12 research outputs found
Electronic Structure of Sodium Superoxide Bulk, (100) Surface, and Clusters using Hybrid Density Functional: Relevance for NaāO<sub>2</sub> Batteries
Clarifying
the electronic structure of sodium superoxide (NaO<sub>2</sub>) is
a key step in understanding the electrochemical behavior
of NaāO<sub>2</sub> batteries. Here we report a density functional
theory study to explore the effect of atomic structure and morphology
on the electronic properties of different model systems: NaO<sub>2</sub> bulk, (100) surface, and small (NaO<sub>2</sub>)<sub><i>n</i></sub> clusters (<i>n</i> = 3ā8). We found that
a correct description of the open-shell 2p electrons of O<sub>2</sub><sup>ā</sup> requires the use of a hybrid functional, which
reveals a clear insulating nature of all of the investigated systems.
This sheds light onto the capacity limitations of pure NaO<sub>2</sub> as a discharge product and highlights the need for developing new
strategies to enhance its electron transport in the optimization of
NaāO<sub>2</sub> cells
Silicon-Reduced Graphene Oxide Self-Standing Composites Suitable as Binder-Free Anodes for Lithium-Ion Batteries
Silicon-reduced
graphene oxide (Si-rGO) composites processed as
self-standing aerogels (0.2 g cm<sup>ā3</sup>) and films (1.5
g cm<sup>ā3</sup>) have been prepared by the thermal reduction
of composites formed between silicon nanoparticles and a suspension
of graphene oxide (GO) in ethanol. The characterization of the samples
by different techniques (X-ray diffraction, Raman, thermogravimetric
analysis, and scanning electron microscopy) show that in both cases
the composites are formed by rGO sheets homogeneously decorated with
50 nm silicon nanoparticles with silicon contents of ā¼40% wt.
The performances of these self-standing materials were tested as binder-free
anodes in lithium-ion batteries (LIBs) in a half cell configuration
under two different galvanostatic chargeādischarge cutoff voltages
(75 and 50 mV). The results show that the formation of a solid electrolyte
interphase (SEI) is favored in composites processed as aerogels due
to its large exposed surface, which prevents the activation of silicon
when they are cycled within the 2 to 0.075 V voltage windows. It is
also found that the composites processed in the form of self-standing
films exhibit good stability over the first 100 cycles, high reversible
specific capacity per mass of electrode (ā¼750 mAh g<sup>ā1</sup>), areal capacities that reach 0.7 mAh cm<sup>ā2</sup>, and
high Coulombic efficiencies (80% for the first chargeādischarge
cycle and over 99% in the subsequent cycles)
Toward Safe and Sustainable Batteries: Na<sub>4</sub>Fe<sub>3</sub>(PO<sub>4</sub>)<sub>2</sub>P<sub>2</sub>O<sub>7</sub> as a Low-Cost Cathode for Rechargeable Aqueous Na-Ion Batteries
The
electrochemical properties of Na<sub>4</sub>Fe<sub>3</sub>(PO<sub>4</sub>)<sub>2</sub>P<sub>2</sub>O<sub>7</sub> in aqueous and organic
electrolyte are compared under similar conditions. Na<sub>4</sub>Fe<sub>3</sub>(PO<sub>4</sub>)<sub>2</sub>P<sub>2</sub>O<sub>7</sub> is
able to deliver almost the same capacity in both types of electrolytes
despite the smaller electrochemical window entailed by the aqueous
one. As shown by electrochemical impedance spectroscopy (EIS), this
is possible thanks to the lower overpotential that this material exhibits
in aqueous electrolyte. It is shown here that the main contribution
to overpotential in organic electrolyte mainly originates from a SPI
(Solid Permeable Interphase) layer formed below 3.5 V vs Na<sup>+</sup>/Na that acts as a blocking layer and hinders Na<sup>+</sup> diffusion
and that is absent in aqueous electrolyte. Overall, the obtained results
highlight the positive attributes of using low-cost and environmentally
friendly aqueous electrolytes and the challenges to be overcome in
terms of air and moisture stability of the studied material
Composition and Evolution of the Solid-Electrolyte Interphase in Na<sub>2</sub>Ti<sub>3</sub>O<sub>7</sub> Electrodes for Na-Ion Batteries: XPS and Auger Parameter Analysis
Na<sub>2</sub>Ti<sub>3</sub>O<sub>7</sub> is considered a promising negative electrode for Na-ion batteries;
however, poor capacity retention has been reported and the stability
of the solid-electrolyte interphase (SEI) could be one of the main
actors of this underperformance. The composition and evolution of
the SEI in Na<sub>2</sub>Ti<sub>3</sub>O<sub>7</sub> electrodes is
hereby studied by means of X-ray photoelectron spectroscopy (XPS).
