55 research outputs found
MXene as a Charge Storage Host
ConspectusThe development of efficient electrochemical energy storage (EES)
devices is an important sustainability issue to realize green electrical
grids. Charge storage mechanisms in present EES devices, such as ion
(de)Âintercalation in lithium-ion batteries and electric double layer
formation in capacitors, provide insufficient efficiency and performance
for grid use. Intercalation pseudocapacitance (or redox capacitance)
has emerged as an alternative chemistry for advanced EES devices.
Intercalation pseudocapacitance occurs through bulk redox reactions
with ultrafast ion diffusion. In particular, the metal carbide/nitride
nanosheets termed MXene discovered in 2011 are a promising class of
intercalation pseudocapacitor electrode materials because of their
compositional versatility for materials exploration (e.g., Ti<sub>2</sub>CT<sub><i>x</i></sub>, Ti<sub>3</sub>C<sub>2</sub>T<sub><i>x</i></sub>, V<sub>2</sub>CT<sub><i>x</i></sub>, and Nb<sub>2</sub>CT<sub><i>x</i></sub>, where
T is a surface termination group such as F, Cl, O, or OH), high electrical
conductivity for high current charge, and a layered structure of stacked
nanosheets for ultrafast ion intercalation. Various MXene electrodes
have been reported to exhibit complementary battery performance, such
as large specific capacity at high charge/discharge rates. However,
general design strategies of MXenes for EES applications have not
been established because of the limited understanding of the electrochemical
mechanisms of MXenes. This Account describes current knowledge of
the fundamental electrochemical properties of MXenes and attempts
to clarify where intercalation capacitance ends and intercalation
pseudocapacitance begins.MXene electrodes in aqueous electrolytes
exhibit intercalation
of hydrated cations. The hydrated cations form an electric double
layer in the interlayer space to give a conventional capacitance within
the narrow potential window of aqueous electrolytes. When nonaqueous
electrolytes are used, although solvated cations are intercalated
into the interlayer space during the initial stage of charging, the
confined solvation shell should gradually collapse because of the
large inner potential difference in the interlayer space. Upon further
charging, desolvated ions solely intercalate, and the atomic orbitals
of the desolvated cations overlap with the orbitals of MXene to form
a donor band. The formation of the donor band induces the reduction
of MXene, giving rise to an intercalation pseudocapacitance through
charge transfer from the ions to MXene sheets. Differences in the
electrochemical reaction mechanisms lead to variation of the electrochemical
responses of MXenes (e.g., cyclic voltammetry curves, specific capacitance),
highlighting the importance of establishing a comprehensive grasp
of the electrochemical reactions of MXenes at an atomic level. Because
of their better charge storage kinetics compared with those of typical
materials used in present EES devices, aqueous/nonaqueous asymmetric
capacitors using titanium carbide MXene electrodes are capable of
efficient operation at high charge/discharge rates. Therefore, the
further development of novel MXene electrodes for advanced EES applications
is warranted
Electrode Properties of P2–Na<sub>2/3</sub>Mn<sub><i>y</i></sub>Co<sub>1–<i>y</i></sub>O<sub>2</sub> as Cathode Materials for Sodium-Ion Batteries
The
development of high-performance Na-ion intercalation electrodes
has been required recently because Na-ion batteries hold much promise
for inexpensive and efficient energy storage, which can be deployed
in a power grid. For both optimization and better understanding of
the electrode materials, it is indispensable to clarify the relationship
between the electronic state and electrochemical properties systematically.
