The crystal growth and magnetic properties of Ln2LiIrO6 (Ln=La, Pr, Nd, Sm, Eu)

Single crystals of a series of lanthanide lithium iridium oxides, Ln₂LiIrO₆ (Ln=La, Pr, Nd, Sm, Eu) with the double perovskite structure have been grown from molten LiOH/KOH fluxes. The compounds crystallize in a distorted 1:1 rock salt lattice of Li⁺ and Ir⁵⁺ cations in the monoclinic space group P2₁/n. The magnetic susceptibilities of Ln₂LiIrO₆ (Ln=Pr, Nd, Sm, Eu) are presented.     

Sur une série de solutions solides de formule Ca2−xLnxMnO4 (Ln = Pr,Nd, Sm,Eu, Gd)

A new series of solid solutions Ca_2−xLn_xMnO₄ (Ln = Pr, Nd, Sm, Eu et Gd) in which manganese is found in both oxidation state of +III and +IV, have a structure derived from that of K₂NiF₄. The cationic distribution in sites of nine-fold coordination is random.     

Triangulation in the Li2O-Ln2O3-B2O3 (Ln = Nd, Eu, Dy, Yb, and Y) systems and the melting character of ternary compounds

Li₂O-Ln₂O₃-B₂O₃ (Ln = Nd, Eu, Dy, Yb, and Y) ternary systems were studied along their inner sections. Two types of ternary compounds were found: Li₃Ln₂(BO₃)₃ (Ln = Nd, Eu, Dy, and Yb) and Li₆Ln(BO₃)₃ (Ln = Dy and Yb). The systems were triangulated. Melts were chosen for growing single crystals of ternary compounds in multinary systems. Original Russian Text ? Sh.A. Gamidova, 2009, published in Zhurnal Neorganicheskoi Khimii, 2009, Vol. 54, No. 1, pp. 142–145.     

Molecular hydrides of samarium and europium LnH2(THF)2 (Ln=Sm or Eu): Synthesis and properties

The molecular hydrides Ln¹¹H₂(THF)₂ (Ln=Sm or Eu) were prepared by hydrogenolysis of the naphthalene complexes of divalent samarium and europium C₁₀H₈Ln(THF)₂ (Ln=Sm or Eu, respectively) as well as of the stilbene derivative of samarium(II) (PhCHCHPh)Sm(DME)₂ in THF at room temperature under atmospheric pressure. The resulting complexes were characterized by the data of microanalysis, IR spectroscopy, and magnetic susceptibility. Chemical properties of the complexes were studied. Translated fromIzvestiya Akademii Nauk. Seriya Khimicheskaya, No. 5, pp. 947–945, May, 2000.     

Syntheses, crystal structures and vibrational spectra of KLn(SO4)2·H2O (Ln=La, Nd, Sm, Eu, Gd, Dy)

The potassium lanthanide double sulphates KLn(SO₄)₂·H₂O (Ln=La, Nd, Sm, Eu, Gd, Dy) were obtained by evaporation of aqueous reaction mixtures of rare earth (III) sulphates and potassium thiocyanate at 298 K. X-ray single-crystal investigations show that KLn(SO₄)₂·H₂O (Ln=Nd, Sm, Eu, Gd, Dy) crystallise monoclinically (Ln=Sm: P2₁/c, Z=4, a=10.047(1), b=8.4555(1), c=10.349(1) Å, wR2=0.060, R1=0.024, 945 reflections, 125 parameters) while KLa(SO₄)₂·H₂O adopts space group P3₂21 (Z=3, a=7.1490(5), c=13.2439(12) Å, wR2=0.038, R1=0.017, 695 reflections, 65 parameters). The coordination environment of the lanthanide ions in KLn(SO₄)₂·H₂O is different in the case of the Nd/Sm/Gd and the Eu/Dy compounds, respectively. In the first case the Ln atoms are nine-fold coordinated in contrast to the latter where the Ln ions are eight-fold coordinated by oxygen atoms. The vibrational spectra of KLn(SO₄)₂·H₂O and the UV-vis reflection spectra of KEu(SO₄)₂·H₂O and KNd(SO₄)₂·H₂O are also reported.     

