11 research outputs found
New Hybrid Layered Molybdates Based on <sup>2</sup>/<sub>ā</sub>[Mo<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub>]<sup>2ā</sup> Units (<i>n</i> = 7, 9) with Systematic OrganicāInorganic Interfaces
Two new hybrid organicāinorganic molybdates based
on layered <sup>2</sup>/<sub>ā</sub>[Mo<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub>]<sup>2ā</sup> blocks
and organoammonium cations <sup>+</sup>(Me<sub><i>x</i></sub>H<sub>3ā<i>x</i></sub>N)Ā(CH<sub>2</sub>)<sub>6</sub>(NH<sub>3ā<i>x</i></sub>Me<sub><i>x</i></sub>)<sup>+</sup> (<i>x</i> = 0ā1), namely, (H<sub>3</sub>NĀ(CH<sub>2</sub>)<sub>6</sub>NH<sub>3</sub>)Ā[Mo<sub>7</sub>O<sub>22</sub>]Ā·H<sub>2</sub>O (<b>1</b>) and (MeH<sub>2</sub>NĀ(CH<sub>2</sub>)<sub>6</sub>NH<sub>2</sub>Me)Ā[Mo<sub>9</sub>O<sub>28</sub>] (<b>2</b>), have been synthesized
under hydrothermal conditions. The <sup>2</sup>/<sub>ā</sub>[Mo<sub>9</sub>O<sub>28</sub>]<sup>2ā</sup> unit in <b>2</b> is an unprecedented member of the <sup>2</sup>/<sub>ā</sub>[Mo<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub>]<sup>2ā</sup> family with the <i>n</i> value extended
to 9. The structural filiation between the <sup>2</sup>/<sub>ā</sub>[Mo<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub>]<sup>2ā</sup> (<i>n</i> = 5, 7, 9) blocks is well
established, and their structural similarity with the <sup>2</sup>/<sub>ā</sub>[MoO<sub>3</sub>] slabs in Ī±-MoO<sub>3</sub> is also discussed. Single-crystal X-ray analyses show that the <sup>2</sup>/<sub>ā</sub>[Mo<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub>]<sup>2ā</sup> layers in <b>1</b> and <b>2</b> are pillared in the three-dimensional
networks by the organic cations with a similar connection at the organicāinorganic
interface. In addition, a correlation between the topology of the <sup>2</sup>/<sub>ā</sub>[Mo<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub>]<sup>2ā</sup> blocks in <b>1</b> and <b>2</b> and the overall sizes of the associated
organic cations is pointed out. Finally, the efficiency of Fourier
transform Raman spectroscopy to easily discriminate the different <sup>2</sup>/<sub>ā</sub>[Mo<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub>]<sup>2ā</sup> blocks (<i>n</i> = 5, 7, 9) in hybrid organicāinorganic layered
molybdate materials
is clearly evidenced
New Hybrid Layered Molybdates Based on <sup>2</sup>/<sub>ā</sub>[Mo<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub>]<sup>2ā</sup> Units (<i>n</i> = 7, 9) with Systematic OrganicāInorganic Interfaces
Two new hybrid organicāinorganic molybdates based
on layered <sup>2</sup>/<sub>ā</sub>[Mo<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub>]<sup>2ā</sup> blocks
and organoammonium cations <sup>+</sup>(Me<sub><i>x</i></sub>H<sub>3ā<i>x</i></sub>N)Ā(CH<sub>2</sub>)<sub>6</sub>(NH<sub>3ā<i>x</i></sub>Me<sub><i>x</i></sub>)<sup>+</sup> (<i>x</i> = 0ā1), namely, (H<sub>3</sub>NĀ(CH<sub>2</sub>)<sub>6</sub>NH<sub>3</sub>)Ā[Mo<sub>7</sub>O<sub>22</sub>]Ā·H<sub>2</sub>O (<b>1</b>) and (MeH<sub>2</sub>NĀ(CH<sub>2</sub>)<sub>6</sub>NH<sub>2</sub>Me)Ā[Mo<sub>9</sub>O<sub>28</sub>] (<b>2</b>), have been synthesized
under hydrothermal conditions. The <sup>2</sup>/<sub>ā</sub>[Mo<sub>9</sub>O<sub>28</sub>]<sup>2ā</sup> unit in <b>2</b> is an unprecedented member of the <sup>2</sup>/<sub>ā</sub>[Mo<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub>]<sup>2ā</sup> family with the <i>n</i> value extended
to 9. The structural filiation between the <sup>2</sup>/<sub>ā</sub>[Mo<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub>]<sup>2ā</sup> (<i>n</i> = 5, 7, 9) blocks is well
