Metal-insulator transition in VnO2n−1

Research on phase relationships and structure studies by electron diffraction confirm V_nO_2n?1 (n = 3–9) phases between V₂O₃ and VO₂. Metal-insulator phase transitions have been found in all phases but V₃O₅ and V₇O₁₃. Electrical, magnetic and thermodynamic properties associated with the transitions are reported for sintered samples or for single crystals prepared by a vapor-transport method. The results are collated and reviewed in summarized form.     

Preparation and studies of a new ammonium vanadium bronze, (NH4)xV2O5

A new bronze-type phase of composition (NH₄)_0.40±0.02V₂O₅ is obtained around 230°C during the thermal decomposition of NH₄VO₃ in hydrogen atmosphere. The bronze intermediate is characterized by X-ray diffraction, electrical conductivity, magnetic susceptibility, and ESR studies. It is found to be isostructural with other known β-type vanadium bronzes of general formula M_xV₂O₅, where M is usually a monovalent metal. Electrical conductivity and magnetic studies indicate the localized character of conduction electrons at V⁺⁴ sites. At high temperatures (>400°C), the bronze undergoes decomposition and subsequent reduction to V₂O₃ in hydrogen atmosphere.     

Thermochemische Untersuchungen im System V/Nb/O. II Zum chemischen Transportverhalten im Bereich V2O5/Nb2O5/VO2/NbO2

Thermochemical Investigations in the System V/Nb/O. II. Chemical Transport in the Region V₂O₅/Nb₂O₅/VO₂/NbO₂ Transport experiments were used to support the phase relationships of the V₂O₅/Nb₂O₅/VO₂/NbO₂ system, which were established by annealing experiments of powder mixtures. The phase relations were studied in the NbO₂-rich region of the system by means of X-ray and ESMA methods. The NbO₂-rich section is characterized by the following two phase and three phase regions: Two phase region: V₃Nb₉O₂₉/rutile mixed crystal V_1?xNb_xO₂ Two phase region: BI-mixed crystal/V_xNb_1?xO₂ Three phase region: V₃Nb₉O₂₉/solubility limit LG1 (V_1?xNb_xO₂)/BI-mixed crystal Three phase region: solubility limit LG1 (V_1?xNb_xO₂)/BI-mixed crystal/solubility limit LG2 (V_xNb_1?xO₂). The composition of the solubility limits LG1 and LG2 was ascertained by means of ESMA-investigation: LG1: 57.5 ± 5 mol% NbO₂/43.5 ± 5 mol% VO₂ LG2: 22.5 ± 5 mol% NbO₂/78.5 ± 5 mol% VO_2?     

Uniform Decoration of Vanadium Oxide Nanocrystals on Reduced Graphene‐Oxide Balls by an Aerosol Process for Lithium‐Ion Battery Cathode Material

VO₂‐decorated reduced graphene balls were prepared by a one‐pot spray‐pyrolysis process from a colloidal spray solution of well‐dispersed graphene oxide and ammonium vanadate. The graphene–VO₂ composite powders prepared directly by spray pyrolysis had poor electrochemical properties. Therefore, the graphene–VO₂ composite powders were transformed into a reduced graphene ball (RGB)–V₂O₅ (RGB) composite by post‐treatment at 300 °C in an air atmosphere. The TEM and dot‐mapping images showed a uniform distribution of V and C components, originating from V₂O₅ and graphene, consisting the composite. The graphene content of the RGB–V₂O₅ composite, measured by thermogravimetric analysis, was approximately 5 wt %. The initial discharge and charge capacities of RGB–V₂O₅ composite were 282 and 280 mA h g^?1, respectively, and the corresponding Coulombic efficiency was approximately 100 %. On the other hand, the initial discharge and charge capacities of macroporous V₂O₅ powders were 205 and 221 mA h g^?1, respectively, and the corresponding Coulombic efficiency was approximately 93 %. The RGB–V₂O₅ composite showed a better rate performance than the macroporous V₂O₅ powders.     

