications. Conventional solid-state synthesis of pyrochlore oxides
is typically performed at high calcination temperatures above 800
°C, resulting in micron-scale products with low surface area.[38] Therefore, significant efforts have been made
to synthesize nanoscale pyrochlore oxides using various methods, including
hydrothermal synthesis,[27] sol–gel
process,[35] templating approach,[75] Adams fusion method,[15] glycine-nitrate combustion method,[76] perchloric
acid-based porogen method,[30] and polymerentrapment flash pyrolysis method.[77] These
efforts allow the size of pyrochlore oxides to be reduced to tens
of nanometers with significantly improved surface area, making them
more qualified catalysts and conductive supports.While most
of the reported works have focused on the use of pyrochloreoxides as active OER catalysts, a recent study first showed that pyrochloreoxide can be a promising substrate for depositing other transition
metal catalysts to design high-performance hybrid catalysts.[78] Kim et al. have designed the metallic cobalt
(Co) nanoparticles anchored pyrochlore oxide hybrid catalysts through
the in situ exsolution process of Co substituted
yttrium ruthenate pyrochlore oxide (Y2Ru2–CoO7) (Figure a). Through careful
control of the reduction temperature, metallic Co nanoparticles were
formed on the surface of Y2Ru2–CoO7 pyrochlore without
collapsing the crystal structure of the pyrochlore oxide support (Figure b–d).[78] The synthesized Co nanoparticles decorated Y2Ru2–CoO7 catalyst (YRCO-560) exhibited superior OER activity
and stability in 0.1 M KOH (Figure e–g).[78]
Figure 6
(a) Schematic
illustration synthesis of YRCO-560 via the in situ exsolution of Co nanoparticles from Y2Ru2–CoO7 at 560
°C under a mixture of H2/Ar gases.[78] (b, c) Transmission electron
microscopy (TEM) images of YRCO-560.[78] (d)
Scanning TEM energy dispersive X-ray mapping images for Y, Ru, Co,
and O elements distributed at the YRCO-560.[78] (e) OER polarization curves and (f) Tafel plots for YRCO-560 and
IrO2 in 0.1 M KOH.[78] (g) Chronopotentiometric
tests for YRCO-560 at 10 and 20 mA/cm2 for 10 h.[78] Images reproduced with permission from ref (78). Copyright 2019 WILEY-VCH.
(a) Schematic
illustration synthesis of YRCO-560 via the in situ exsolution of Co nanoparticles from Y2Ru2–CoO7 at 560
°C under a mixture of H2/Ar gases.[78] (b, c) Transmission electron
microscopy (TEM) images of YRCO-560.[78] (d)
Scanning TEM energy dispersive X-ray mapping images for Y, Ru, Co,
and O elements distributed at the YRCO-560.[78] (e) OER polarization curves and (f) Tafel plots for YRCO-560 and
IrO2 in 0.1 M KOH.[78] (g) Chronopotentiometric
tests for YRCO-560 at 10 and 20 mA/cm2 for 10 h.[78] Images reproduced with permission from ref (78). Copyright 2019 WILEY-VCH.The in situ X-ray absorption spectroscopy
(XAS)
technique was employed for in-depth understanding of the origin of
the superior OER performance of this hybrid catalyst (YRCO-560). While
the applied potential increased, the Y K-edge XANES spectra were positively
shifted and the Y–O bonds peak in the Y K-edge extended X-ray
absorption fine structure (EXAFS) spectra were negatively shifted,
clearly indicating the oxidation behavior of Y cations in YRCO-560
under OER conditions (Figure a and b).[78] The oxidation of Ru
cations at the B-site in YRCO-560 was also confirmed by observing
the positively shifted Ru K-edge XANES spectra with increasing potential
(Figure c).[78] Such facile oxidation behavior of the Y and
Ru cations may infer efficient charge transfer from the surface to
the inner layer of pyrochlore oxide during the OER process.[78] In addition, the reduced distance of Ru–O
bonds in the Ru K-edge EXAFS spectra showed negligible changes under
OER conditions (Figure d).[78] Such rigid B-site RuO6 octahedral frameworks can contribute to the high stability of YRCO-560
during the OER process.[36] Both the decreased
pre-edge peak intensity and the positively shifted absorption edge
in the Co K-edge XANES spectra of YRCO-560 (Figure e) indicate the transformation of metallic
Co nanoparticles to CoOOH during the OER process.[78] The Co K-edge EXAFS spectra of YRCO-560 showed a Co–O
peak at a reduced distance of 1.55 Å from the CoO6 octahedral framework of pyrochlore due to the substitution of Co
cations for the B-site (Figure f).[78] With the increase of applied
potential, this peak remained constant possibly due to the rigid CoO6 octahedral frameworks, whereas a new peak of the Co–O
bond from CoOOH appeared at a reduced distance of 1.44 Å.[78] Moreover, the metallic Co–Co bond from
Co nanoparticles was transformed into that of the edge-sharing Co3+ in CoOOH during the OER process. Both observations clearly
indicate the conversion of metallic Co to CoOOH during the OER process.[78] Based on these in situ XAS
characterizations, the superior OER activity of YRCO-560 was attributed
to the synergetic contributions of (1) the facilitated oxidation of
metallic Co to CoOOH on the pyrochlore oxide surface, which is often
considered as the rate-determining step of the OER, and (2) the facile
oxidation characteristic of both A-site Y and B-site Ru cations in
pyrochlore oxide that can promote the efficient charge transfer from
the oxidation of transition metal toward the inner layers of the support
during the OER (Figure g).[78] The introduced pyrochlore-support-based
hybrid catalyst is underexplored, and it may allow for designing high-performance
electrocatalysts for other reactions including ORR and hydrogen evolution
reaction (HER) through favorable interactions between metal nanoparticles
and pyrochlore oxide supports.
