Growth and self-organization of nanostructures on interlayer surfaces of A<Stack><Subscript>2</Subscript><Superscript>V</Superscript></Stack>B<Stack><Subscript>3</Subscript><Superscript>VI</Superscript></Stack> layered crystals

This paper examines the formation of arrays of interlayer nanostructures in layered crystals grown by directional solidification and the Bridgman method. Sb₂Te₃ and Bi₂Te₃ layers are shown to contain steplayered structures with nanostructured islands on them. Atomic force microscope images of interlayer nanostructures in such crystals are analyzed in terms of the physics of fractals and self-organization processes.     

Estimative calculations of the dispersion limit for A<Superscript>II</Superscript>B<Superscript>VI</Superscript> and A<Superscript>III</Superscript>B<Superscript>V</Superscript> crystals

Estimative calculations are carried out for the critical sizes of crystalline grains of some semiconductor compounds A^IIB^VI and A^IIIB^V, a further decrease in which leads to a crystalline-amorphous transition. The correlation between the critical grain size and the band gap of a semiconductor is found. Values of critical grain sizes are in agreement with sizes of the disordered (amorphous) phase appearing at the initial stage of growth of epitaxial films (Si and CdHgTe) on different substrates.     

Crystal structure of the perovskites Ba<Subscript>2</Subscript>A<Superscript>II</Superscript>UO<Subscript>6</Subscript> (A<Superscript>II</Superscript> = Zn,Cd, Pb)

The compounds Ba₂ZnUO₆, Ba₂CdUO₆, and Ba₂PbUO₆ were prepared by high-temperature solidphase reactions. Their structures (space group Fm \(\bar 3\) m) were refined by the Rietveld method. In the morphotropic series Ba₂A^IIUO₆, correlations were found between the A^II-O, U-O, and Ba-O bond lengths and the crystal-chemical radius of A^II.     

Low-temperature heat capacity and thermodynamic functions of compounds with the composition Ba(A<Stack><Subscript>2/3</Subscript><Superscript>III</Superscript></Stack>U<Subscript>1/3</Subscript>)O<Subscript>3</Subscript> (A<Superscript>III</Superscript> = Sc,Y)

The heat capacity of crystalline Ba(Sc_2/3U_1/3)O₃ and Ba(Y_2/3U_1/3)O₃ in the range 80–350 K was studied by adiabatic vacuum calorimetry, and the thermodynamic characteristics of these compounds were evaluated. Their standard entropies of formation at 298.15 K were calculated.     

Synthesis and properties of laser-active liquids POCl<Subscript>3</Subscript>-SbCl<Subscript>5</Subscript>-<Superscript>235</Superscript>UO<Stack><Subscript>2</Subscript><Superscript>2+</Superscript></Stack>-Nd<Superscript>3+</Superscript>

The effect of the synthesis conditions on the properties of inorganic laser-active liquids POCl₃-SbCl₅-²³⁵UO ₂ ²⁺ -Nd³⁺ is considered. The kinetic dependences of the U(IV) content and decay time of the Nd³⁺ luminescence in POCl₃-SbCl₅-²³⁵UO ₂ ²⁺ -Nd³⁺ solutions for various synthesis procedures at 380 K have been obtained. In POCl₃-SbCl₅-²³⁵UO ₂ ²⁺ -Nd³⁺ solutions, nonradiative energy transfer Nd³⁺ → U⁴⁺ is observed, and quenching of the Nd³⁺ luminescence is described by the Stern-Volmer law: k _q = (6.4 ± 0.6) × 10⁵ l mol^?1 s^?1. Laser liquids POCl₃-SbCl₅-²³⁵UO ₂ ²⁺ -Nd³⁺ with neodymium concentration of up to 0.7 M, uranyl concentration of up to 0.1 M, and decay time of the Nd³⁺ luminescence of up to 220 μs have been prepared for the first time.     