To overcome typical XPS limitations in the photoelectron energy assignments,
the analysis of the Auger parameter is here proposed for the first
time in battery materials characterization. We have found that the
electrode/electrolyte interface formed upon discharge, mostly composed
by carbonates and semicarbonates (Na<sub>2</sub>CO<sub>3</sub>, NaCO<sub>3</sub>R), fluorides (NaF), chlorides (NaCl) and polyĀ(ethylene oxide)Ās,
is unstable upon electrochemical cycling. Additionally, solid state
nuclear magnetic resonance (NMR) studies prove the reaction of the
polyvinylidene difluoride (PVdF) binder with sodium. The powerful
approach used in this work, namely Auger parameter study, enables
us to correctly determine the composition of the electrode surface
layer without any interference from surface charging or absolute binding
energy calibration effects. As a result, the suitability for Na-ion
batteries of binders and electrolytes widely used for Li-ion batteries
is questioned here
Flexible and Dynamic Thermal Behavior of Self-Catenated [{Ni<sub>3</sub>(H<sub>2</sub>O)<sub>3</sub>(Bpa)<sub>4</sub>}(V<sub>6</sub>O<sub>18</sub>)]Ā·8H<sub>2</sub>O Constructed from 10-c Heterometallic InorganicāOrganic Clusters
The hydrothermal treatment of NiĀ(NO<sub>3</sub>)<sub>2</sub>Ā·6H<sub>2</sub>O, NaVO<sub>3</sub>, and Bpa (1,2-DiĀ(pyridyl)Āethane)
(C<sub>12</sub>H<sub>12</sub>N<sub>2</sub>) at 120 Ā°C during
3 days
leads to green single crystals of the title compound. The single crystal
X-ray diffraction reveals that [{Ni<sub>3</sub>(H<sub>2</sub>O)<sub>3</sub>(Bpa)<sub>4</sub>}Ā(V<sub>6</sub>O<sub>18</sub>)]Ā·8H<sub>2</sub>O crystallizes in the monoclinic system, <i>P</i>2<sub>1</sub>/<i>c</i> space group, with <i>a</i> = 13.5536 (2), <i>b</i> = 19.0463 (2), <i>c</i> = 27.7435 (3) Ć
, Ī² = 112.3880 (10)Ā°, <i>V</i> = 6622(3) Ć
<sup>3</sup>, with R1Ā(obs) = 0.0558, wR2Ā(obs) =
0.1359, for 10278 observed reflections. The complexity of the crystal
structure is based on different points, as the existence of: both
āgaucheā and ātransā conformations of
the organic ligand, the [V<sub>12</sub>O<sub>36</sub>]<sup>ā12</sup> cycles, formed by 12 corner-sharing VO<sub>4</sub> tetrahedra, and,
finally, the combination of both three-dimensional metalāorganic
and inorganic substructures, giving rise to a self-catenated highly
connected net. The crystallization water molecules are semi-encapsulated
in the channels along the [100] direction, and their loss gives rise
to a dynamical and reversible structural contraction. Moreover, after
the removal of the crystallization water molecules, the compound exhibits
a negative thermal behavior in the 85ā155 Ā°C temperature
range, and irreversible structural transformation due to the loss
of coordinated water molecules up to 200 Ā°C. The IR and UVāvis
spectra were determined for the as-synthesized sample, after the removal
of crystallization water molecules and after the irreversible transformation
due to the loss of coordinated water molecules. The thermal evolution
of Ļ<sub>m</sub> was adjusted to a magnetic model considering
an isotropic dimer plus two NiĀ(II) d<sup>8</sup> isolated octahedra
Flexible and Dynamic Thermal Behavior of Self-Catenated [{Ni<sub>3</sub>(H<sub>2</sub>O)<sub>3</sub>(Bpa)<sub>4</sub>}(V<sub>6</sub>O<sub>18</sub>)]Ā·8H<sub>2</sub>O Constructed from 10-c Heterometallic InorganicāOrganic Clusters
