9 research outputs found
Grafting Spiropyran Molecular Switches on TiO<sub>2</sub>: A First-Principles Study
To
explore the optoelectronic properties of spiropyran molecular
switches adsorbed onto TiO<sub>2</sub> anatase surfaces, we performed
a density functional theory (DFT)/time-dependent density functional
theory (TD-DFT) study considering the two isomeric forms of the photochromes
anchored by both their sides. A comparison between the features of
the hybrid and isolated systems is proposed to probe the adsorption
effects on both subsystems. This comparison considered, on the one
hand, the density of states and the alignment of the energy levels,
and, on the other hand, the UVâvisible spectra of these systems.
We show that several electronic and optical characteristics of the
hybrid systems are modulated by the open/closed state of the photochromes.
These properties are also modified by the localization of the anchor
group on the photochrome
How Adsorption Onto TiO<sub>2</sub> Modifies the Properties of Multiswitchable DTE Systems: Theoretical Insights
In
order to best employ multiphotochromes as complex molecular
gates, each isomer should ideally have a distinct optical profile
to be selectively addressable. In this ab initio DFT and TD-DFT study, we have modeled the electronic
and optical properties of a series of dithienylethene (DTE) dimers
grafted onto an anatase (101) surface. We seek to investigate how
grafting onto a TiO<sub>2</sub> surface modifies the energy levels
and UVâvisible spectra of the dimers and enhances the asymmetry
of the isomers. By extracting information from the density of states,
we have qualified the distinct degrees of interaction between the
substrate and each isomeric configuration as CO > CC > OC >
OO in
order of decreasing electronic coupling. We subsequently use this
information to interpret the UVâvis spectra computed for the
isomers. The results show that the grafted systems present new peaks
and shifted <i>S</i><sub>1</sub> energies compared with
the isolated photochrome, suggesting that adsorption onto a TiO<sub>2</sub> surface may induce an asymmetric character in the DTE dyad
Elucidation of the Na<sub>2/3</sub>FePO<sub>4</sub> and Li<sub>2/3</sub>FePO<sub>4</sub> Intermediate Superstructure Revealing a Pseudouniform Ordering in 2D
Based
on TEM, synchrotron X-ray diffraction, DFT calculations,
and MoÌssbauer spectroscopy, a unified understanding of the
Na and Li intercalation process in FePO<sub>4</sub> is proposed. The
key to this lies in solving the highly sought-after intermediate A<sub>2/3</sub>FePO<sub>4</sub> (A = Na, Li) superstructures that are characterized
by alkali ions as well as Fe<sup>II</sup>/Fe<sup>III</sup> charge
orderings in a monoclinic three-fold supercell. Formation energies
and electrochemical potential calculations confirm that Na<sub>2/3</sub>FePO<sub>4</sub> and Li<sub>2/3</sub>FePO<sub>4</sub> are stable
and metastable, respectively, and that they yield insertion potentials
in fair agreement with experimental values. The 2/3 NaÂ(Li) and 1/3
vacancy sublattice of the intermediate phases forms a dense (101Ì
)<sub><i>Pnma</i></sub> plane in which the atom/vacancy ordering
is very similar to that predicted for the most uniform distribution
of 1/3 of vacancies in a 2D square lattice. Structural analysis strongly
suggests that the key role of this dense plane is to constrain the
intercalation in the diffusion channels to operate by cooperative
filling of (<i>bc</i>)<sub><i>Pnma</i></sub>.
From a practical point of view, this generalized mechanism highlights
the fact that an interesting strategy for obtaining high-rate FePO<sub>4</sub> materials would consist in designing grains with an enhanced
(101) surface area, thereby offering potential for substantial improvements
with respect to the performance of rechargeable Li and Na batteries
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 HartreeâFock
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
Structural Investigation of α- and ÎČ-Sodium Hexafluoroarsenate, NaAsF<sub>6</sub>, by Variable Temperature X-ray Powder Diffraction and Multinuclear Solid-State NMR, and DFT Calculations
We report the phase transition between the α- and
ÎČ-phases
of NaAsF<sub>6</sub> monitored by DTA, variable temperature <sup>19</sup>F solid-state NMR and temperature controlled X-ray powder diffraction
(XRPD) as well as their crystalline structures determined from XRPD
data. The structural type of ÎČ-NaAsF<sub>6</sub> has been determined
thanks to <sup>19</sup>F and <sup>75</sup>As solid-state NMR experiments. <sup>19</sup>F, <sup>23</sup>Na, and <sup>75</sup>As NMR parameters, including <sup>19</sup>Fâ<sup>75</sup>As <sup>1</sup><i>J</i> coupling,
have been measured for both phases. The <sup>19</sup>F, <sup>23</sup>Na, and <sup>75</sup>As solid-state NMR investigations are in full
agreement with both crystalline structures from a qualitative point
of view. Chemical shielding tensors have been calculated from the
gauge including projector augmented wave approach. The electric field
gradient tensors of <sup>23</sup>Na and <sup>75</sup>As have been
calculated in α-NaAsF<sub>6</sub> from the all-electrons method
and the projector augmented-wave approach. Two difficulties were encountered:
the libration of the rigid and regular AsF<sub>6</sub><sup>â</sup> anions in the ÎČ-phase, highlighted by the atomic anisotropic
displacement parameters for F, which leads to erroneous shortened
AsâF bond length, and the overestimation of the AsâF
bond length with the PBE functional used in the density functional
theory calculations. We show that both difficulties can be overcome
by full optimization and rescaling of the cell parameters of the crystalline
structures. Additionally, a linear correlation is observed between
experimental <sup>23</sup>Na ÎŽ<sub>iso</sub> values and calculated <sup>23</sup>Na Ï<sub>iso</sub> values from previously reported
data and from our own measurements and calculations
Interplay between TiO<sub>2</sub> Surfaces and Organic Photochromes: A DFT Study of Adsorbed Azobenzenes and Diarylethenes
Because
photochromes act as light-induced molecular switches, there
is considerable interest in exporting their molecular functionality
in the solid state in order to develop photoresponsive materials.
