11 research outputs found

    New Hybrid Layered Molybdates Based on <sup>2</sup>/<sub>āˆž</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 Organicā€“Inorganic Interfaces

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    Two new hybrid organicā€“inorganic molybdates based on layered <sup>2</sup>/<sub>āˆž</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> = 0ā€“1), 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>āˆž</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>āˆž</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>āˆž</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>āˆž</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>āˆž</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 organicā€“inorganic interface. In addition, a correlation between the topology of the <sup>2</sup>/<sub>āˆž</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>āˆž</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 organicā€“inorganic layered molybdate materials is clearly evidenced

    New Hybrid Layered Molybdates Based on <sup>2</sup>/<sub>āˆž</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 Organicā€“Inorganic Interfaces

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    Two new hybrid organicā€“inorganic molybdates based on layered <sup>2</sup>/<sub>āˆž</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> = 0ā€“1), 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>āˆž</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>āˆž</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>āˆž</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>āˆž</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>āˆž</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 organicā€“inorganic interface. In addition, a correlation between the topology of the <sup>2</sup>/<sub>āˆž</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>āˆž</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 organicā€“inorganic 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

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    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+ dā€“d transition as expected, while the blue band is the combination of the Ti3+ + Oā€“ ā†’ Ti4+ + O2ā€“ and VOā€¢+eā€“ ā†’ VOƗ 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

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    Seven hybrid organicā€“inorganic 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>NRRā€²Rā€³)Ā­(O)Ā­PO<sub>3</sub>)<sub>4</sub>]<sup>8ā€“</sup> (<i>m</i> = 3; R, Rā€², and Rā€³ = 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>NRRā€²Rā€³)Ā­(O)Ā­PO<sub>3</sub>)<sub>2</sub>]<sup>6ā€“</sup> (<i>m</i> = 3 or 4; R, Rā€², and Rā€³ = 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 organicā€“inorganic interface

    Incorporation of Jahnā€“Teller 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)

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    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 Jahnā€“Teller-inactive Mn<sup>2+</sup> (d<sup>5</sup>, <i>S</i> = 5/2) ions with Jahnā€“Teller-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 Jahnā€“Teller-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 NeĢel 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 Ī³ā€‘MnO<sub>2</sub>

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    In the presence of ā€œAg<sub>2</sub>Oā€ as a promoter, Ī³-MnO<sub>2</sub> traps dihydrogen in its (2 Ɨ 1) and (1 Ɨ 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>/ā€œAg<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 Ɨ 1) tunnels of Ī³-MnO<sub>2</sub>, which is then followed by that in the (1 Ɨ 1) tunnels. Our DFT analysis shows that this process is thermodynamically favorable

    Photochromic Properties of Polyoxotungstates with Grafted Spiropyran Molecules

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    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 organicā€“inorganic 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 SPā€“POT materials display highly effective solid-state photochromism from neutral SP molecules initially nonphotochromic in the crystalline state. The photoresponses of the SPā€“POT 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

    No full text
    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 organicā€“inorganic 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 SPā€“POT materials display highly effective solid-state photochromism from neutral SP molecules initially nonphotochromic in the crystalline state. The photoresponses of the SPā€“POT 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

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    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 organicā€“inorganic 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 UVā€“visā€“NIR 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
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