established, and their structural similarity with the <sup>2</sup>/<sub>ā</sub>[MoO<sub>3</sub>] slabs in Ī±-MoO<sub>3</sub> is also discussed. Single-crystal X-ray analyses show that the <sup>2</sup>/<sub>ā</sub>[Mo<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub>]<sup>2ā</sup> layers in <b>1</b> and <b>2</b> are pillared in the three-dimensional
networks by the organic cations with a similar connection at the organicāinorganic
interface. In addition, a correlation between the topology of the <sup>2</sup>/<sub>ā</sub>[Mo<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub>]<sup>2ā</sup> blocks in <b>1</b> and <b>2</b> and the overall sizes of the associated
organic cations is pointed out. Finally, the efficiency of Fourier
transform Raman spectroscopy to easily discriminate the different <sup>2</sup>/<sub>ā</sub>[Mo<sub><i>n</i></sub>O<sub>3<i>n</i>+1</sub>]<sup>2ā</sup> blocks (<i>n</i> = 5, 7, 9) in hybrid organicāinorganic layered
molybdate materials
is clearly evidenced
Luminescence Properties of Al<sub>2</sub>O<sub>3</sub>:Ti in the Blue and Red Regions: A Combined Theoretical and Experimental Study
Using jointly experimental results and first-principles
calculations,
we unambiguously assign the underlying mechanisms behind two commonly
observed luminescence bands for the Al2O3 material.
Indeed, we show that the red band is associated with a Ti3+ dād transition as expected,
while the blue band is the combination of the Ti3+ + Oā ā Ti4+ + O2ā and
VOā¢+eā ā VOĆ de-excitation processes. Thanks
to our recent developments, which take into account the vibrational
contributions to the electronic transitions in solids, we were able
to simulate the luminescence spectra for the different signatures.
The excellent agreement with the experiment demonstrates that it should
be possible to predict the color of the material with a CIE chromaticity
diagram. We also anticipated the luminescence signature of Al2O3:Ti,Ca and Al2O3:Ti,Be
that were confirmed by experiment
Tuning the Photochromic Properties of Molybdenum Bisphosphonate Polyoxometalates
Seven hybrid organicāinorganic bisphosphonate
molybdenumĀ(VI)
polyoxometalate complexes with the general formula [(Mo<sub>3</sub>O<sub>8</sub>)<sub>4</sub>(O<sub>3</sub>PCĀ(C<sub><i>m</i></sub>H<sub>2<i>m</i></sub>NRRā²Rā³)Ā(O)ĀPO<sub>3</sub>)<sub>4</sub>]<sup>8ā</sup> (<i>m</i> = 3;
R, Rā², and Rā³ = H or CH<sub>3</sub>) and [(Mo<sub>3</sub>O<sub>8</sub>)<sub>2</sub>(O)Ā(O<sub>3</sub>PCĀ(C<sub><i>m</i></sub>H<sub>2<i>m</i></sub>NRRā²Rā³)Ā(O)ĀPO<sub>3</sub>)<sub>2</sub>]<sup>6ā</sup> (<i>m</i> = 3
or 4; R, Rā², and Rā³ = H or CH<sub>3</sub>) have been
synthesized and their structures solved using single-crystal X-ray
diffraction. These compounds are made of a {Mo<sub>12</sub>} or a
{Mo<sub>6</sub>} inorganic core functionalized by various alkylammonium
bisphosphonates, with these ligands differing by the length of their
alkyl chains and the number of methyl groups grafted on the N atom.
The nature of the counter-cations (Na<sup>+</sup>, K<sup>+</sup>,
Rb<sup>+</sup>, Cs<sup>+</sup>, and/or NH<sub>4</sub><sup>+</sup>)
constituting these materials has also been modulated. <sup>31</sup>P NMR spectroscopic studies in aqueous media have shown that all
the dodecanuclear complexes reported here are stable in solution,
whereas for the hexanuclear compounds, a dynamic equilibrium between
two isomers has been evidenced, and the corresponding standard thermodynamic
parameters determined for one of them. The electrochemical properties
of six representative compounds of this family have been investigated.
