Die Systeme des Typs MCl/AlCl3/SO2 (M = Li,Na, K,NH4)

The MCl/AlCl₃/SO₂ Systems (M = Li, Na, K, NH₄) Phase diagrams of the ternary systems of the type MCl/AlCl₃/SO₂ were determined by measurement of SO₂ pressure, solubilities, and by thermal analysis. The complete phase diagram in the range from ?30 to +50°C is given for the case M = Na, partial diagrams for M = Li, K, NH₄. There exist solid compounds of the type MAlCl₄ · nSO₂ (M = Li, Na; n = 1.5 and 3) (M = K; n = 1.5 and 5) (M = NH₄; n = 5). Liquid phases can be obtained at room temperature and atmospheric pressure in the NaCl or LiCl containing systems.     

Kristallstruktur,Leitfähigkeit und magnetische Suszeptibilität von Er2Te3

Crystal Structure, Conductivity, and Magnetic Susceptibility of Er₂Te₃ Via a chemical vapour transport reaction with ErCl₃ as transporting agent, single crystals of Er₂Te₃ up to a size of 1.5 mm are available. X-ray structure analysis revealed for the compound the Sc₂S₃-type with the space group Fddd and the lattice parameters a = 1212.7(2) pm, b = 858.1(2) pm and c = 2572.8(4) pm (Z = 16). According to measurements of the fundamental absorption (DRIFT) the compound is a semiconductor with a band gap of 0.77(5) eV. Magnetic susceptibility measurements revealed paramagnetic behaviour in the temperature range 5–300 K with μ_p = 9.07 B.M. and θ_p = –4.3 K.     

Kristallstruktur und elektrische Leitfähigkeit von Li2–2xMn1+xCl4-Spinelltyp-Mischkristallen

Crystal Structure and Electric Conductivity of Spinel-Type Li_2–2xMn_1+xCl₄ Solid Solutions The electric conductivity of the fast lithium ion conductors Li_2–2xMn_1+xCl₄ was measured by impedance spectroscopic methods. The conductivities obtained, e.g. ～ 4 × 10^?1 Ω^?2 cm^?1 at 570 K, depend only little on the lithium content. The crystal structure of Li_1.6Mn_1.2Cl₄ was determined by neutron powder and X-ray single crystal diffraction (space group Fd3 m, Z = 8, a = 1 049.39(6) pm, R_w = 1.4% on the basis of 170 reflections). The lithium deficient chloride crystallizes in an inverse spinel structure like the stoichiometric compound Li₂MnCl₄ according to the formula (Li_0,8)[Li_0,4Mn_0,6]₂Cl₄ with vacancies ( ) at the tetrahedral sites. The decrease of the M_oct? Cl distances with the increase of x reveals that the ionic radius of Mn²⁺ in chlorides is equal or even smaller than that of Li⁺ opposite to fluorides and oxides. The ? Cl distances of spinel type chlorides are 237 ( _tet) and 274 pm ( _oct), respectively. The mechanism of the ionic conductivity is discussed.     

RbHg2 und CsHg2, Darstellung,Kristallstruktur, elektrische Leitfähigkeit

RbHg₂ and CsHg₂ — Preparation, Crystal Structures, and Electrical Conductivities Preparation, crystal structures and electrical conductivities of the new compounds RbHg₂ and CsHg₂ are described. Both compounds form reddish-black, air sensitiv single crystals with a metallic lustre and crystallize isotypically to the orthorhombic KHg₂ in the space group Imma (No. 74). The specific electrical resistivity of pressed powder pellets shows a metallic behaviour between 1.4 K and room temperature. From an analysis of crystal structures and electrical properties one can suggest a formula M⁺(Hg₂)⁰e^? to describe the chemical bonding in these compounds qualitatively.     