Crystal structures, magnetic and thermal properties of Ln3IrO7 (Ln=Pr, Nd, Sm, and Eu)

Ternary iridium oxides Ln₃IrO₇ (Ln=Pr, Nd, Sm, and Eu) were prepared and their crystal structures, magnetic and thermal properties were investigated. Powder X-ray diffractions (XRDs) were measured for all samples and neutron diffraction (ND) measurements were performed for Pr₃IrO₇. All the profiles were refined with space group Cmcm (No. 63). The lattice parameters for Pr₃IrO₇ refined by using ND data are a=10.9782(13) Å, b=7.4389(9) Å, and c=7.5361(9) Å. From specific heat and differential thermal analysis (DTA) measurements, Ln₃IrO₇ (Ln=Pr, Nd, Sm, and Eu) show thermal anomalies at 261, 342, 420, and 485 K, respectively. The results of powder high-temperature XRD and ND measurements indicate that these anomalies are due to the structural phase transition. Magnetic susceptibilities of these compounds were measured in the temperature range between 1.8 and 400 K. Nd₃IrO₇ shows an antiferromagnetic transition at 2.6 K. A specific heat anomaly has also been observed at the same temperature. For Ln₃IrO₇ (Ln=Pr, Sm, and Eu), no magnetic anomalies have been found in the experimental temperature range.     

Darstellung,Kristallstrukturen und Eigenschaften von Ln4Au2O9 (Ln = Nd,Sm, Eu)

Syntheses, Crystal Structures, and Properties of Ln₄Au₂O₉ (Ln = Nd, Sm, Eu) The compounds Ln₄Au₂O₉ (Ln = Nd, Sm, Eu) have been prepared from amorphous Au₂O₃ · 2–3 H₂O and Ln₂O₃ (Ln = Nd, Sm, Eu) via solid state reaction under elevated oxygen pressure adding KOH as mineralising agent. They are isostructural with La₄Au₂O₉ (Nd₄Au₂O₉: a = 11.9813(3), b = 6.1474(1), c = 11.9641(4); 453 powder intensities, R_p = 3.75%; Sm₄Au₂O₉: a = 11.8689(4), b = 6.0360(1), c = 11.8469(4) Å; 812 unique reflections, R₁ = 2.75%; Eu₄Au₂O₉: a = 11.8241(3), b = 5.9922(1) Å, c = 11.8013(3) Å; 1315 unique reflections, R₁ = 7.83%). The crystal structure of Nd₄Au₂O₉ was refined from powder diffraction data. The structures of Sm₄Au₂O₉ and Eu₄Au₂O₉ were solved and refined from single crystal data. The isolated square planar AuO₄ units are stacked as columns and are linked to each other by LnO₇‐polyhedra. One of the oxygen atoms is exclusively connected to the trivalent lanthanides in tetrahedral geometry. Ln₄Au₂O₉, Bi₂CuO₄, Bi₂AuO₅ and Bi₄Au₂O₉ are closely related, structurally. The lanthanoid aurates decompose between 700 and 800 °C into Ln₂O₃, Au and O₂. The effective magnetic moments 3.64 μ_B (Nd₄Au₂O₉), 1.7 μ_B (Sm₄Au₂O₉) and 3.3 μ_B (Eu₄Au₂O₉) confirm that the lanthanides are trivalent. The UV/VIS absorption spectra can be interpreted at assuming free ions.     

The Heterometallic Clusters of Trivalent Rare Earth Metals of [Ln(OPh)6{Li(dme)}3], with Ln=Eu and Sm

Two new heterobimetallic phenoxide Ln^III–Li complexes of formula [Ln(μ₂‐OPh)₆{Li(dme)}₃] (Ln=Sm, Eu) have been synthesized and characterized using single‐crystal X‐ray diffraction. These two compounds are isostructural.     

Crystal growth of Ln3GaO6 (Ln = Nd, Sm, Eu and Gd): Structural and optical properties

Single crystals of Ln₃GaO₆ (Ln = Nd, Sm, Eu, Gd) were grown out of a reactive high temperature hydroxide melt. The structures were solved by single-crystal X-ray diffraction. These gallium oxides crystallize in the polar space group Cmc2₁ where the orientation of the GaO₄ tetrahedra determines the polarity of the structure. The atomic positions along with the determination of the absolute structure are reported. The lanthanide atoms are located in a seven-fold coordination environment forming edge-sharing zigzag-chains. The photoluminescence was investigated and the europium and gadolinium members of this series exhibit intense luminescence in the visible portion of the spectrum.     

Kinetic diagrams of Ln2O2SO4 phase transformations in a H2 flow (Ln = La, Pr, Nd, Sm)

Kinetic diagrams of Ln₂O₂SO₄ (Ln = La, Pr, Nd, Sm) systems reduction in a H₂ flow are plotted for the first time in temperature-duration of treatment coordinates in which there are five areas of phase states. The temperatures of formation are established for products of the Ln₂O₂SO₄ + 4H₂ = Ln₂O₂S + 4H₂O reaction in the temperature range of 880–900 K and products of the Ln₂O₂SO₄ + H₂ = Ln₂O₃ + SO₂+ H₂O reaction in the temperature range of 1090–1220 K. The ranges of the temperature of formation of the homo-geneous Ln₂O₂S phase were found to decrease: 880–1220, 900–1200, 900–1180, and 900–1090 K in the sequence La-Pr-Nd-Sm.     

