15 research outputs found
Origin of Vanadium Site Sequential Oxidation in K<sub><i>x</i></sub>VPO<sub>4</sub>F<sub>1ā<i>y</i></sub>O<sub><i>y</i></sub>
M-ion
batteries (M = Li, Na, K ...) positive electrode materials
most often operate through the reversible oxidation of transition-metal
ions. In complex materials involving many transition metals or many
redox centers, understanding the sequence in which they participate
to the reaction is not trivial but is often necessary to explain the
electrochemical properties. Mixed anion vanadium phosphates, such
as KVPO4F0.5O0.5, are known to contain
two different redox entities that are V3+O4F2 and V3+O5F āionicā entities
on the one hand and {V4+O}O5 and {V4+O}O4F ācovalentā vanadyl-type
units on the other hand. However, their participation to the redox
mechanism occurring during the charge of this material has never been
studied. Here, we use V K-edge X-ray absorption spectroscopy to unveil
the redox mechanism of KVPO4F1āyOy (y = 0, 0.5,
1), performing data analysis via a chemometric approach. With XAS
being very sensitive to the oxidation state and bond length, it was
found that the ionic V3+āF units oxidize at a lower
potential than the covalent {V4+O} ones, which
is surprising considering the high electronegativity of fluoride anions
but is consistent with the redox potential observed for KVPO4F and KVOPO4. Further, ab initio calculations
and ex situ X-ray diffraction analyses allowed an
atomistic description of the redox mechanism with the sequential oxidation
of the cis V site before the trans V site in KVPO4F upon charge. Finally, the complete atomically
resolved redox mechanism of KVPO4F0.5O0.5 is proposed
Simulation of NMR Fermi Contact Shifts for Lithium Battery Materials: The Need for an Efficient Hybrid Functional Approach
In the context of the development of NMR Fermi contact
shift calculations
for assisting structural characterization of battery materials, we
propose an accurate, efficient, and robust approach based on the use
of an all electron method. The full-potential linearized augmented
plane wave method, as implemented in the WIEN2k code, is coupled with
the use of hybrid functionals for the evaluation of hyperfine field
quantities. The WIEN2k code uses an autoadaptive basis set that is
highly accurate for the determination of the hyperfine field. Furthermore
the implementation of an onsite version for the HartreeāFock
exchange offers the possibility to use hybrid functional schemes at
no additional computational cost. In this paper, NMR Fermi contact
shifts for lithium are studied in different classes of paramagnetic
materials that present an interest in the field of Li-ion batteries:
olivine LiMPO<sub>4</sub> (M = Mn, Fe, Co, and Ni), anti-NASICON type
Li<sub>3</sub>M<sub>2</sub>(PO<sub>4</sub>)<sub>3</sub> (M = Fe and
V), and antifluorite-type Li<sub>6</sub>CoO<sub>4</sub>. Making use
of the possibility to apply partial hybrid functionals either only
on the magnetic atom or also on the anionic species, we evidence the
role played by oxygen atoms on polarization mechanisms. Our method
is quite general for an application on various types of materials.