Ternäre Halogenide vom Typ A3MX6. III [1, 2]. Synthese,Strukturen und Ionenleitfähigkeit der Halogenide Na3MX6 (X = Cl,Br)

Ternary Halides of the A₃MX₆ Type. III [1, 2]. Synthesis, Structures, and Ionic Conductivity of the Halides Na₃MX₆ (X = Cl, Br) The bromides Na₃MBr₆ crystallize with the stuffed LiSbF₆-type structure (type I; M = Sm? Gd) or with the structure of the mineral cryolite (type II; M = Gd? Lu). The structure types were refined from single crystal X-ray data (Na₃SmBr₆: trigonal, space group R3 , a = 740.8(2) pm, c = 1 998.9(8) pm, Z = 3; Na₃YBr₆: monoclinic, space group P2₁/n, a = 721.3(4) pm, b = 769.9(2) pm, c = 1 074.8(4) pm, β = 90.60(4)°, Z = 2). Reversible phase transitions from one structure to the other occur. The phase transition temperatures were determined for the bromides as well as for the chlorides Na₃MCl₆ (M = Eu? Lu). The refinement of both structures for one compound was possible for Na₃GdBr₆ (I: trigonal, space group R3 , a = 737.1(5) pm, c = 1 887(2) pm, Z = 3; II: monoclinic, space group P2₁/n, a = 725.2(1) pm, b = 774.1(3) pm, c = 1 080.1(3) pm, β = 90.76(3)°, Z = 2). All compounds exhibit ionic conductivity of the sodium ions which decreases with the change from type I to type II. The conductivity of the bromides is always higher when compared with the respective chlorides.     

Neue schnelle Ionenleiter vom Typ MMIIICl6 (MI = Li,Na, Ag; MIII = In,Y)

Novel Fast Ion Conductors of the Type M M^IIICl₆ (M^I = Li, Na, Ag; M^III = In, Y) The ternary chlorides Li₃InCl₆, Na₃InCl₆, Ag₃InCl₆, and Li₃YCl₆ have been studied by difference scanning calorimetry, high-temperature X-ray, infrared, and high-temperature Raman methods. Impedance spectroscopic measurements exhibit fast ionic conductivity increasing in the sequence Na₃InCl₆ < Li₃YCl₆ < Ag₃InCl₆ < Li₃InCl₆. In the range of 300°C, Li₃InCl₆ is the best lithium ion conductor known so far (σ = 0,2 Ω^?1 cm^?1 at 300°C). With the exception of Na₃InCl₆, the chlorides exhibit complicated order-disorder phase transitions.     

Synthese und Kristallstruktur der Ternären Selten-Erd-Chloride Na2MCl5 (M = Sm,Eu, Gd)

Synthesis and Crystal Structure of the Ternary Rare Earth Chlorides Na₂MCl₅ (M = Sm, Eu, Gd) Single crystals of Na₂EuCl₅ were obtained from the melt of NaCl and EuCl₃ in a 2:1.2 molar ratio by slow cooling. It crystallizes in the orthorhombic crystal system (space group Pnma) with the structure of K₂PrCl₅ with a = 1 204.0(3) pm, b = 833.9(3) pm, c = 768.2(3) pm, Z = 4. Pure powder samples of the compounds Na₂MCl₅ (M = Sm? Gd) are available by heating mixtures of the binary components below the melting point.     

Beiträge zu den Eigenschaften von Titanaten mit Ilmenitstruktur. II. Zur Thermodynamik und elektrischen Leitfähigkeit von NiTiO3 und anderen oxidischen Phasen mit Ilmenitstruktur

Contributions to the Properties of Titanates with Ilmenite Structure. II. Study on the Thermodynamics and the Electrical Conductivity of NiTiO₃ and Other Phases with Ilmenite Structure NiTiO₃ shows a phase transition at high temperatures (T_c = 1290°C). The standard enthalpy and entrop of the reaction NiO + TiO₂ = NiTiO₃ was estimated for temperatures above and below the transition temperature using emf-measurements based on the following solid state galvanic cell: Ni,TiO₂, NiTiO₃|ZrO₂(+CaO)|Ni,NiO. The transition enthalpy was found to be 18 ± 2 kJmol^?1, The transition entropy is 12 ± 1 JK^?1mol^?1. This is in good agreement with the calculated entropy change for an order-disorder transition (11.5 JK^?1mol^?1). The influence of other cations like Mg²⁺ and Co²⁺ on the transition temperature was investigated by measurements of the electrical conductivity as a function of composition. Ni_1?xMg_xTiO₃ shows a strong shift of the transition to higher temperatures if a small part of the Ni²⁺ was replaced by Mg²⁺. A linear correlation between the temperature shift and the amount of Co²⁺ was found for Ni_1?xCo_xTiO₃. Thermoanalytical investigations reveal an endothermic peak during the heating period some degrees below the melting point of CoTiO₃. The substitution of Ge⁴⁺ for Ti⁴⁺ is without any influence on the transition temperature. By doping the NiTiO₃ with Ga₂O₃, the anomalous increase of the electrical conductivity with temperature is shifted to lower temperatures.     