Interaction of aqueous UO<Stack><Subscript>2</Subscript><Superscript>2+</Superscript></Stack> solutions with sorbents based on modified silica gel containing Cu,Ni, and Zn

Interaction of aqueous UO ₂ ²⁺ solutions with modified sorbents based on coarsely porous silica gel MSKG, containing Cu, Ni, and Zn ions, was studied. Uranyl ions are sorbed on all the sorbents. The decontamination factors of 10^?2 M aqueous UO ₂ ²⁺ solutions on straight MSKG and on MSKG modified with Cu, Ni, and Zn are of the same order of magnitude and do not exceed 100. In the case of 1.1 × 10^?1 M UO ₂ ²⁺ solutions, the decontamination factors on straight MSKG and on MSKG modified with Cu, Ni, and Zn are also of the same order of magnitude but do not exceed 10. Interaction of the modified Ni-containing sorbent with a UO ₂ ²⁺ solution results in formation of a swamp-green precipitate of the composition NiU(OH)₆·4N₂H₅OH, i.e., UO ₂ ²⁺ is reduced to U⁴⁺.     

Emission Activity under Impact Destruction of A<Subscript>2</Subscript>B<Subscript>6</Subscript> Ceramics

In this paper, we present results of a study of the generation of electromagnetic emission during impact loading of ZnS and ZnSe ceramics prepared by various techniques. The choice of the type of mechanical action is associated with the typical applications of these ceramics. Separate contributions to emission activity from the dislocations movement and the microcracks development depending on the crystallite size in the ceramics are shown. The electromagnetic emission is compared with parallel time series of pulses of mechanoluminescence and acoustic emission. In all three cases, emission activity was recorded with a time resolution of 10 ns.     

The nature of optical pumping losses in low-threshold LiF(F<Subscript>2</Subscript>, F<Stack><Subscript>3</Subscript><Superscript>+</Superscript></Stack>) crystal microlasers

The character of optical losses in Li(F₂, F ₃ ⁺ ) crystals were studied for the first time by methods of optical absorption spectroscopy and X-ray diffraction. It is suggested that centers absorbing at 420 nm represent quasi-metallic defects of the F₂F_L type.     

X-ray diffraction study of the Tm<Subscript>2</Subscript>M<Stack><Subscript>3</Subscript><Superscript>I</Superscript></Stack>Fe<Subscript>5</Subscript>O<Subscript>12</Subscript> (M<Superscript>I</Superscript> = Li,Na, K) ferrites

The Tm₂M₃^IFe₅O₁₂ (M_I = Li, Na, K) compounds have been prepared for the first time by solid-state reactions between thulium(III) oxide, iron(III) oxide, and alkali metal carbonates, and their symmetry class and unit-cell parameters have been determined by X-ray diffraction.     

A physicochemical study of compounds formed in the systems A<Superscript>III</Superscript>(HSiUO<Subscript>6</Subscript>)<Subscript>3</Subscript>-H<Subscript>2</Subscript>O (A<Superscript>III</Superscript> = Y,La-Lu)

Compounds in the systems A^III(HSiUO₆)₃-H₂O (A^III = Y, La-Lu) were prepared by stepwise dehydration of uranosilicate A^III(HSiUO₆)₃ decahydrates (A^III = Y, La-Lu), and their structural transformations were studied by high-temperature X-ray diffraction technique and IR spectroscopy.     

Refractive index of Al<Subscript>3</Subscript>C<Subscript>2</Subscript>B<Subscript>48</Subscript> aluminum borocarbide crystals

Aluminum borocarbide single crystals have been grown from an Al-based solution melt. The crystal lattice parameters have been determined, the dispersion of the refractive index in a 0.55–1.3 μm wavelength interval has been studied, and the temperature coefficient of the refractive index in a 300–600 K range has been measured. The crystals are characterized by a high refractive index in the visible spectral range in combination with at a high hardness, which makes them of interest for jewelry, as well as for both traditional and X-ray optics.     