Phase diagram and infrared-spectral investigation of the 2TeO2 · V2O5-Na2O · V2O5 · 2TeO2 system

The phase diagram of the 2TeO₂ · V₂O₅-Na₂O · V₂O₅ · 2TeO₂ system is studied by X-ray diffraction, ir spectroscopy, and DTA. A new compound with a composition of Na₂O · 3V₂O₅ · 6TeO₂ is established. The ir spectra of the alkaline trivanadates are interpreted. They are considered as structural analogs of the new phase. As a result of this comparison, the postulate is made that the main structural units in the Na₂O · 3V₂O₅ · 6TeO₂ compound are V₂O₈ groups, while tellurium is present both in the TeO₃ and TeO₄ groups. Contrary to the crystal phases, in glasses the transition from VO₅ toward VO₄ does not proceed through the formation of new structural units of vanadium; but rather a gradual transition of the structure is observed with a change in the composition from 2TeO₂ · V₂O₅ to Na₂O · V₂O₅ · 2TeO₂.     

Ein neues Syntheseverfahren für Vanadiumbronzen. Die Kristallstruktur von β?Ag0,33V2O5. Verfeinerung der Kristallstruktur von ϵ?Cu0,76V2O5

A Novel Means of Synthesis for Vanadium Bronzes. Crystal Structure of β? Ag_0.33V₂O₅. Refinement of the Crystal Structure of ?? Cu_0.76V₂O₅ Ag_0.33V₂O₅ and Cu_0.76V₂O₅ were obtained by heating equimolar mixtures of AgI + V₂O₅ (700°C) and CuI + V₂O₅ (525°C), respectively, in sealed quartz glass ampoules. In each case, one of the well-formed crystals served for an X-ray structure analysis. Ag_0.33V₂O₅ has the structure known of the β phase of the vanadium bronzes, i. e. layers of edge-sharing, distorted VO₆ octahedra are liked by certain common octahedron vertices, the Ag atoms randomly occupy two positions with occupation probabilities of 0.5. Cu_0.76V₂O₅ has the previously determined structure of the ? phase, however, its space group is not Cm but C2/m.     

Flexible V7O16 Layers as the Common Structural Element of Vanadium Oxide Nanotubes and a New Crystalline Vanadate

The walls of vanadium oxide nanotubes (VO_x‐NTs) are built up by vanadate layers between which the structure‐directing template, either a primary amine or a diamine with long alkyl chain, is located. The feasibility of various exchange reactions under preservation of the tubular morphology indicates a high structural flexibility of the VO_x‐NTs. The structure of the vanadate layers appears to be the same in all tubular vanadates, as revealed by the similarity of the diffraction patterns. Plate‐like crystals of a new crystalline phase, structurally closely related to the nanotubes, have now been prepared with ethylene diamine, applying a route that is analogous to the VO_x‐NT synthesis. The single crystal X‐ray structure determination showed that this new phase has the composition (en)V₇O₁₆ and crystallizes with triclinic symmetry. The structure is composed of V₇O₁₆ layers between which ethylene diamine mo le cules are embedded. The V₇O₁₆ layers comprise two sheets of square VO₅ pyramids and VO₄ tetrahedra that connect these sheets. The available experimental data establish that this V₇O₁₆ layer also is the basic element of the VO_x‐NT wall structure. The simulated X‐ray powder diffraction pattern calculated with a corresponding structural mode for VO_x‐NTs agrees well with the observed one.     