Ternäre Halogenide vom Typ A3MX6. VI [1]. Ternäre Chloride der Selten-Erd-Elemente mit Lithium,Li3MCl6 (M  Tb?Lu,Y, Sc): Synthese,Kristallstrukturen und Ionenbewegung

Ternary Halides of the A₃MX₆ Type. VI. Ternary Chlorides of the Rare-Earth Elements with Lithium, Li₃MCl₆ (M ? Tb? Lu, Y, Sc): Synthesis, Crystal Structures, and Ionic Motion Single crystal X-ray studies on the ternary chlorides Li₃ErCl₆, Li₃YbCl₆ and Li₃ScCl₆ show that they crystallize in three different structure types. Li₃ErCl₆ (trigonal, P3 ml, Z = 3, a = 1117.7(2); c = 603.6(2) pm; the chlorides with M ? Tb? Tm, Y are isotypic) and Li₃YbCl₆ (orthorhombic, Pnma, Z = 4, a = 1286.6(1); b = 1113.2(1); c = 602.95(8) pm; Li₃LuCl₆ is isotypic) have very similar structures that may be derived from hexagonal closest packings of chloride ions with the cations occupying octahedral holes in part statistically. Li₃ScCl₆ (monoclinic, C2/m, Z = 2, a = 639.8(1); b = 1104.0(2); c = 639,1(1) pm; β = 109.89(1)°) crystallizes isotypic with Na₃GdI₆ and Li₃ErBr₆, structures that may be derived from a cubic closes packings of anions. The ionic movement in Li₃YCl₆ and Li₃YbCl₆ has been investigated by impedance and ⁷Li-NMR spectroscopy.     

Neue gemischtvalente ternäre Bromide und Iodide mit Dysprosium und Thulium vom Typ A5M3X12

New Mixed‐Valence Ternary Bromides and Iodides of Dysprosium and Thulium of the Type A₅M₃X₁₂ The new ternary mixed‐valence bromides and iodides of dysprosium and thulium Rb₅Dy₃Br₁₂, Rb₅Tm₃Br₁₂, K₅Dy₃I₁₂, K₅Tm₃I₁₂, Rb₅Dy₃I₁₂ and Rb₅Tm₃I₁₂ were obtained by metallothermic reduction of DyBr₃, TmBr₃, DyI₃ and TmI₃, respectively, with potassium and rubidium in the presence of the respective alkali metal halides in sealed niobium containers. The crystal structure was determined for the example of K₅Dy₃I₁₂ (hexagonal, P 6 2m, Z = 1; a = 1446.7(2), c = 473.3(1) pm): DyI₆ octahedra are connected via common trans edges to chains. Magnetic measurements on X‐ray pure samples show Curie‐Weiss behaviour at sufficiently high temperatures. Antiferromagnetic coupling occurs at low temperatures.     

Les systemes binaires AlPO4−M3PO4 (M=Li,Na, K)

The liquid-solid phase diagram of the binary systems AlPO₄?M₃PO₄(M=Li, Na, K) have been established. The additional compounds Na₃Al(PO₄)₂, Na₃Al₂(PO₄)₃ and K₃Al₂(PO₄)₃ have been found again. A new compound K₃Al(PO₄)₂ is observed. The melting point of Na₃PO₄ is 1545°C and K₃PO₄ does not melt up to 1700°C.     

