7446-07-3Relevant academic research and scientific papers
Structural and thermal studies on PuTe2O6
Krishnan,Mudher,Venugopal
, p. 114 - 118 (2000)
PuTe2O6 was synthesised by the solid state reaction route and characterized by X-ray diffraction and thermal methods. The structure of PuTe2O6 was derived by the Rietveld analysis of X-ray powder diffraction data in the monoclinic system with cell parameters a = 0.69937(1), b = 1.10014(2), c = 0.73404(2) nm, β = 107.98(2)°, Z = 4 in the space group P21/n. In the structure, each plutonium atom is coordinated to eight oxygen atoms. The structure is made up of zigzag strings of PuO8 distorted edge-sharing polyhedron parallel to the a axis. Tellurium atoms are coordinated to three oxygen atoms. PuTe2O6 melts at 1125 K incongruently and decomposes according to the reaction: PuTe2O6(s) → PuO2(s) + 2TeO2(g). The kinetics of decomposition under isothermal heating conditions in flowing air were studied to determine the rate constants, activation energy and reaction mechanism.
Synthesis, structure, and characterization of a new one-dimensional tellurite phosphate, Ba2TeO(PO4)2
Ok, Kang Min,Shiv Halasyamani
, p. 1345 - 1350 (2006)
A new one-dimensional tellurite phosphate, Ba2TeO(PO4)2 has been synthesized by standard solid-state reaction techniques using BaCO3, TeO2, and (NH4)H2PO4 as reagents. The structure of Ba2TeO(PO4)2 was determined by single-crystal X-ray diffraction. Ba2TeO(PO4)2 crystallizes in the triclinic space group P-1 (No. 2), with a = 6.9461 ( 16 ) A, b = 7.3970 ( 17 ) A, c = 8.887 ( 2 ) A, α = 76.843 ( 4 ) °, β = 79.933 ( 4 ) °, γ = 75.688 ( 4 ) °, V = 427.40 ( 17 ) A3, and Z = 2. Ba2TeO(PO4)2 has a novel one-dimensional chain structure that is composed of PO4 tetrahedra and TeO5 polyhedra. Te4+ cations are in asymmetric coordination environments attributable to their lone pairs. The lone pairs on the Te4+ cations point in the [100] and [-100] direction and interact with the Ba2+ cations. Infrared, Raman, and UV-Vis diffuse reflectance spectroscopy, thermogravimetric analysis, and dipole moment calculations are also presented.
Preparation and Characterization of Mixed Oxides of Selenium and Tellurium
Castro, Alicia,Jerez, Antonio,Pico, Carlos,Veiga, Maria Luisa
, p. 733 - 736 (1982)
Double oxides of Se and Te of composition Te3SeO8, Te2Se2O9, and TeSeO4 have been obtained for the first time by solid-state reactions between the corresponding elements and their oxides.The preparative conditions and the characterization of these compoun
Synthesis and characterization of the wide band-gap compound Pr2Te4O11
Ijjaali, Ismail,Flaschenriem, Christine,Ibers, James A.
, p. 115 - 119 (2003)
Single crystals of Pr2Te4O11 have been grown through the reaction of Pr6O11 and TeO2 in a CsCl flux at 1123 K. This compound, which is isostructural with Nd2Te4O11 and Ho2Te4O11, crystallizes in space group C2/c of the monoclinic system with four formula units in a cell of dimensions at 153 K of a = 12.6880(6) ?, b = 5.2361(3) ?, c = 16.2920(8) ?, β = 106.052(1)°, and V = 1040.17(9) ?3. The three dimensional structure is made from the interconnection between ∞2[Pr2O1014-] and ∞2[Te4O116-] networks. Pr2Te4O11 is a Curie-Weiss paramagnetic with an effective magnetic moment of 3.59(2) μB. Optical diffuse reflectance spectroscopy shows typical 4f-4f optical transitions for Pr(III), in addition to a wide band gap of 3.65 eV.
Standard enthalpies of formation of tellurium compounds. I. Tellurium dioxide
Cordfunke, E. H. P.,Ouweltjes, W.,Prins, G.
, p. 369 - 376 (1987)
The enthalpy of formation of TeO2(s) has been obtained by solution calorimetry using two independent thermochemical cycles: the first, in -3 H2SO4 + 0.10 mol * dm-3 K2Cr2O7 + 0.010 mol * dm-3 MnSO4>(aq), based
Synthesis of α-tellurium dioxide nanorods from elemental tellurium by laser ablation
Jiang, Zhi-Yuan,Xie, Zhao-Xiong,Zhang, Xian-Hua,Xie, Su-Yuan,Huang, Rong-Bin,Zheng, Lan-Sun
, p. 179 - 181 (2004)
Elemental tellurium was evaporated by laser ablation, the vapor of which was condensed and deposited on the surface of the heated glass surface and then formed α-tellurium dioxide nanorods with uniformly size distribution by oxidation in the chamber with hot air atmosphere. TEM images and Electron diffraction (ED) pattern confirm the crystallinity of α-phase tellurium dioxide. The formation process of the nanorods involves a vapor-liquid-solid (VLS) following a chemical oxidation in the hot air atmosphere, in which the low melting point tellurium serves as a liquid-forming reagent.