Preparation and properties of the oxyfluoride systems V2O5−xFx and VO2−xFx

Partial substitution of fluorine for oxygen in VO₂ and V₂O₅ was achieved by reacting V and V₂O₅ under 1.33 kb pressure in the presence of concentrated or dilute solutions of HF. Two new phases having the composition V₂O_5−xF_x (0 < x < 0.025) and VO_2−xF_x (0 < x < 0.2) were prepared. X-Ray diffraction studies have been carried out on both phases and show the structure of V₂O_5−xF_x to be orthorhombic and isostructural to V₂O₅, while VO_2−xF_x has a tetragonal structure of the rutile type (for x ? 0.03). Single-crystal-resistivity data show V₂O_5−xF_x to be a semiconductor, whereas VO_2−xF_x undergoes a metallic to semiconductor transition at a temperature solely dependent upon the value of x.     

Rapid hydrothermal synthesis of Li<Subscript>3</Subscript>VO<Subscript>4</Subscript> with different favored facets

Here, we demonstrate a new, rapid, and flexible hydrothermal method using the V₂O₅ and LiOH as the precursors to synthesize Li₃VO₄. The ratios of precursor of V₂O₅ and LiOH can be changed in a wide range to control different preferred facets and morphologies, and the reason has been discussed from the structure of Li₃VO₄. The electrical performance of the Li₃VO₄ has also been systematically investigated. The thus-synthesized Li₃VO₄ exhibits significantly improved rate capability and cycling life compared with commercial graphite, synthesized Li₄Ti₅O₁₂, and previously reported results on Li₃VO₄.     

Substrate temperature effects on the structural,compositional, and electrical properties of VO2 thin films deposited by pulsed laser deposition

The vanadium dioxide (VO₂) thin films were deposited on silicon (100) substrate using the pulsed laser deposition technique. The thin films were deposited at different substrate temperatures (500°C, 600°C, 700°C, and 800°C) while keeping all the other parameters constant. X‐ray diffraction confirmed the crystalline VO₂ (B) and VO₂ (M) phase formation at different substrate temperatures. X‐ray photoelectron spectroscopy analysis showed the presence of V⁴⁺ and V⁵⁺ charge states in all the deposited thin films which confirms that the deposited films mainly consist of VO₂ and V₂O₅. An increase in the VO₂/V₂O₅ ratio has been observed in the films deposited at higher substrate temperatures (700°C and 800°C). Scanning electron microscope micrographs revealed different surface morphologies of the thin films deposited at different substrate temperatures. The electrical properties showed the sharp semiconductor to metal transition behavior with approximately 2 orders of magnitude for the VO₂ thin film deposited at 800°C. The transition temperature for heating and cooling cycles as low as 46.2°C and 42°C, respectively, has been observed which is related to the smaller difference in the interplanar spacing between the as‐deposited thin film and the standard rutile VO₂ as well as to the lattice strain of approximately −1.2%.     

Phase equilibria in the V2O5-NaVO3-Ca(VO3)2-Mn2V2O7 system and interactions of phases with H2SO4 and NaOH solutions

Phase composition of the V₂O₅-NaVO₃-Ca(VO₃)₂-Mn₂V₂O₇ system was studied, and a subsolidus phase diagram constructed. The tetrahedration of the diagram is determined by the fact that the end-member of Ca_1–x Mn _x (VO₃)₂ solid solution is in equilibrium with all compounds of the system (V₂O₅, NaVO₃, Ca(VO₃)₂), vanadium β-bronzes Na _x V₂O₅ (0.22 ≤ x ≤ 0.40) and κ-bronzes (0.25 ≤ x ≤ 0.45, 0 ≤ y ≤ 0.16), Mn₂V₂O₇, and Na₂Mn₃(V₂O₇)₂ and with the end-members of reciprocal solid solutions based on calcium and sodium metavanadates. At 20°C, the degree of vanadium dissolution α for Na₂Ca(VO₃)₄ is 100% for 0.5 ≤ pH ≤ 10; for the other phases of the system, vanadium dissolution ranges from 100 to 10% for pH below 3.5; in the alkaline pH range, ≤ 10%. Sodium for calcium substitution in Ca(VO₃)₂ increases α in aqueous NaOH to 20%. For Na₂Mn₃(V₂O₇)₂, α decreases from 92 to 80% as pH changes from 0.5 to 2.5; at pH above 4, α = 30%.     