Furthermore, it is very competitive compared to the other methods
recently proposed that are based either on a plane wave basis set
with a PAW implementation or on an LCAO one with a full potential
description
P2-Na<sub><i>x</i></sub>Mn<sub>1/2</sub>Fe<sub>1/2</sub>O<sub>2</sub> Phase Used as Positive Electrode in Na Batteries: Structural Changes Induced by the Electrochemical (De)intercalation Process
The
electrochemical properties of the P2-type Na<sub><i>x</i></sub>Mn<sub>1/2</sub>Fe<sub>1/2</sub>O<sub>2</sub> (<i>x</i> = 0.62) phase used as a positive electrode in Na batteries were
tested in various voltage ranges at <i>C</i>/20. We show
that, even if the highest capacity is obtained for the first cycles
between 1.5 and 4.3 V, the best capacity after 50 cycles is obtained
while cycling between 1.5 and 4.0 V (120 mAh g<sup>ā1</sup>). The structural changes occurring in the material during the (de)Āintercalation
were studied by operando in situ X-ray powder diffraction (XRPD) and
ex situ synchrotron XRPD. We show that a phase with an orthorhombic
Pā²2-type structure is formed for <i>x</i> ā
1, due to the cooperative JahnāTeller effect of the Mn<sup>3+</sup> ions. P2 structure type stacking is observed for 0.35 < <i>x</i> < 0.82, while above 4.0 V, a new phase appears. A full
indexation of the XRPD pattern of this latter phase was not possible
because of the broadening of the diffraction peaks. However, a much
shorter interslab distance was found that may imply a gliding of the
MO<sub>2</sub> slab occurring at high voltage. Raman spectroscopy
was used as a local probe and showed that in this new phase the MO<sub>2</sub> layers are maintained, but the phase exhibits a strong degree
of disorder
DFT+U Calculations and XAS Study: Further Confirmation of the Presence of CoO<sub>5</sub> Square-Based Pyramids with IS-Co<sup>3+</sup> in Li-Overstoichiometric LiCoO<sub>2</sub>
LiCoO<sub>2</sub>, one of the major
positive electrode materials
for Li-ion batteries, can be synthesized with excess Li. Previous
experimental work suggested the existence of intermediate spin (IS)
Co<sup>3+</sup> ions in square-based pyramids to account for the defect
in this material. We present here a theoretical study based on density
functional theory (DFT) calculations together with an X-ray absorption
spectroscopy (XAS) experimental study. In the theoretical study, a
hypothetical Li<sub>4</sub>Co<sub>2</sub>O<sub>5</sub> material, where
all the Co ions are in pyramids, was initially considered as a model
material. Using DFT+U, the intermediate spin state of the Co<sup>3+</sup> ions is found stable for U values around 1.5 eV. The crystal and
electronic structures are studied in detail, showing that the defect
must actually be considered as a pair of such square-based pyramids,
and that CoāCo bonding can explain the position of Co in the
basal plane. Using a supercell corresponding to more diluted defects
(as in the actual material), the calculations show that the IS state
is also stabilized. In order to investigate experimentally the change
in the electronic structure in the Li-overstoichiometric LiCoO<sub>2</sub>, we used X-ray absorption near edge structure (XANES) spectroscopy
and propose an interpretation of the O Kedge spectra based on the
DFT+U calculations, that fully supports the presence of pairs of intermediate
spin state Co<sup>3+</sup> defects in Li-overstoichiometric LiCoO<sub>2</sub>
Iron(III) Phosphates Obtained by Thermal Treatment of the Tavorite-Type FePO<sub>4</sub>Ā·H<sub>2</sub>O Material: Structures and Electrochemical Properties in Lithium Batteries
Thermal treatment of the Tavorite-type material FePO<sub>4</sub>Ā·H<sub>2</sub>O leads to the formation of two crystallized
iron
phosphates, very similar in structure. Their structural description
is proposed taking into account results obtained from complementary
characterization tools (thermal analyses, diffraction, and spectroscopy).