In this work, we studied the electrochemical properties of P2–Na<sub>2/3</sub>Mn<sub><i>y</i></sub>Co<sub>1–<i>y</i></sub>O<sub>2</sub> in detail. A series of the P2 phases was successfully
synthesized by the conventional solid-state reaction. The solid solution
P2 compounds showed that the redox potential of Co<sup>4+</sup>/Co<sup>3+</sup> and Mn<sup>4+</sup>/Mn<sup>3+</sup> shifts systematically
by the transition-metal substitution. The charge–discharge
cycle tests revealed that with increasing <i>y</i> the initial
specific capacity increases while the cycle stability degrades. The
origin for the cycle degradation was analyzed by the electrochemical
impedance spectroscopy, which evidenced that the substitution of Co
for Mn accelerates the formation of the passivating layer at the electrode
surface
Electrochemical Redox Mechanism in 3.5 V Li<sub>2‑<i>x</i></sub>FeP<sub>2</sub>O<sub>7</sub> (0 ≤ <i>x</i> ≤ 1) Pyrophosphate Cathode
Li<sub>2</sub>FeP<sub>2</sub>O<sub>7</sub> pyrophosphate
is the
latest phosphate-based polyanionic cathode material operating at 3.5
V (vs Li+/Li). Capable of two-dimensional Li<sup>+</sup>-ion diffusion,
the pyrophosphate has a complex three-dimensional crystal structure,
rich in Li–Fe antisite defects. The electrochemical (de)Âlithiation
of pristine Li<sub>2</sub>FeP<sub>2</sub>O<sub>7</sub> involves permanent
structural rearrangement, as reflected by the voltage drop between
the first and subsequent charging segments. The current article presents
the structural analysis of the electrochemical redox mechanism of
Li<sub>2</sub>FeP<sub>2</sub>O<sub>7</sub> cathode coupling <i>in situ</i> and <i>ex-situ</i> structural characterization.
Contrary to previous reports, it involves a single-phase redox reaction
during (de)Âlithiation cycles involving a minimal <2% volume expansion.
Further, it forms a rare example of cathode showing positive expansion
upon delithiation similar to LiCoO<sub>2</sub>. The mechanism of single-phase
(de)Âlithiation and related (ir)Âreversible structural arrangement is
elucidated
Fe<sup>3+</sup>/Fe<sup>2+</sup> Redox Couple Approaching 4 V in Li<sub>2–<i>x</i></sub>(Fe<sub>1–<i>y</i></sub>Mn<sub><i>y</i></sub>)P<sub>2</sub>O<sub>7</sub> Pyrophosphate Cathodes
Li-metal pyrophosphates have been recently reported as
novel polyanionic
cathode materials with competent electrochemical properties. The current
study presents a detailed analysis of inherent electrochemical properties
of mixed-metal pyrophosphates, Li<sub>2</sub>(Fe<sub>1–<i>y</i></sub>Mn<sub><i>y</i></sub>)ÂP<sub>2</sub>O<sub>7</sub>, synthesized by an optimized solid-state route. They form
a complete solid solution assuming a monoclinic framework with space
group <i>P</i>2<sub>1</sub>/<i>c</i>. The electrochemical
analysis of these single-phase pyrophosphates shows absence of activity
associated with Mn, where near-theoretical redox activity associated
with Fe metal center was realized around 3.5 V. We noticed a closer
look revealed the gradual substitution of Mn into parent Li<sub>2</sub>FeP<sub>2</sub>O<sub>7</sub> phase triggered a splitting of Fe<sup>3+</sup>/Fe<sup>2+</sup> redox peak and partial upshifting in Fe<sup>3+</sup>/Fe<sup>2+</sup> redox potentials nearing 4.0 V. Introduction
of Mn into the pyrophosphate structure may stabilize the two distinct
Fe<sup>3+</sup>/Fe<sup>2+</sup> redox reactions by Fe ions in octahedral
and trigonal-bipyramidal sites. Increase of the Gibb’s free
energy at charged state by introducing Li<sup>+</sup>–Fe<sup>3+</sup> and/or Li vacancy–Mn<sup>2+</sup> pairs can be the
root cause behind redox upshift. The underlying electrochemical behavior
has been examined to assess these mixed-metal pyrophosphates for usage
in Li-ion batteries
Sacrificial Anion Reduction Mechanism for Electrochemical Stability Improvement in Highly Concentrated Li-Salt Electrolyte
Li-salt concentration has been recently
proposed as an important
control parameter of reduction stability of electrolytes in lithium-ion
battery (LIB). Here we theoretically investigated low (LC) and high
(HC) concentration systems of LiNÂ(SO<sub>2</sub>CF<sub>3</sub>)<sub>2</sub> (Li-TFSA) salt in acetonitrile (AN) solution, to elucidate
the mechanism of improving the low reduction stability of AN at the
HC condition, by density functional theory based molecular dynamics
(DFT-MD) sampling of the solvation character with extra electron(s).