Reactivity of some vanadium oxides: An EPR and XRD study

V₂O₅, VO₂ and V₂O₃ fresh samples and at different times after purchase or preparation (aged samples) were investigated by chemical analysis, redox treatments, XRD and EPR. The ageing process through a reaction with water and oxygen slowly oxidize crystalline VO₂ and V₂O₃, leading to a quasi-amorphous phase with bariandite structure (V₁₀O₂₄·12H₂O). The role of water is the progressive demolition of the compact structures and formation of hydrated phase. Kinetic study of VO₂ oxidation by O₂ and O₂+H₂O mixture indicates that increasing the temperature up to 723 K the effect of water becomes less important. The reaction leads to partially oxidized products with decreasing water content: bariandite at room temperature, V₃O₇·H₂O at 383 K and V₃O₇ at 723 K. Kinetic investigation of V₂O₅ reduction by CO at 633-723 K showed that the reduction process proceeds trough the formation of V⁴⁺ and of electrons delocalized in the conduction band.     

Influence of the grain morphology of V2O5 on its reduction-reoxidation behaviour

The influence of the grain morphology of V₂O₅ on its reduction-reoxidation behaviour has been investigated by means of thermoanalytical methods. X-ray analysis and electron microscopy. Well-developed V₂O₅ platelets exposing predominantly the (010) face exhibited a significantly different reduction profile than poorly defined agglomerates of microcrystalline V₂O₅. Intermediate phases detected during reduction were V₆O₁₃ and VO₂ (rutile). The corresponding reoxidation profiles were found to be only weakly dependent on the grain morphology of V₂O₃. Electron microscopy showed that the original grain morphology of the V₂O₅ samples was not influenced markedly by the reduction-reoxidation cycle.     

Die Vanadin-Koordination in den Phasen 4 PbO · V2O5 und 8 PbO · V2O5

Coordination of Vanadium in the Phases 4 PbO · V₂O₅ and 8 PbO · V₂O₅ It is demonstrated, using infrared spectroscopy, that the coordination of vanadium in the two binary phases 4 PbO · V₂O₅ and 8 PbO · V₂O₅ is tetrahedral. The spectra in the V? O stretching region closely resembles that of the lead(II) orthovanadate, Pb₃(VO₄)₂.     

Exafs and electron-microscopy studies on V/SiO2 catalysts

Extended x-ray-absorption fine structure and scanning electron microscopy have been applied to the structure of the vanadium oxide layers on impregnated and grafted vanadium aerosils. When aerosil is impregnated with NH₄VO₃ solution, V₂O₅ crystals are formed; when vanadium is grafted by reacting the oxychloride with carrier OH groups, there are no visible crystals. On the other hand, the EXAFS spectra for the grafted specimens show all the oscillations found for crystalline V₂O₅. It is concluded that the vanadium oxide layers in these grafted materials have a long-range order similar to that in V₂O₅ and contain microcrystals having sizes up to 5 nm.Translated from Teoreticheskaya i Éksperimental'naya Khimiya, Vol. 23, No. 5, pp. 652–655, September–October, 1987.     

Effect of Fullerene Volume Fraction on Two‐Dimensional Crystal‐Constructed Supramolecular Liquid Crystals

The volume fraction plays an important role in phase segregated soft matters. We demonstrate here that at high fullerene volume fraction in soft chain‐tethered‐fullerene dyads, different two‐dimensional (2D) crystal‐constructed smectic‐like lamella liquid crystalline (LC) phases can be formed with triple‐layer (S_T phase) or quadruple‐layer (S_Q phase) stacking of fullerenes in 2D crystals. The combination of 2D crystal and LC properties in one system affords these fullerene dyads controlled electron mobility in the range of 10^?5–10^?3 cm² V^?1 s^?1 at room temperature (S_T phase), by regulating the insulated soft layer thickness between 2D crystals via the manipulation of fullerene volume fraction.     