These structures are similar to that of the pristine material FePO<sub>4</sub>Ā·H<sub>2</sub>O: iron atoms are distributed between the
chains of corner-sharing FeO<sub>6</sub> octahedra observed in FePO<sub>4</sub>Ā·H<sub>2</sub>O and the octahedra from the tunnels previously
empty, in good agreement with the formation of a Fe<sub>4/3</sub>PO<sub>4</sub>(OH)-type phase. The formation of an extra disordered phase
was also proposed. These samples obtained by thermal-treatment of
FePO<sub>4</sub>Ā·H<sub>2</sub>O also intercalate lithium ions
through the reduction of Fe<sup>3+</sup> to Fe<sup>2+</sup> at an
average voltage of ā¼2.6 V (vs Li<sup>+</sup>/Li), with a good
cyclability and a reversible capacity around 120 mA h g<sup>ā1</sup> (>160 mA h g<sup>ā1</sup> during the first discharge)
Self-Discharge Mechanism of High-Voltage KVPO<sub>4</sub>F for KāIon Batteries
Current performances of Li-, Na-, or K-ion batteries
are mainly
limited by the specific capacity of the positive electrode. Therefore,
it is important to reach the highest capacity possible for a given
electrode material. Here, we investigate the performance limitation
of KVPO4F, a prospective material for K-ion batteries,
which can deliver only 80% of its theoretical capacity. We discover
that the capacity limitation of KVPO4F is related to a
kinetic competition between K+ deinsertion and side reactions
ascribed to the electrolyte degradation at high potentials. Homeotypic
VPO4F can be obtained from KVPO4F through a
chemical deintercalation process, which disproves a possible structural
limitation or instability. The deintercalated compound was characterized
by electron and X-ray diffraction, X-ray absorption spectroscopy,
and nuclear magnetic resonance spectroscopy. Despite the structural
stability, a spontaneous reaction occurs between the deintercalated
KxVPO4F (x 6 in ethylene
carbonate/diethylene carbonate), with an electron transfer to vanadium
compensated by K+ intercalation. This reaction leads to
self-discharge until the open circuit potential is lower than 4.7
V versus K+/K, corresponding to the K0.5VPO4F composition
V<sup>IV</sup> Disproportionation Upon Sodium Extraction From Na<sub>3</sub>V<sub>2</sub>(PO<sub>4</sub>)<sub>2</sub>F<sub>3</sub> Observed by Operando Xāray Absorption Spectroscopy and Solid-State NMR
Among
the series of polyanionic positive electrodes for sodium-ion
batteries having the general formula Na<sub>3</sub>V<sub>2</sub>(PO<sub>4</sub>)<sub>2</sub>F<sub>3ā<i>y</i></sub>O<sub><i>y</i></sub> (0 ā¤ <i>y</i> ā¤
2), the composition Na<sub>3</sub>V<sub>2</sub>(PO<sub>4</sub>)<sub>2</sub>F<sub>3</sub> (<i>y</i> = 0) has the highest theoretical
energy that offers competitive electrochemical performances compared
to sodium transition metal oxides. Recently, the structural phase
diagram from Na<sub>3</sub>V<sub>2</sub>(PO<sub>4</sub>)<sub>2</sub>F<sub>3</sub> to Na<sub>1</sub>V<sub>2</sub>(PO<sub>4</sub>)<sub>2</sub>F<sub>3</sub> has been thoroughly investigated by operando
synchrotron X-ray diffraction revealing an unexpected structural feature
for the end member composition. In fact, the crystal structure of
Na<sub>1</sub>V<sub>2</sub>(PO<sub>4</sub>)<sub>2</sub>F<sub>3</sub> has two very different vanadium environments within each bioctahedron
that suggests a charge disproportionation of two V<sup>IV</sup> into
V<sup>III</sup> and V<sup>V</sup>. This work shows an operando X-ray
absorption spectroscopy at vanadium K edge during the electrochemical
extraction of Na<sup>+</sup> in order to monitor the redox processes
involved in this compound. The large data set provided by this experiment
has been processed by the principal component analysis combined with
multivariate curve resolution. The results suggest that the bioctahedra
have to be considered as the basic structural unit. The peculiar geometry
of this material combined with the mixed vanadium valence, directly
investigated here along the reaction, seems to allow original electronic
configurations. In particular, the two vanadium sites into the basic
bioctahedra unit evolve from V<sup>III</sup>āV<sup>III</sup> to V<sup>III</sup>āV<sup>IV</sup> and to a final V<sup>III</sup>āV<sup>IV</sup> configuration. These observations are completed
with <sup>51</sup>V NMR sensitive to diamagnetic V<sup>V</sup>
Simultaneous Reduction of Co<sup>3+</sup> and Mn<sup>4+</sup> in P2-Na<sub>2/3</sub>Co<sub>2/3</sub>Mn<sub>1/3</sub>O<sub>2</sub> As Evidenced by Xāray Absorption Spectroscopy during Electrochemical Sodium Intercalation
Sodium intercalation in P2-Na<sub>2/3</sub>Co<sub>2/3</sub>Mn<sub>1/3</sub>O<sub>2</sub> (obtained
by a coprecipitation method) was
investigated by ex situ and in situ X-ray absorption spectroscopy.