Standard molar Gibbs energy of formation of Ba3Te2O9(s) by transpiration technique
Parida,Banerjee,Prasad,Singh,Venugopal
, p. 285 - 287 (2002)
The standard molar Gibbs energy of formation of barium tellurite, Ba3Te2O9(s), was determined by the transpiration technique using pure oxygen as the carrier gas in the temperature range from 1119 to 1280 K. The condensate
Dynamics and crystal chemistry of tellurites - 1. Raman spectra of thallium tellurites: Tl2TeO3, Tl2Te2O5 and Tl2Te3O7
Mirgorodsky,Merle-Méjean,Thomas,Champarnaud-Mesjard,Frit
, p. 545 - 554 (2002)
Raman spectra of the three entitled crystals are analysed within the framework of a lattice-dynamical model treatment using preliminary obtained X-ray diffraction data. The short range atomic arrangement and spectrochemical peculiarities of these structures are jointly discussed, which is considered as an initial step for studying the nature of the glass phases in the xTl2O+(1-x)TeO2 system. The charged TeO32- groups and the neutral TeO2 quasi-molecules are proposed as the basic units forming the complex tellurite anions. However, no relevant characteristic frequencies can be indicated in the spectra since the interatomic separation in those units are highly variables and their vibrational states are mixed and delocalised.
Thermodynamic stability of Sm2TeO6
Balakrishnan,Pankajavalli,Ananthasivan,Anthonysamy
, p. 80 - 85 (2008)
The vapour pressure of Sm2TeO6 was measured using a thermal analyser with a horizontal arm. This TG based transpiration technique, was validated by measuring the vapour pressure of pure TeO2(s). The temperature dependence of the latter was measured to be log p (Pa) = {14.2 - 13321/T (K)} (±0.03) in the range 884-987 K. These data yielded a Δ H298 ° value of 269.7 ± 0.6 kJ mol-1 for the enthalpy of sublimation (third-law method) of TeO2 which compared well with the data reported in the literature. The temperature dependence of the vapour pressure of TeO2 over the mixture Sm2TeO6(s) + Sm2O3(s) generated by the incongruent vapourisation reaction,Sm2TeO6(s) → Sm2O3(s) + TeO2(g) + 1/2O2(g)could be expressed aslog p (Pa) = { 18.56 - 25469 / T (K) } ± 0.06 (1374 - 1533 K). The standard Gibbs energy of formation of Sm2TeO6(s) was derived from the above vapour pressure data in conjunction with auxiliary data for the other coexisting phases. The temperature dependence of the Gibbs energy of formation of Sm2TeO6 over the temperature range 1374-1533 K could be represented asΔ Gf ° (S m2 Te O6) (kJ mo l- 1) = { - 2399.3 + 0.5714 T (K) } ± 5.8. The Gibbs energy of formation of Sm2TeO6(s) is being reported for the first time.
Syntheses, structures, and characterization of new lead(II)-tellurium(IV)-oxide halides: Pb3Te2O6X2 and Pb3TeO4X2 (X = Cl or Br)
Porter, Yetta,Halasyamani, P. Shiv
, p. 205 - 209 (2003)
The syntheses, structures, and characterization of four new lead(II)-tellurium(IV)-oxide halides, Pb3Te2O6X2 and Pb3TeO4X2 (X = Cl or Br) are reported. The materials are synthesized by solid-state techniques, using Pb3O2Cl2 or Pb3O2Br2 and TeO2 as reagents. The compounds have three-dimensional structural topologies consisting of lead-oxide halide polyhedra connected to tellurium oxide groups. In addition, the Pb2+ and Te4+ cations are in asymmetric coordination environments attributable to their stereoactive lone pair. We also demonstrate that Pb3Te2O6X2 and Pb2TeO4X2 can be interconverted reversibly through the loss or addition of TeO2. X-ray data: Pb3Te2O6Cl2, monoclinic, space group C2/m (No. 12), a = 16.4417(11) A, b = 5.6295(4) A, c = 10.8894(7) A, β= 103.0130(10)°, Z = 4; Pb3Te2O6Br2, monoclinic, space group C2/m (No. 12), a = 16.8911(8) A, b = 5.6804(2) A, c = 11.0418(5) A, β = 104.253(2)°, Z = 4; Pb3TeO4Cl2, orthorhombic, space group Bmmb (No. 63), a = 5.576(1) A, b = 5.559(1) A, c = 12.4929(6) A, Z = 4; Pb3TeO4Br2, orthorhombic, space group Bmmb (No. 63), a = 5.6434(4) A, b = 5.6434(5) A, c = 12.9172(6) A, Z = 4.