It has been found that the Mo<sup>6+</sup>/Mo<sup>5+</sup> reduction
potential is similar for all the polyoxometalates studied. Besides,
it is shown that electrochemical cycling is an efficient method for
the deposition of these compounds on a surface. The photochromic properties
of all the complexes reported herein have been studied in the solid
state. Under irradiation in the near ultraviolet (UV), the {Mo<sub>12</sub>} systems shift from white to reddish-brown, while the {Mo<sub>6</sub>} compounds develop a purple coloration. The coloration kinetics
has been systematically quantified and the optical band gaps, the salient coloration kinetic parameters and the coloration kinetic
half-life times have been determined. This has evidenced that several
of these materials develop very strong and rapid UV-induced color
changes, with remarkable coloration contrasts. Finally, the optical
properties of these systems are discussed in light of several salient
parameters as the POM topology, the nature of the grafted bisphosphonate
ligand, and the design of the hydrogen-bonding network at the organicāinorganic
interface
Persistent Type-II Multiferroicity in Nanostructured MnWO<sub>4</sub> Ceramics
Persistent
Type-II Multiferroicity in Nanostructured
MnWO<sub>4</sub> Ceramic
Incorporation of JahnāTeller Cu<sup>2+</sup> Ions into Magnetoelectric Multiferroic MnWO<sub>4</sub>: Structural, Magnetic, and Dielectric Permittivity Properties of Mn<sub>1ā<i>x</i></sub>Cu<sub><i>x</i></sub>WO<sub>4</sub> (<i>x</i> ā¤ 0.25)
Polycrystalline
samples of Mn<sub>1ā<i>x</i></sub>Cu<sub><i>x</i></sub>WO<sub>4</sub> (<i>x</i> ā¤ 0.5)
have been prepared by a solid-state synthesis as well
as from a citrate synthesis at moderate temperature (850 Ā°C).
The goal is to study changes in the structural, magnetic, and dielectric
properties of magnetoelectric type-II multiferroic MnWO<sub>4</sub> caused by replacing JahnāTeller-inactive Mn<sup>2+</sup> (d<sup>5</sup>, <i>S</i> = 5/2) ions with JahnāTeller-active
Cu<sup>2+</sup> (d<sup>9</sup>, <i>S</i> = 1/2) ions. Combination
of techniques including scanning electron microscopy, powder X-ray
and neutron diffraction, and Raman spectroscopy demonstrates that
the polycrystalline samples with low copper content 0 ā¤ <i>x</i> ā¤ 0.25 are solid solution that forms in the monoclinic <i>P</i>2/c space group. Rietveld analyses indicate that Cu atoms
substitutes for Mn atoms at the Mn crystallographic site of the MnWO<sub>4</sub> structure and suggest random distributions of JahnāTeller-distorted
CuO<sub>6</sub> octahedra in the solid solution. Magnetic susceptibility
reveals that only 5% of Cu substitution suppresses the nonpolar collinear
AF1 antiferromagnetic structure observed in pure MnWO<sub>4</sub>.
Type-II multiferroicity survives a weak Cu substitution rate (<i>x</i> < 0.15). Multiferroic transition temperature and NeĢel
temperature increase as the amount of Cu increases. New trends in
some of the magnetic properties and in dielectric behaviors are observed
for <i>x</i> = 0.20 and 0.25. Careful analysis of the magnetic
susceptibility reveals that the incorporation of Cu into MnWO<sub>4</sub> strengthens the overall antiferromagnetic interaction and
reduces the magnetic frustration
Pair Distribution Function and Density Functional Theory Analyses of Hydrogen Trapping by Ī³āMnO<sub>2</sub>
In the presence of āAg<sub>2</sub>Oā as a promoter,
Ī³-MnO<sub>2</sub> traps dihydrogen in its (2 Ć 1) and (1
Ć 1) tunnels. The course of this reaction was examined by analyzing
the X-ray diffraction patterns of the H<sub><i>x</i></sub>MnO<sub>2</sub>/āAg<sub>2</sub>Oā system (0 ā¤ <i>x</i> < 1) on the basis of pair distribution function and
density functional theory (DFT) analyses. Hydrogen trapping occurs
preferentially in the (2 Ć 1) tunnels of Ī³-MnO<sub>2</sub>, which is then followed by that in the (1 Ć 1) tunnels. Our
DFT analysis shows that this process is thermodynamically favorable
Photochromic Properties of Polyoxotungstates with Grafted Spiropyran Molecules
The first systems associating in
a single molecule polyoxotungstates (POTs) and photochromic organic
groups have been elaborated. Using the (TBA)<sub>4</sub>Ā[PW<sub>11</sub>O<sub>39</sub>Ā{SnĀ(C<sub>6</sub>H<sub>4</sub>I)}]
precursor, two hybrid organicāinorganic species where a spiropyran
derivative (SP) has been covalently grafted onto a {PW<sub>11</sub>Sn} fragment via a Sonogashira coupling have been successfully obtained.