Manifestation of metastable cubic modifications in finely dispersed A<Subscript>2</Subscript>B<Subscript>6</Subscript> compounds

The presence of metastable cubic modifications has been revealed by X-ray diffraction in polycrystalline CdS and CdSe powders with grain sizes on the order of several dozen nanometers. The optical reflection and photoluminescence spectra of the cubic CdS phase have been measured in the temperature interval of 77–295 K. The main exciton transition energies and the temperature coefficients of the bandgap width variation have been determined.     

A physicochemical study of the perovskites M<Superscript>II</Superscript>(In<Subscript>2/3</Subscript>U<Subscript>1/3</Subscript>)O<Subscript>3</Subscript> (M<Superscript>II</Superscript> = Sr,Ba) at low temperatures

The heat capacity of crystalline Sr(In_2/3U_1/3)O₃ and Ba(In_2/3U_1/3)O₃ in the range 80–350 K was determined by adiabatic vacuum calorimetry, and the thermodynamic functions of these compounds in the range from T → 0 to 350 K were calculated. The standard entropies of formation of these compounds at 298.15 K were calculated. The absolute entropies and standard entropies of formation of perovskites M^II(A^III _2/3U_1/3)O₃ (M^II = Sr, A^III = Sc, In, Fe; M^II = Ba, A^III = Sc, In, Y, Nd-Lu) were estimated.     

Luminescence of Pb<Superscript>2+</Superscript> in MAl<Subscript>2</Subscript>B<Subscript>2</Subscript>O<Subscript>7</Subscript> (M = Ca,Sr)

Pb²⁺ doped SrAl₂B₂O₇ was prepared by solution combustion synthesis. The synthesized material was determined by powder XRD. The photoluminescence properties of the synthesized phosphor were investigated at room temperature using a spectrofluorometer. The emission peak of Pb²⁺ doped SrAl₂B₂O₇ was observed at 420 nm upon excitation at 277 nm. The Stokes shift of SrAl₂B₂O₇:Pb²⁺ was calculated to be 12 292 cm⁻¹. The luminescence behavior of Pb²⁺ in both SrAl₂B₂O₇ and CaAl₂B₂O₇ was discussed. The text was submitted by the authors in English.     

Enhancement in electrical conductivity of Li<Subscript>2</Subscript>O: B<Subscript>2</Subscript>O<Subscript>3</Subscript>: V<Subscript>2</Subscript>O<Subscript>5</Subscript> glasses

The study of electrical conductivity of 30Li₂O: (70 − x) B₂O₃: xV₂O₅ glass samples has been carried out. The results have been explained by dividing the temperature range into two regions. In region I, conductivity shows Arrhenius behaviour for all the samples. The conductivity increases with addition of V₂O₅. The results have been explained in the light of Anderson and Stuart Model. In region II, an anomalous enhancement in the conductivity is observed for all the samples up to certain temperature beyond which the conductivity decreases. The enhancement in the conductivity in the annealed glass sample has been attributed to nanocrystallization.     

Heat Capacity and thermodynamic functions of DyMe<Superscript>II</Superscript>Cr<Subscript>2</Subscript>O<Subscript>5.5</Subscript>(Me<Superscript>II</Superscript>-Mg,Ca) in the range from 298.15 to 673 K

The calorimetric method is used to investigate the heat capacity of DyMe^IICr₂O_5.5(Me^II-Mg, Ca) chromites in the range from 298.15 to 673 K. The C _p ⁰ ～ f(T) curves exhibit λ-like effects at 348 and 548 K for DyMgCr₂O_5.5 and at 473 K for DyCaCr₂O_5.5, which apparently relate to second-order phase transitions. The temperature dependences are calculated for thermodynamic functions C _p ⁰ (T), H ⁰(T)-H ⁰(298.15), S ⁰(T), and Φ**(T).     