Figure 7
In situ (a, b) Y, (c,
d) Ru, and (e, f) Co K-edge
XANES and EXAFS spectra of YRCO-560 from 1.43 to 1.48 V vs RHE in
0.1 M KOH.[78] (g) Schematic of the efficient
electron transfer characteristic of YRCO-560 during OER.[78] Images reproduced with permission from ref (78). Copyright 2019 WILEY-VCH.
In situ (a, b) Y, (c,
d) Ru, and (e, f) Co K-edge
XANES and EXAFS spectra of YRCO-560 from 1.43 to 1.48 V vs RHE in
0.1 M KOH.[78] (g) Schematic of the efficient
electron transfer characteristic of YRCO-560 during OER.[78] Images reproduced with permission from ref (78). Copyright 2019 WILEY-VCH.
Outlook
Various combinations of
A-site and B-site compositions of pyrochloreoxides, including cation doping, offer a myriad of opportunities to
engineer the OER mechanisms and performance through fine-tuning the
electronic structure and the surface adsorption energies of oxygen
intermediates. Given the numerous combinations of pyrochlore oxide
candidates, a computer-simulation-based screening process is extremely
helpful in identifying the ideal structure of materials that can have
superior catalytic activity and stability. A recent study first showed
that the computational approach could be used to identify suitable
pyrochlore oxides as OER catalysts based on the calculations of the
phase, Pourbaix, and band energy diagrams and projected density of
states.[31] Such a computational approach
is highly needed to establish the structure–mechanism–performance
relationship of pyrochlore oxides for specific electrochemical reactions.Although significant advances have been achieved in designing high-performance
pyrochlore oxide catalysts for OER under both acidic and alkaline
conditions, a fundamental understanding of the OER mechanisms associated
with the structure of pyrochlore is still largely lacking in comparison
to other metal oxide catalysts. In particular, understanding the LOM
mechanism involving the oxidation of the lattice oxygen of pyrochloreoxides remains a critical task. A recent study first revealed that
the contribution of the LOM mechanism to the highly crystalline pyrochlore
is negligible.[31] If the conventional AEM
mechanism dominates highly crystalline metal oxides, facet engineering
is crucial to improve the OER activity through the controlled surface
atomic structure.[66] A recent study reported
the correlation between low-index facets of micrometer-sized polyhedral
pyrochlore (Bi2Ru2O7) and their ORR
and OER activities,[3] suggesting a new design
strategy of pyrochlore oxides through facet engineering. On the other
hand, in the case of doped pyrochlores containing large amounts of
oxygen vacancies, the role of the LOM mechanism may be significant.
A recent study has hypothesized that the increased oxygen lability
and surface density of OV in metal-doped pyrochlores favors the LOM
mechanism.[34] Thus, in-depth experimental
and computational investigations should focus on revealing the active
sites, including involvement of lattice oxygens, and the OER mechanisms,
providing more guidelines for the discovery of pyrochlore oxides that
can overcome the scaling limitations of the traditional OER mechanism.
In addition, more in situ and operando analyses are needed to probe the surface structural changes of pyrochloreoxides and the corresponding reaction mechanism under OER conditions.The role of pyrochlore oxides can be further increased when used
as a conductive support material for other metal catalysts, because
it can not only directly participate in the OER reaction but also
efficiently transfer charges for facile oxidation of anchored metal
catalysts. Recently, we have demonstrated that metallic Co nanoparticles
anchored yttrium ruthenate pyrochlore oxide prepared by the in situ exsolution process can exhibit excellent OER activity.
The superior OER activity of this hybrid catalyst is due to the facile
oxidation of metallic Co to CoOOH by efficient charge transfer from
the transition metal to the inner layers of the pyrochlore oxide support.
Based on the same strategy, various transition metals or their alloy
nanoparticles can be further synthesized on the pyrochlore oxide support
by carefully controlling the reduction temperature. Such a significant
advantage allows for the design of new pyrochlore-based hybrid catalysts
capable of catalyzing specific electrochemical reactions, including
ORR and HER. The synthesis of Ni and NiRu alloy nanoparticles on pyrochloreoxides is under investigation to design highly active catalysts for
OER and HER.
Authors: Alexis Grimaud; Oscar Diaz-Morales; Binghong Han; Wesley T Hong; Yueh-Lin Lee; Livia Giordano; Kelsey A Stoerzinger; Marc T M Koper; Yang Shao-Horn Journal: Nat Chem Date: 2017-01-09 Impact factor: 24.427
Authors: Kripasindhu Sardar; Enrico Petrucco; Craig I Hiley; Jonathan D B Sharman; Peter P Wells; Andrea E Russell; Reza J Kashtiban; Jeremy Sloan; Richard I Walton Journal: Angew Chem Int Ed Engl Date: 2014-09-04 Impact factor: 15.336