In that context, we have carried out a DFT investigation of a series
of photochromic derivatives of <i>trans</i>/<i>cis</i>-azobenzene and open/closed-diarylethene adsorbed onto rutile (110)
and anatase (101) slabs. By varying the auxochromes and the photochromic
state, we examine the trends in the surfaceâadsorbate interplay
in terms of the electronic structure, adsorption geometries, and Bader
charge transfer. Using principal components analysis, we demonstrate
how the dipole moment of the isolated photochrome in the direction
of the anchoring group is the most important predictor of the electronic
structure of the adsorbed system. A key point of this paper is to
show how the energy levels of the isolated photochrome and bare slab
change as a result of adsorption and how first-principles modeling
helps to rationalize and predict these trends
Synthesis and Structure Resolution of RbLaF<sub>4</sub>
The synthesis and structure resolution of RbLaF<sub>4</sub> are
described. RbLaF<sub>4</sub> is synthesized by solid-state reaction
between RbF and LaF<sub>3</sub> at 425 °C under a nonoxidizing
atmosphere. Its crystal structure has been resolved by combining neutron
and synchrotron powder diffraction data refinements (<i>Pnma,</i> <i>a</i> = 6.46281(2) Ă
, <i>b</i> = 3.86498(1)
Ă
, <i>c</i> = 16.17629(4) Ă
, <i>Z</i> = 4). One-dimensional <sup>87</sup>Rb, <sup>139</sup>La, and <sup>19</sup>F MAS NMR spectra have been recorded and are in agreement
with the proposed structural model. Assignment of the <sup>19</sup>F resonances is performed on the basis of both <sup>19</sup>Fâ<sup>139</sup>La <i>J</i>-coupling multiplet patterns observed
in a heteronuclear DQ-filtered <i>J</i>-resolved spectrum
and <sup>19</sup>Fâ<sup>87</sup>Rb HMQC MAS experiments. DFT
calculations of both the <sup>19</sup>F isotropic chemical shieldings
and the <sup>87</sup>Rb, <sup>139</sup>La electric field gradient
tensors using the GIPAW and PAW methods implemented in the CASTEP
code are in good agreement with the experimental values and support
the proposed structural model. Finally, the conductivity of RbLaF<sub>4</sub> and luminescence properties of Eu-doped LaRbF<sub>4</sub> are investigated
Synthesis and Structure Resolution of RbLaF<sub>4</sub>
The synthesis and structure resolution of RbLaF<sub>4</sub> are
described. RbLaF<sub>4</sub> is synthesized by solid-state reaction
between RbF and LaF<sub>3</sub> at 425 °C under a nonoxidizing
atmosphere. Its crystal structure has been resolved by combining neutron
and synchrotron powder diffraction data refinements (<i>Pnma,</i> <i>a</i> = 6.46281(2) Ă
, <i>b</i> = 3.86498(1)
Ă
, <i>c</i> = 16.17629(4) Ă
, <i>Z</i> = 4). One-dimensional <sup>87</sup>Rb, <sup>139</sup>La, and <sup>19</sup>F MAS NMR spectra have been recorded and are in agreement
with the proposed structural model. Assignment of the <sup>19</sup>F resonances is performed on the basis of both <sup>19</sup>Fâ<sup>139</sup>La <i>J</i>-coupling multiplet patterns observed
in a heteronuclear DQ-filtered <i>J</i>-resolved spectrum
and <sup>19</sup>Fâ<sup>87</sup>Rb HMQC MAS experiments. DFT
calculations of both the <sup>19</sup>F isotropic chemical shieldings
and the <sup>87</sup>Rb, <sup>139</sup>La electric field gradient
tensors using the GIPAW and PAW methods implemented in the CASTEP
code are in good agreement with the experimental values and support
the proposed structural model. Finally, the conductivity of RbLaF<sub>4</sub> and luminescence properties of Eu-doped LaRbF<sub>4</sub> are investigated