The [Au(CH3SO3)4]– Anion in the Crystal Structures of M[Au(CH3SO3)4] (M = Li,Na, Rb)

The reactions of Au(OH)₃, M₂CO₃ (M = Li, Na, Rb), and methanesulfonic acid at elevated temperatures in sealed glass ampoules lead to single crystals of M[Au(CH₃SO₃)₄] (M = Li, Na, Rb). In the crystal structures of Li[Au(CH₃SO₃)₄] (tetragonal, I$\bar{4}$ , Z = 2,a = 938.64(2) pm, c = 917.01(3) pm, V = 807.93(4) ų) and Rb[Au(CH₃SO₃)₄] (tetragonal, P$\bar{4}$ 2₁c, Z = 2, a = 946.7(1) pm,c = 889.9(1) pm, V = 797.6(2) ų) the complex aurate anions are linked by the M⁺ ions in three dimensions. Contrastingly, in the structure of Na[Au(CH₃SO₃)₄] (triclinic, P$\bar{4}$ , Z = 1, a = 540.04(2) pm,b = 863.75(2) pm, c = 973.29(3) pm, α = 72.694(2)°, β = 75.605(2)°, γ = 77.687(2)°, V = 415.05(2) ų) the complex anions are connected into layers that are further connected by weak hydrogen bonds. The thermal decomposition of Li[Au(CH₃SO₃)₄] was monitored up to 500 °C and leads in a multi‐step process to elemental gold and Li₂SO₄.     

Ternäre Bromide und Iodide zweiwertiger Lanthanide und ihre Erdalkali-Analoga vom Typ AMX3 und AM2X5

Ternary Bromides and Iodides of Divalent Lanthanides and Their Alkaline-Earth Analoga of the Type AMX₃ and AM₂X₅ Metallothermic reduction of the tribromides and -iodides MX₃ (M = Sm, Dy, Tm, Yb) with alkali metals as well as with indium and thallium (A = Cs, Rb, K, In, Tl) results in most cases in ternary compounds with the composition AMX₃ and AM₂X₅, respectively. Analogous compounds with M = Ba, Sr, Ca were synthesized from the binary components. The AMX₃ compounds crystallize with the following types of structure: the perovskite-type and its distorted variants, the NaNbO₃-II- and the GdFeO₃-type, the NH₄CdCl₃- and the stuffed PuBr₃-type. These structure types differ by a gain of condensation of the [MX₆] octahedra (three-dimensional connection via corners within the variants of the perovskite-type, double chains of edge- and face-connected octahedra within the NH₄CdCl₃-type, and layers of corner- and edge-connected octahedra within the stuffed PuBr₃-type of structure). This comes along with a reduction of the coordination number of A⁺ from 12 (“ideal” perovskite) to 8 + 2 (GdFeO₃-type), 9 (NH₄CdCl₃-type), and 8 (stuffed PuBr₃-type). Thus, the A/[MX₆] size ratio determines which AMX₃ type of structure is adopted. If the M²⁺ ion is large enough, ternary compounds with the composition AM₂X₅ occur either in addition to the AMX₃ compounds or exclusively. They crystallize with the TlPb₂Cl₅ type of structure (C.N.(M²⁺) = 7 and 8). All of the AMX₃ and AM₂X₅ compounds are summarized in a structure field diagram.     

Ternäre Bromide des Aluminiums,Galliums und Indiums vom Typ AIMIIIBr4 (AI = Na,Ga, K,In, Rb) Eine Übersicht

Ternary Bromides of Aluminium, Gallium, and Indium of the Formula Type A^IM^IIIBr₄ (A^I = Na, Ga, K, In, Rb). An Overview The fourteen possible bromides A^IM^IIIBr₄ with A^I = Na, Ga, K, In, Rb and M^III = Al, Ga, In are obtained from mixtures of the binary components, ABr and MBr₃. Six different structure types are observed: NaGaBr₄-, NaAlCl₄-, GaCl₂-, β-GaBr₂-, KAlBr₄-, and BaSO₄-type. Singlecrystal data are reported for the examples of NaGaBr₄, KGaBr₄, and InGaBr₄. Without exception, slightly distorted tetrahedra [MBr₄]^? occur. The structural variety must be sought in the adjustment of the coordinational needs of the counter cations A⁺ (coordination numbers between six and twelve).     