We demonstrated that TFSA anions sacrificially accept the reductive
electron at the HC condition, which is ascribed to formation of specific
network structure and the resulting shift of electron affinity of
the anions. We also found that, even in the LC condition, TFSA eventually
decomposes with one electron reduction. This sacrificial anion reduction
hinders two electron reductive decomposition of AN, leading to improved
electrochemical stability. The mechanism may give a guiding principle
for the design of better LIB electrolytes
Kröhnkite-Type Na<sub>2</sub>Fe(SO<sub>4</sub>)<sub>2</sub>·2H<sub>2</sub>O as a Novel 3.25 V Insertion Compound for Na-Ion Batteries
Kröhnkite-Type
Na<sub>2</sub>Fe(SO<sub>4</sub>)<sub>2</sub>·2H<sub>2</sub>O
as a Novel 3.25 V Insertion Compound
for Na-Ion Batterie
Increased Conductivity in the Metastable Intermediate in Li<sub><i>x</i></sub>FePO<sub>4</sub> Electrode
With increasing concerns about energy
and environmental issues,
lithium ion batteries are now penetrating into large-scale applications
such as electric vehicles. As an electrode reaction process, it is
generally believed that two-phase reaction with structural rearrangement
and large lattice mismatch impedes high-rate capability. However,
Li<sub><i>x</i></sub>FePO<sub>4</sub>, with its two-phase
reaction between LiFePO<sub>4</sub> and FePO<sub>4</sub>, exhibits
an exceptional high-rate performance. In this article, after confirming
the existence of a single-phase reaction even under moderate rates,
we demonstrate an approximately 2 orders of magnitude increase of
the conductivity for the quenched intermediate Li<sub>0.6</sub>FePO<sub>4</sub>. In addition to the widely accepted strain relaxation effect
at the two-phase interface, the dramatically increased conductivity
due to polaron/lithium carrier density increase in the intermediate
phase should be highlighted as an important factor to accelerate the
electrode reaction of olivine Li<sub><i>x</i></sub>FePO<sub>4</sub>
Phase Diagram of Olivine Na<sub><i>x</i></sub>FePO<sub>4</sub> (0 < <i>x</i> < 1)
The composition–temperature
phase diagram of cathode material
Na<sub><i>x</i></sub>FePO<sub>4</sub> in the olivine phase
for sodium-ion battery has been determined. Samples were prepared
by solid-state synthetic, electrochemical and chemical oxidation/reduction
methods. Powder X-ray diffraction and Mössbauer spectroscopies
were employed to investigate the phase behavior. At room temperature,
despite the resemblance to the Li<sub><i>x</i></sub>FePO<sub>4</sub> structure, the solubility limit of alkali metal (sodium)
vacancy in Na<sub><i>x</i></sub>FePO<sub>4</sub> is found
to be large. In the range 2/3 < <i>x</i> < 1 Na<sub><i>x</i></sub>FePO<sub>4</sub> is found to be a solid-solution
phase. Two distinguished Fe<sup>2+</sup> sites in the solid-solution
phase were found by Mössbauer spectroscopy. <i>Ab initio</i> calculations reproduce the quadrupole splitting constants and suggest
large distortion of the Fe<sup>2+</sup> octahedra. High-temperature <i>in situ</i> X-ray diffraction suggests a completely different
phase diagram of sodium olivine with a much more stable nature of
the intermediate at <i>x</i> = 2/3 in comparison to the
lithium one
Kinetics of Nucleation and Growth in Two-Phase Electrochemical Reaction of Li<sub><i>x</i></sub>FePO<sub>4</sub>
The kinetics of a two-phase electrochemical reaction in Li<sub><i>x</i></sub>FePO<sub>4</sub> was investigated by potential-step
chronoamperometry under various experimental conditions: amplitude
of potential step, direction of potential step, particle size, and
thickness of composite electrodes. Only under a small potential step
(10 mV) applied to large Li<sub><i>x</i></sub>FePO<sub>4</sub> particles (203 nm), the chronoamperogram showed a momentary current
increase, followed by gradual decline, indicating that the nucleation
and growth governed the electrode kinetics. In that condition, the
chronoamperogram was analyzed with the Kolmogorov–Johnson–Mehl–Avrami
(KJMA) model, which describes the kinetics of phase transition. The
obtained Avrami exponent of ca. 1.1 indicates that the phase transition
proceeds with a one-dimensional phase-boundary movement, which is
consistent with the previously reported mechanism. From the temperature
dependence of the obtained rate constant, the activation energy of
the phase-boundary movement in Li<sub><i>x</i></sub>FePO<sub>4</sub> was estimated to be 42 and 40 kJ mol<sup>–1</sup> in
cathodic and anodic reactions, respectively
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