4 research outputs found

    Ex Situ Xā€‘ray Diffraction, Xā€‘ray Absorption Near Edge Structure, Electron Spin Resonance, and Transmission Electron Microscopy Study of the Hydrothermal Crystallization of Vanadium Oxide Nanotubes: An Insight into the Mechanism of Formation

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    The nucleation and growth of vanadium oxide nanotubes (VO<sub><i>x</i></sub>-NT) have been followed by a combination of numerous ex situ techniques along the hydrothermal process. Intermediate solid phases extracted at different reaction times have been characterized by powder X-ray diffraction, scanning and transmission electron microscopy, electron spin resonance, and Vā€“K edge X-ray absorption near-edge structure spectroscopy. The supernatant vanadate solutions extracted during the hydrothermal treatment have been studied by liquid <sup>51</sup>V NMR and flame spectroscopy. For short durations of the hydrothermal synthesis, the initial V<sub>2</sub>O<sub>5</sub>-surfactant intercalate is progressively transformed into VO<sub><i>x</i></sub>-NT whose crystallization starts to be detected after a hydrothermal treatment of 24 h. Upon heating from 24 h to 7 days, VO<sub><i>x</i></sub>-NT are obtained in larger amount and with an improved crystallinity. The detection of soluble amines and cyclic metavanadate [V<sub>4</sub>O<sub>12</sub>]<sup>4ā€“</sup> in the supernatant solution along the hydrothermal process suggests that VO<sub><i>x</i></sub>-NT result from a dissolutionā€“precipitation mechanism. Metavanadate species [V<sub>4</sub>O<sub>12</sub>]<sup>4ā€“</sup> could behave as molecular precursors in the polymerization reactions leading to VO<sub><i>x</i></sub>-NT

    Ex Situ Xā€‘ray Diffraction, Xā€‘ray Absorption Near Edge Structure, Electron Spin Resonance, and Transmission Electron Microscopy Study of the Hydrothermal Crystallization of Vanadium Oxide Nanotubes: An Insight into the Mechanism of Formation

    No full text
    The nucleation and growth of vanadium oxide nanotubes (VO<sub><i>x</i></sub>-NT) have been followed by a combination of numerous ex situ techniques along the hydrothermal process. Intermediate solid phases extracted at different reaction times have been characterized by powder X-ray diffraction, scanning and transmission electron microscopy, electron spin resonance, and Vā€“K edge X-ray absorption near-edge structure spectroscopy. The supernatant vanadate solutions extracted during the hydrothermal treatment have been studied by liquid <sup>51</sup>V NMR and flame spectroscopy. For short durations of the hydrothermal synthesis, the initial V<sub>2</sub>O<sub>5</sub>-surfactant intercalate is progressively transformed into VO<sub><i>x</i></sub>-NT whose crystallization starts to be detected after a hydrothermal treatment of 24 h. Upon heating from 24 h to 7 days, VO<sub><i>x</i></sub>-NT are obtained in larger amount and with an improved crystallinity. The detection of soluble amines and cyclic metavanadate [V<sub>4</sub>O<sub>12</sub>]<sup>4ā€“</sup> in the supernatant solution along the hydrothermal process suggests that VO<sub><i>x</i></sub>-NT result from a dissolutionā€“precipitation mechanism. Metavanadate species [V<sub>4</sub>O<sub>12</sub>]<sup>4ā€“</sup> could behave as molecular precursors in the polymerization reactions leading to VO<sub><i>x</i></sub>-NT

    A Comprehensive Study of the Mechanism of Formation of Polyol-Made Hausmannite Nanoparticles: From Molecular Species to Solid Precipitation

    No full text
    This study aims at achieving a better understanding of the mechanisms of formation of Mn<sub>3</sub>O<sub>4</sub> nanoparticles prepared by the polyol process. The role of each reactant is studied, and a possible scheme of reaction is proposed, involving the activation of dioxygen by MnĀ­(II) species. The growth of the particles (evolution of the size and concentration of particles) has been followed in solution by SAXS, and the results have been compared to those obtained by other techniques on dried powders. The results indicate a decrease of the number of particles in solution with time together with their enlargement. A stabilization of the size and number of particles is reached after a few hours. The shape of the particles then evolves into a truncated ditetragonal-dipyramidal polyhedron

    Storage of Visible Light for Long-Lasting Phosphorescence in Chromium-Doped Zinc Gallate

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    ZnGa<sub>2</sub>O<sub>4</sub>:Cr<sup>3+</sup> presents near-infrared long-lasting phosphorescence (LLP) suitable for in vivo bioimaging. It is a bright LLP material showing a main thermally stimulated luminescence (TSL) peak around 318 K. The TSL peak can be excited virtually by all visible wavelengths from 1.8 eV (680 nm) via dā€“d excitation of Cr<sup>3+</sup> to above ZnGa<sub>2</sub>O<sub>4</sub> band gap (4.5 eVā€“275 nm). The mechanism of LLP induced by visible light excitation is entirely localized around Cr<sub>N2</sub> ion that is a Cr<sup>3+</sup> ion with an antisite defect as first cationic neighbor. The charging process involves trapping of an electronā€“hole pair at antisite defects of opposite charges, one of them being first cationic neighbor to Cr<sub>N2</sub>. We propose that the driving force for charge separation in the excited states of chromium is the local electric field created by the neighboring pair of antisite defects. The cluster of defects formed by Cr<sub>N2</sub> ion and the complementary antisite defects is therefore able to store visible light. This unique property enables repeated excitation of LLP through living tissues in ZnGa<sub>2</sub>O<sub>4</sub>:Cr<sup>3+</sup> biomarkers used for in vivo imaging. Upon excitation of ZnGa<sub>2</sub>O<sub>4</sub>:Cr<sup>3+</sup> above 3.1 eV, LLP efficiency is amplified by band-assistance because of the position of Cr<sup>3+4</sup>T<sub>1</sub> (<sup>4</sup>F) state inside ZnGa<sub>2</sub>O<sub>4</sub> conduction band. Additional TSL peaks emitted by all types of Cr<sup>3+</sup> including defect-free Cr<sub>R</sub> then appear at low temperature, showing that shallower trapping at defects located far away from Cr<sup>3+</sup> occurs through band excitation
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