Intense blue and violet luminescence in the (B<Subscript>2</Subscript>O<Subscript>3</Subscript>-Al<Subscript>2</Subscript>O<Subscript>3</Subscript>-SiO<Subscript>2</Subscript>):Eu<Superscript>2+</Superscript> system

Glassy-crystalline samples of compositions (B₂O₃-Al₂O₃-SiO₂):Eu²⁺ (3 at %) and (B₂O₃-2SiO₂):Eu²⁺ (3 at %) were obtained by sintering the initial powdered mixtures at 1300°C in air. Being excited by laser radiation at a wavelength of 325 nm, the former samples exhibit intense blue photoluminescence with a maximum at 434–448 nm, while the latter samples emit in the violet spectral interval with a maximum at 409 nm. An increase in the content of B₂O₃ leads to a shift of the emission maximum toward a shorter wavelength, while additional annealing at 1300°C C in vacuum shifts the spectrum toward longer wavelengths.     

Luminescence studies on Eu<Superscript>2+</Superscript> and Tb<Superscript>3+</Superscript> doped Ca<Subscript>2</Subscript>MgSi<Subscript>2</Subscript>O<Subscript>7</Subscript> phosphors

Eu²⁺ and Tb³⁺ doped Ca₂MgSi₂O₇ phosphors were synthesized by conventional solid-state reaction. The phase formation was confirmed by X-ray powder diffraction technique and refined lattice parameters were calculated by rietveld refinement process using Celref v3. The photoluminescence (PL) excitation and emission spectra were investigated. The phosphors exhibited broaden green emitting luminescence peaking at 520 nm when excited at 374 nm source. Morphological studies were carried out using Scanning electron microscopy (SEM) images of the sample with optimum PL emission. The dependence of photoluminescence intensity on co-dopant concentration and the kinetic parameters were also reported. Time resolved fluorescence spectroscopy (TRFS) is used to investigate the decay in luminescence signals with respect to time. The sample proved to be a good long lasting material, which makes it useful in emergency signs, textile printing, textile exit sign boards and electronic instrument dial pads etc.     

The calorimetry and thermodynamic functions of Nd Mg<Stack><Subscript>3</Subscript><Superscript>I</Superscript></Stack>Mn<Subscript>4</Subscript>O<Subscript>12</Subscript> (Me<Superscript>I</Superscript>-Li,Na, K) manganites in the range from 298.15 to 673 K

The ceramic technology is employed for synthesizing manganites of composition Nd Mg ₃ ^I Mg₃Mn₄O₁₂(Me^I-Li, Na, K). The X-ray technique is used to find that the compounds crystallize in tetragonal syngony. The parameters of their crystal lattices are determined. Their heat capacities are experimentally determined in the range from 298.15 to 673 K, which enables one to reveal second-order phase transitions. In view of these transitions, equations describing the C _p ^° ～ f(T) dependence are derived, and the thermodynamic functions C _p ^° (T), H°(T)-H°(298.15), S°(T), and Φ ^xx (T) are calculated.     

Complexation of Tc(CO)<Stack><Subscript>3</Subscript><Superscript>+</Superscript></Stack>·aq with Anions of Monobasic Carboxylic Acids in Aqueous Solutions: A <Superscript>99</Superscript>Tc NMR Study

Carboxylate anions in aqueous solutions coordinate with the Tc(CO) ₃ ⁺ ion mainly in the monodentate fashion to form weak 1 : 1, 1 : 2, and 1 : 3 complexes. The stability of the complexes decreases with increasing size of the alkyl radical. In the series of halo-substituted acetates, all the stability constants decrease with a decrease in the basicity of the anion.__________Translated from Radiokhimiya, Vol. 47, No. 1, 2005, pp. 49–52.Original Russian Text Copyright © 2005 by Suglobov, Miroslavov, Sidorenko, Gorshkov, Lumpov.