On the Perovskites Ba2LnSbO6 (Ln = Nd,Sm, Eu,Gd, Tb,Dy, Ho,Er, Yb)

Polycrystalline Ba₂LnSbO₆ (Ln = Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Yb) are cubic, perovskite-type compounds, space group Fm3m (No. 225), Z = 4, with a values from a = 8.544(2) Å for Ba₂NdSbO₆ to a = 8.368(1) Å for Ba₂YbSbO₆. X-ray diffraction data for all the compounds and the results of magnetic measurements for two of them are given.     

Darstellung und elektronenmikroskopische Untersuchung neuer Verbindungen des Typs Ln3MO4Cl5 (Ln = La?Nd; M = Ge,V)

Preparation and Electronmicroscopic Investigation of New Compounds Ln₃MO₄Cl₅ (Ln = La? Nd; M = Ge, V) By heating mixtures of LnOCl, LnCl₃ und GeO₂ (2:1:1) in evacuated silica tubes (Pt-shells inside) the compounds Ln₃GeO₄Cl₅ (Ln = La? Nd) were prepared. The case that the temperature of preparation (La: T = 900°C, 8d; Ce: T = 800°C, 9d; Pr, Nd: T = 650°C, 13 d) had to be reduced from Ln = La to Ln = Nd indicates a decreasing thermodynamic stability in this direction. The compound La₃VO₄Cl₅ was prepared by heating (900°C, 8d) a mixture (2:1:1) of LaOCl, LaCl₃ and VO₂ and was investigated by electronmicroscopic techniques.     

Ln3UO6Cl3 (Ln=La,Pr, Nd) -. Die ersten Oxochlorouranate der Seltenen Erden

Ln₃UO₆Cl₃ (Ln=La, Pr, Nd) — The First Oxochlorouranates of the Rare Earths . The new compounds Ln₃UO₆Cl₃ (Ln=La, Pr, Nd) were prepared by heating stoichiometric amounts of LnOCl/Ln₂O₃/U₃O₈ (7 : 1 : 1) (Ln=La, Nd) and PrOCl/Pr₆O₁₁/U₃O₈ (12 : 1 : 2) in silica ampoules (5 d, 1000°C, Ln=La; 9 d 800°C, Ln=Pr, Nd) in the presence of an excess of chlorine [p(Cl₂, 25°C)=1 atm]. Single crystals were obtained by chemical transport reactions using chlorine [p(Cl₂, 25°C)=1 atm] as transport agent [T₂=1000°C→T₁=900°C (Ln=La); T₂=840°C→T₁=780°C (Ln=Pr, Nd)]. Crystals of Ln₃UO₆Cl₃ (Ln=La, Pr, Nd) were investigated by X-ray diffraction methods and La₃UO₆Cl₃ additionally by high resolution electron microscopy. The compounds Ln₃UO₆Cl₃ crystallize in the hexagonal spacegroup P6₃/m (No. 176) with Z=2 formula units per unit cell. Isotypical structure refinements resulted in R=3.04% respectively R_w=1.91% (Ln=La), R=4.72% respectively R_w=3.80% (Ln=Pr) and R=3.99% respectively R_w=2.49% (Ln=Nd). Uranium is coordinated with six oxygen atoms forming a trigonal prism. Lanthanide ions are 10-coordinated (6 oxygen atoms, 4 chlorine atoms).     

Hydrothermal phase equilibria in Ln2O3-H2O systems

Hydrothermal phase equilibria studies have been carried out in the Ln₂O₃-H₂O systems (Ln = La, Pr, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb and Lu) and the stability fields of the phases Ln(OH)₃ LnOOH and Ln₂O₃-C have been established in the pressure-temperature range of 25000 psi and 900° C. The sequioxides Ln₂O₃-C are stable only in the last four systems of Er to Lu along with the Ln(OH)₃ and LnOOH. The systems from Nd to Ho have only Ln(OH)₃ and LnOOH as stable phases and those from La to Pr have only Ln(OH)₃ as the stable phase. The unit cell parameters of trihydroxides deviate from the values reported in the literature and this is attributed to the contamination of CO₂ in the starting material.     