Cadmium vanadates of potassium,rubidium, and cesium

The solid-phase reactions between the components have been used to study the equilibrium phase composition of the systems M₂O(M₂CO₃)-CdO-V₂O₅ (M = K, Rb, or Cs) in the range of the subsolidus temperatures. New potassium cadmium vanadates KCd₃V₃O₁₁, K₂Cd₅(VO₄)₄, and K₂Cd₄V₄O₁₅ have been synthesized. A monoclinic solid solution has been identified on the basis of the KCd₄(VO₄)₃ structure. Double orthovanadate RbCdVO₄ has been prepared for the first time. Equilibrium phase diagrams have been constructed using both previously known compounds, and those synthesized by us. The effect of the size factor (the M⁺ ion radius) on the phase formation and phase equilibria in the systems in question has been traced.     

Crystal growth,structure, and properties of manganese orthovanadate Mn3(VO4)2

Manganese orthovanadate Mn₃(VO₄)₂ single crystals were grown for the first time from a flux of MnO/V₂O₅/MoO₃. The flux and oxygen partial pressure used are the key factors for the crystal growth and prevention of the oxidation of Mn²⁺ and the reduction of V⁵⁺ during the crystallization process. The reduction and oxidation chemistry of Mn₃(VO₄)₂ was studied. Mn₃(VO₄)₂ is isostructural with magnesium orthovanadate Mg₃(VO₄)₂, orthorhombic, space group Cmca, a=6.247(1) Å, b=11.728(2) Å, c=8.491(2) Å and Z=4, as determined by single crystal X-ray diffraction. Because it is a Mn²⁺ deficient spinel structure there are two-dimensional sheets of Mn²⁺O₆ octahedra within the structure which show unusual ferrimagnetic properties.     

Phase relations in the system V/Nb/O. V. Investigation of mixed crystals V1-xNbxO2

Mixed crystals V_1-xNb_xO₂ exist over the whole area of the quasibinary line VO₂-NbO₂. The existence of Nb_{5+ beside V3+ and V4+ on the V-rich side and V3+ beside Nb5+ and Nb4+ on the Nb-rich side of the mixed crystals is demonstrated by XANES-measurements. The compound VNbO}4_(V0.5_Nb0.5_O2_{) is described as a double oxide with vanadium only as V3+ and niobium only as Nb5+. At this point the electric resistivity of the solid solution shows a maximum.}     

Microwave‐Assisted Solvothermal Synthesis of VO2 Hollow Spheres and Their Conversion into V2O5 Hollow Spheres with Improved Lithium Storage Capability

Monodispersed hierarchically structured V₂O₅ hollow spheres were successfully obtained from orthorhombic VO₂ hollow spheres, which are in turn synthesized by a simple template‐free microwave‐assisted solvothermal method. The structural evolution of VO₂ hollow spheres has been studied and explained by a chemically induced self‐transformation process. The reaction time and water content in the reaction solution have a great influence on the morphology and phase structure of the resulting products in the solvothermal reaction. The diameter of the VO₂ hollow spheres can be regulated simply by changing vanadium ion content in the reaction solution. The VO₂ hollow spheres can be transformed into V₂O₅ hollow spheres with nearly no morphological change by annealing in air. The nanorods composed of V₂O₅ hollow spheres have an average length of about 70 nm and width of about 19 nm. When used as a cathode material for lithium‐ion batteries, the V₂O₅ hollow spheres display a diameter‐dependent electrochemical performance, and the 440 nm hollow spheres show the highest specific discharge capacity of 377.5 mAhg^?1 at a current density of 50 mAg^?1, and are better than the corresponding solid spheres and nanorod assemblies.