The hydrothermal treatment of NiĀ(NO<sub>3</sub>)<sub>2</sub>Ā·6H<sub>2</sub>O, NaVO<sub>3</sub>, and Bpa (1,2-DiĀ(pyridyl)Āethane)
(C<sub>12</sub>H<sub>12</sub>N<sub>2</sub>) at 120 Ā°C during
3 days
leads to green single crystals of the title compound. The single crystal
X-ray diffraction reveals that [{Ni<sub>3</sub>(H<sub>2</sub>O)<sub>3</sub>(Bpa)<sub>4</sub>}Ā(V<sub>6</sub>O<sub>18</sub>)]Ā·8H<sub>2</sub>O crystallizes in the monoclinic system, <i>P</i>2<sub>1</sub>/<i>c</i> space group, with <i>a</i> = 13.5536 (2), <i>b</i> = 19.0463 (2), <i>c</i> = 27.7435 (3) Ć
, Ī² = 112.3880 (10)Ā°, <i>V</i> = 6622(3) Ć
<sup>3</sup>, with R1Ā(obs) = 0.0558, wR2Ā(obs) =
0.1359, for 10278 observed reflections. The complexity of the crystal
structure is based on different points, as the existence of: both
āgaucheā and ātransā conformations of
the organic ligand, the [V<sub>12</sub>O<sub>36</sub>]<sup>ā12</sup> cycles, formed by 12 corner-sharing VO<sub>4</sub> tetrahedra, and,
finally, the combination of both three-dimensional metalāorganic
and inorganic substructures, giving rise to a self-catenated highly
connected net. The crystallization water molecules are semi-encapsulated
in the channels along the [100] direction, and their loss gives rise
to a dynamical and reversible structural contraction. Moreover, after
the removal of the crystallization water molecules, the compound exhibits
a negative thermal behavior in the 85ā155 Ā°C temperature
range, and irreversible structural transformation due to the loss
of coordinated water molecules up to 200 Ā°C. The IR and UVāvis
spectra were determined for the as-synthesized sample, after the removal
of crystallization water molecules and after the irreversible transformation
due to the loss of coordinated water molecules. The thermal evolution
of Ļ<sub>m</sub> was adjusted to a magnetic model considering
an isotropic dimer plus two NiĀ(II) d<sup>8</sup> isolated octahedra
Thermal Response, Catalytic Activity, and Color Change of the First Hybrid Vanadate Containing Bpe Guest Molecules
Four isomorphic compounds with formula [{Co<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>(Bpe)<sub>2</sub>}Ā(V<sub>4</sub>O<sub>12</sub>)]ĀĀ·4H<sub>2</sub>OĀ·Bpe, CoBpe <b>1</b>; [{CoNiĀ(H<sub>2</sub>O)<sub>2</sub>(Bpe)<sub>2</sub>}Ā(V<sub>4</sub>O<sub>12</sub>)]ĀĀ·4H<sub>2</sub>OĀ·Bpe, CoNiBpe <b>2</b>; [{Co<sub>0.6</sub>Ni<sub>1.4</sub>(H<sub>2</sub>O)<sub>2</sub>(Bpe)<sub>2</sub>}Ā(V<sub>4</sub>O<sub>12</sub>)]ĀĀ·4H<sub>2</sub>OĀ·Bpe, NiCoBpe <b>3</b>; and [{Ni<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>(Bpe)<sub>2</sub>}Ā(V<sub>4</sub>O<sub>12</sub>)]ĀĀ·4H<sub>2</sub>OĀ·Bpe, NiBpe <b>4</b>, have
been obtained by hydrothermal synthesis. The crystal structures of
CoBpe <b>1</b> and NiBpe <b>4</b> were determined by single-crystal
X-ray diffraction (XRD). The Rietveld refinement of CoNiBpe <b>2</b> and NiCoBpe <b>3</b> XRD patterns confirms that those
are isomorphic. The compounds crystallize in the <i>P</i>1Ģ
space group, exhibiting a crystal structure constructed
from inorganic layers pillared by Bpe ligands. The crystal structure
contains intralayer and interlayer channels, in which the crystallization
water molecules and Bpe guest molecules, respectively, are located.