Structures of nonlinear hexagonal boratotungstates Ln3BWO9 (Ln = La, Pr, Nd, Sm, Gd, Tb, Dy)

Polycrystalline boratotungstates of composition Ln₃BWO₉ (Ln = Pr, Nd, Sm, Gd, Tb, Dy) are prepared by solid-phase synthesis and structurally studied. The structures are refined using the Rietveld method for hexagonal space group P6₃ (Z = 2). The boratotungstate structures are frameworks. The rare-earth cations in the structure are coordinated by an array of nine oxygen atoms (three oxygen atoms from borato groups BO₃ and six from WO₆ polyhedra). The nature of the optical nonlinearity in the hexagonal boratotungstates Ln₃BWO₉ is a direct consequence of the acentricity of both the tungstate and the rare-earth polyhedra in the structure. Dimorphism is discovered in polycrystalline La₃BWO₉.     

Standard molar enthalpies of formation of Ln(C9H6NO)2(C2H3O2) (Ln: Nd, Sm)

Using an on-line solution-reaction isoperibol calorimeter, the standard molar enthalpies of reaction for the general thermochemical reaction: LnCl₃·6H₂O(s) + 2C₉H₇NO(s) + CH₃COONa(s) = Ln(C₉H₆NO)₂(C₂H₃O₂)(s) + NaCl(s) + 2HCl(g) + 6H₂O(l) (Ln: Nd, Sm), were determined at T=298.15 K, as  kJ mol^−l, respectively. From the mentioned standard molar enthalpies of reaction and other auxiliary thermodynamic quantities, the standard molar enthalpies of formation of Ln(C₉H₆NO)₂(C₂H₃O₂)(s) (Ln: Nd, Sm), at T=298.15 K, have been derived to be: −(1494.7±3.3) and −(1501.5±3.4) kJ mol^−l, respectively.     

Kinetics of Ruddlesden-Popper Phase Formation: II. Mechanism of Nd2SrAl2O7 and Sm2SrAl2O7 Formation

Phase formation in the Ln₂O₃-SrO-Al₂O₃ system (Ln = Nd, Sm) was studied in the range 900-1530°C. Comparative examination of the kinetics of the synthesis of Ln₂SrAl₂O₇ oxides (Ln = La, Nd, Sm) showed that this reaction proceeds by a common mechanism and is substantially faster for neodymium and samarium complex aluminates than for lanthanum aluminate.     

Synthesis of Lanthanide Bromide Complexes from Oxides. The Crystal Structures of [LnBr2(diglyme)2][LnBr4(diglyme)] (Ln = Sm,Eu) and [LnBr2(HMPA)4]Br·0.5H2O (Ln = La,Sm)

The reaction of the lanthanide oxides, bromotrimethylsilane and water in THF resulted in [LnBr₃(THF)_x]. If digylme (diglyme = diethylen glicol dimethyl ether) was added to these reaction mixtures in the mole ratio n(Ln): n(diglyme) ～ 1: 2.2 – 3, the ionic complexes [LnBr₂(diglyme)₂][LnBr₄(diglyme)] (Ln = La ( 1 ), Sm ( 2 ), Eu ( 3 )) were isolated. Crystal structures of the two new complexes, 2 and 3 , which were recrystallized from dichloromethane, were determined. The immediate reaction of the complexes 1 and 2 with HMPA (HMPA = hexamethylphosphoramide) in toluene resulted in [LnBr₂(HMPA)₄]Br·0.5H₂O (Ln = La( 4 ), Sm ( 5 )).     

Kinetics of the transformation of Ln2O2SO4 into Ln2O2S (Ln = La, Pr, Nd, and Sm) in a hydrogen flow

The kinetic dependences of the yield of Ln₂O₂S (Ln = La, Pr, Nd, and Sm) upon the treatment of Ln₂O₂SO₄ in a hydrogen flow at 950, 1120, and 1170 K are constructed. The plots are approximated by Avrami-Erofeev equations, equations of compressed volume and compressed surface, and Jander’s equation. The correctness of choosing these equations is evaluated using the numerical values of Fisher’s criterion. Images of the particles of Nd₂O₂SO₄ → Nd₂O₂S transformation in the flow are obtained on an Ntegra Aura atomic force probe microscope. A mechanism of the crystal growth of the Nd₂O₂S phase from the nucleation site of the Nd₂O₂SO₄ and Nd₂O₂S phase boundaries is proposed.     

The thermodynamic properties of Ln2BaO4 (Ln = Sm, Dy, Ho)

The thermodynamic properties of the Ln₂BaO₄ phases (Ln = Dy, Ho, Sm) were studied by the electromotive force method with a fluoride electrolyte (890–1180 K), solution calorimetry in 1.07 N hydrochloric acid at 298.15 K, and differential scanning calorimetry (298–860 K). The experimental data were jointly processed, and the thermodynamic functions of the compounds over the temperature range 298–1200 K were calculated.