The electronic transitions at the O K-edge and the charge compensation
mechanism, during the sodium intercalation process, were elucidated
by combining Density Function Theory (DFT) calculations and X-ray
absorption spectroscopy (XAS) data. The pre-edge of the oxygen K-edge
moves to higher energy while the integrated intensity dramatically
decreases, indicating that the population of holes in O 2p states
is reduced with increasing numbers of sodium ions. From the K-edge
and L-edge observations, the oxidation states of pristine Co and Mn
were determined to be +III and +IV, respectively. The absorption energy
shifts to lower positions during the discharging process for both
the Co and the Mn edges, suggesting that the redox pairs, that is,
Co<sup>3+</sup>/Co<sup>2+</sup> and Mn<sup>4+</sup>/Mn<sup>3+</sup>, are both involved in the reaction
Oxidation under Air of Tavorite LiVPO<sub>4</sub>F: Influence of Vanadyl-Type Defects on Its Electrochemical Properties
Tavorite-type
compositions offer a very rich crystal chemistry,
among which LiV<sup>III</sup>PO<sub>4</sub>F has the highest theoretical
energy density (i.e., 655 Wh/kg). In this article, an in-depth study
of vanadyl-type defects generated by temperature-controlled oxidation
of LiV<sup>III</sup>PO<sub>4</sub>F under air is proposed, and the
influence of the defects on the electrochemical properties is demonstrated.
A combination of high resolution synchrotron diffraction, infrared
spectroscopy, and magic angle spinning nuclear magnetic resonance
was used to fully characterize the materials thus generated, from
their average long-range structure to their local structure with the
presence of defects. The increase of the annealing temperature tends
to substitute oxygen for fluorine with the formation of a series of
LiVPO<sub>4</sub>F<sub>1ā<i>x</i></sub>O<sub><i>x</i></sub> compositions. The miscibility domains appear to
be narrow at the two ends of the solid solution (i.e., in the composition
ranges LiVPO<sub>4</sub>F<sub>[1ā0.9]</sub>O<sub>[0ā0.1]</sub> and LiVPO<sub>4</sub>F<sub>[0ā0.1]</sub>O<sub>[1ā0.9]</sub>). The presence of vanadyl-type defects obtained as localized or
more extended ones, depending on the annealing conditions, affects
drastically the electrochemical properties of these Tavorite LiVPO<sub>4</sub>F-type materials
Vanadium Clustering/Declustering in P2āNa<sub>1/2</sub>VO<sub>2</sub> Layered Oxide
The
new layered phase P2āNa<sub>1/2</sub>VO<sub>2</sub> has
been synthesized by sodium electrochemical deintercalation. Its structure
has been studied by high resolution powder diffraction, pair distribution
function analysis, and nuclear magnetic resonance spectroscopy between
300 and 350 K. An increase of 2 orders of magnitude in its electronic
conductivity has been observed at approximately 322 K, and a structural
transition has been found to occur simultaneously. The arrangement
of sodium ordering in P2āNa<sub>1/2</sub>VO<sub>2</sub>, which
maximizes sodiumāsodium distances to lower electrostatic repulsions
between alkali ions, is found to be unchanged across this transition.
At room temperature, high resolution powder diffraction and pair distribution
function analysis reveal the triangular lattice formed by vanadium
ions to be distorted by the formation of pseudotrimers clusters with
vanadiumāvanadium distances as short as 2.581 Ć
. Above
the transition, the pseudotrimers disappear and the triangular vanadium
lattice becomes more regular with a mean vanadiumāvanadium
distance of ā¼2.88 Ć
. At 350 K, the increase in P2āNa<sub>1/2</sub>VO<sub>2</sub> electronic conductivity is due to enhanced
charge transport resulting from the declustering of vanadium ions.
These results highlight how sodium ordering between the MO<sub>2</sub> layers and the electronic transport within the MO<sub>2</sub> layers
are intimately correlated in Na<sub><i>x</i></sub>MO<sub>2</sub>-type sodium-layered oxides