The solvent molecules establish a hydrogen bonding network with the
coordinated water molecules. Thermodiffractometric and thermogravimetric
studies showed that the loss of crystallization and coordinated water
molecules takes place at different temperatures, giving rise to crystal
structure transformations that involve important reduction of the
interlayer distance, and strong reduction of crystallinity. The IR,
Raman, and UVāvis spectra of the as-synthesized and heated
compounds confirm that the structural building blocks and octahedral
coordination environment of the metal centers are maintained after
the structural transformations. The color change and reversibility
of the water molecules uptake/removal were tested showing that the
initial color is not completely recovered when the compounds are heated
at temperatures higher than 200 Ā°C. The thermal evolution of
the magnetic susceptibility indicates one-dimensional antiferromagnetic
coupling of the metal centers at high temperatures. For NiCoBpe <b>3</b> and NiBpe <b>4</b> compounds magnetic ordering is
established at low temperatures, as can be judged by the maxima observed
in the magnetic susceptibilities. CoNiBpe <b>2</b> was proved
as catalyst being active for cyanosilylation reactions of aldehydes
Electrochemical Na Extraction/Insertion of Na<sub>3</sub>V<sub>2</sub>O<sub>2<i>x</i></sub>(PO<sub>4</sub>)<sub>2</sub>F<sub>3ā2<i>x</i></sub>
A mixed-valence
V<sup>3+</sup>/V<sup>4+</sup> composite material
belonging to the Na<sub>3</sub>V<sub>2</sub>O<sub>2<i>x</i></sub>(PO<sub>4</sub>)Ā2F<sub>3ā2<i>x</i></sub>/C
family is synthesized and the electrochemical Na extraction/insertion
mechanism is determined using a combination of high-resolution synchrotron
X-ray diffraction (XRD) data, X-ray absorption spectroscopy (XAS), <sup>23</sup>Na and <sup>19</sup>F solid state nuclear magnetic resonance
(NMR), double titration (for the elucidation of the vanadium oxidation
state), and electrochemical measurements. The vanadium oxidation state
is found to be +3.8 for the as-prepared sample. Detailed analysis
of the cathode structural evolution illustrated that the V<sup>4+</sup>/V<sup>5+</sup> couple is active in this compound during electrochemical
cycling between 2.8 V and 4.3 V. This study demonstrates how the sodium-ion
extraction and insertion pathways in cathode materials can be followed
(and verified) using several experimental techniques, especially when
multiple potential oxidation states are present in the parent compound
Sodium Distribution and Reaction Mechanisms of a Na<sub>3</sub>V<sub>2</sub>O<sub>2</sub>(PO<sub>4</sub>)<sub>2</sub>F Electrode during Use in a Sodium-Ion Battery
Ambient
temperature sodium-ion batteries are emerging as an exciting
alternative to commercially dominant lithium-ion batteries for larger
scale stationary applications. In order to realize such a sodium-ion
battery, electrodes need to be developed, understood, and improved.
Here, Na<sub>3</sub>V<sub>2</sub>O<sub>2</sub>(PO<sub>4</sub>)<sub>2</sub>F is investigated from the perspective of sodium. Reaction
mechanisms for this cathode during battery function include the following:
a region comprising at least three phases with subtly varying sodium
compositions that transform via two two-phase reaction mechanisms,
which appears at the lower potential plateau-like region during both
charge and discharge; an extended solid solution region for majority
of the cycling process, including most of the higher potential plateau;
and a second two-phase region near the highest charge state during
charge and between the first and second plateau-like regions during
discharge. Notably, the distinct asymmetry in the reaction mechanism,
lattice, and volume evolution on charge relative to discharge manifests
an interesting question: Is such an asymmetry beneficial for this
cathode? These reaction mechanisms are inherently related to sodium
evolution, which shows complex behavior between the two sodium crystallographic
sites in this compound that in turn mediate the lattice and reaction
evolution. Thus, this work relates atomic-level sodium perturbations
directly with electrochemical cycling
High-Performance P2-Phase Na<sub>2/3</sub>Mn<sub>0.8</sub>Fe<sub>0.1</sub>Ti<sub>0.1</sub>O<sub>2</sub> Cathode Material for Ambient-Temperature Sodium-Ion Batteries
High-performance
Mn-rich P2-phase Na<sub>2/3</sub>Mn<sub>0.8</sub>Fe<sub>0.1</sub>Ti<sub>0.1</sub>O<sub>2</sub> is synthesized by a
ceramic method, and its stable electrochemical performance is demonstrated. <sup>23</sup>Na solid-state NMR confirms the substitution of Ti<sup>4+</sup> ions in the transition metal oxide layer and very fast Na<sup>+</sup> mobility in the interlayer space. The pristine electrode delivers
a second charge/discharge capacity of 146.57/144.16 mAĀ·hĀ·g<sup>ā1</sup> and retains 95.09% of discharge capacity at the 50th
cycle within the voltage range 4.0ā2.0 V at C/10. At 1C, the
reversible specific capacity still reaches 99.40 mAĀ·hĀ·g<sup>ā1</sup>, and capacity retention of 87.70% is achieved from
second to 300th cycle. In addition, the moisture-exposed electrode
reaches reversible capacities of more than 130 and 80 mAĀ·hĀ·g<sup>ā1</sup> for C/10 and 1C, respectively, with excellent capacity
retention. The correlation between overall electrochemical performance
of both electrodes and crystal structural characteristics are investigated
by neutron powder diffraction. The stability of pristine electrodeās
crystallographic structure during the charge/discharge process has
been investigated by in situ X-ray diffraction, where only a solid
solution reaction occurs within the given voltage range except for
a small biphasic mechanism occurring at or below 2.2 V during the
discharge process. The relatively small substitution (20%) at the
transition metal site leads to stable electrochemical performance,
which is in part derived from the structural stability during electrochemical
cycling. Therefore, the small cosubstitution (e.g., with Ti and Fe)
route suggests a possible new scope for the design of sodium-ion battery
electrodes that are suitable for long-term cycling