Alternatively, a complex containing a silicotungstate {PW<sub>11</sub>Si<sub>2</sub>} unit connected to two spiropyran entities has been
characterized. The purity of these species has been assessed using
several techniques, including <sup>1</sup>H and <sup>31</sup>P NMR
spectroscopy, mass spectrometry, and electrochemical measurements.
The optical properties of the hybrid materials have been investigated
both in solution and in the solid state. These studies reveal that
the grafting of SPs onto POTs does not significantly alter the photochromic
behavior of the organic chromophore in solution. In contrast, these
novel hybrid SPāPOT materials display highly effective solid-state
photochromism from neutral SP molecules initially nonphotochromic
in the crystalline state. The photoresponses of the SPāPOT
systems in the solid state strongly depend on the nature and the number
of grafted SP groups
Photochromic Properties of Polyoxotungstates with Grafted Spiropyran Molecules
The first systems associating in
a single molecule polyoxotungstates (POTs) and photochromic organic
groups have been elaborated. Using the (TBA)<sub>4</sub>Ā[PW<sub>11</sub>O<sub>39</sub>Ā{SnĀ(C<sub>6</sub>H<sub>4</sub>I)}]
precursor, two hybrid organicāinorganic species where a spiropyran
derivative (SP) has been covalently grafted onto a {PW<sub>11</sub>Sn} fragment via a Sonogashira coupling have been successfully obtained.
Alternatively, a complex containing a silicotungstate {PW<sub>11</sub>Si<sub>2</sub>} unit connected to two spiropyran entities has been
characterized. The purity of these species has been assessed using
several techniques, including <sup>1</sup>H and <sup>31</sup>P NMR
spectroscopy, mass spectrometry, and electrochemical measurements.
The optical properties of the hybrid materials have been investigated
both in solution and in the solid state. These studies reveal that
the grafting of SPs onto POTs does not significantly alter the photochromic
behavior of the organic chromophore in solution. In contrast, these
novel hybrid SPāPOT materials display highly effective solid-state
photochromism from neutral SP molecules initially nonphotochromic
in the crystalline state. The photoresponses of the SPāPOT
systems in the solid state strongly depend on the nature and the number
of grafted SP groups
Novel Soft-Chemistry Route of Ag<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub>Ā·2H<sub>2</sub>O Nanowires and in Situ Photogeneration of a Ag@Ag<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub>Ā·2H<sub>2</sub>O Plasmonic Heterostructure
Ultrathin
Ag<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub>Ā·2H<sub>2</sub>O nanowires
(NWs) were synthesized by soft chemistry under
atmospheric pressure from a hybrid organicāinorganic polyoxometalate
(CH<sub>3</sub>NH<sub>3</sub>)<sub>2</sub>[Mo<sub>7</sub>O<sub>22</sub>] and characterized by powder X-ray diffraction, DSC/TGA analyses,
FT-IR and FT-Raman spectroscopies, scanning electron microscopy (SEM),
and transmission electron microscopy (TEM). Their diameters are a
few tens of nanometers and hence much thinner than that found for
silver molybdates commonly obtained under hydrothermal conditions.
The optical properties of Ag<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub>Ā·2H<sub>2</sub>O NWs before and after UV irradiation were investigated
by UVāvisāNIR diffuse reflectance spectroscopy revealing,
in addition to photoreduction of Mo<sup>6+</sup> to Mo<sup>5+</sup> cations, in situ photogeneration of well-dispersed silver Ag<sup>0</sup> nanoparticles on the surface of the NWs. The resulting Ag@Ag<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub>Ā·2H<sub>2</sub>O heterostructure
was confirmed by electron energy-loss spectroscopy (EELS), X-ray photoelectron
spectroscopy (XPS), and Auger spectroscopy. Concomitant reduction
of Mo<sup>6+</sup> and Ag<sup>+</sup> cations under UV excitation
was discussed on the basis of electronic band structure calculations.
The Ag@Ag<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub>Ā·2H<sub>2</sub>O nanocomposite is an efficient visible-light-driven plasmonic photocatalyst
for degradation of Rhodamine B dye in aqueous solution