Synthese und Kristallstruktur von (NH4)3Cu4Ho2Br13. Weitere Bromide vom Typ (NH4)3Cu4M2Br13 (M = Dy?Lu,Y) und Rb3Cu4Ho2Br13

Synthesis and Crystal Structure of (NH₄)₃Cu₄Ho₂Br₁₃. Further Bromides of the (NH₄)₃Cu₄M₂Br₁₃ Type (M = Dy? Lu, Y) and on Rb₃Cu₄Ho₂Br₁₃ Single crystals of (NH₄)₃Cu₄Ho₂Br₁₃ were obtained for the first time from the reaction of CuBr with HoBr₃ which was contaminated with NH₄Br: cubic, space group Pn3 , Z = 2, a = 1101.71(5) pm. The crystal structure may be considered as a variant of the fluorite type according to [(HoBr₆)₄][(NH₄)₆(Cu₄Br)₂] ? Ca₄F₈. Pure products can be prepared from the binary halides in glass ampoules at 350°C. The bromides (NH₄)₃Cu₄M₂Br₁₃ (M = Dy? Lu, Y) and Rb₃Cu₄Ho₂Br₁₃ are isotypic with (NH₄)₃Cu₄Ho₂Br₁₃.     

Über Ruthenium-Perowskite vom Typ Ba2BRuO6 und Ba3BRu2O9 mit B = Indium,Rhodium

On Ruthenium perovskites of type Ba₂BRuO₆ and Ba₃BRu₂O₉ with B = Indium, Rhodium The black perovskites Ba₂InRu⁵⁺O₆ and Ba₃InRu₂O₉ (mean oxydation state of ruthenium: +4.5) adopt the hexagonal BaTiO₃ structure and form a continuous series of mixed crystals. According to the intensity calculations and analysis of the vibrational spectroscopic data an ordered distribution between indium and ruthenium is present: 1:1 order in Ba₂InRuO₆ (space group P3 m1 ? D; R′ = 5.3%); 1:2 order in Ba₃InRu₂O₉ (space group P6₃/mmc ? D; R′ = 4.6%). The corresponding black Rh compounds, Ba₂RhRuO₆ and Ba₃RhRu₂O₉, crystallize in the rhombohedral 9 L type of BaRuO₃.     

Bildung und Charakterisierung von Oberflächenverbindungen in den Systemen (C6H5CH2)4M/γ-Al2O3 (M = Ti,Zr)

Formation and Characterization of Surface Compounds in the Systems (C₆H₅CH₂)₄M/γ-Al₂O₅ (M = Ti, Zr) By O-bridges anchored surface-compounds are formed by protolytic splitting off of benzyl groups if tetrabenzyltitanium and -zirconium are added to γ-alumina. These compounds contain the metal in different oxidation states in dependence on the carrier/substrate ratio and the density of OH groups on the alumina surface. The different kinds of surface compounds are discussed. Furthermore, the products formed by thermal decomposition and hydrogenolysis of the surface compounds were analysed. With regard to catalytic conversion reactions of hydrocarbons systems of the type (C₆H₅CH₂)₄M/Pt/γ-Al₂O₃were involved in the investigations.     

Schwingungsspektren fester,flüssiger und gelöster Metallpolysulfide. II. Polysulfide Rb2Sn und Cs2Sn (n ⩾ 4) sowie Na2S4

Vibrational Spectra of Solid, Liquid, and Soluted Metal Polysulphides. II Polysulphides Rb₂S_n (n ? 4) and Na₂S₄ All compounds have been prepared from the elements in liquid ammonia. Whereas Rb₂S₄ has no defined composition, the vibrational spectra of Cs₂S₄ and their structure similar to Na₂S₄ indicate that Cs₂S₄ is a well-defined compound in contrast to former suggestions. Rb₂S₅ and Cs₂S₆ are the members with the greatest chainlength of their homologe series. While Na₂S₄ still exists of S₄^2? chains in the melt the other polysulhpides disproportionate to S₃^? radicals and probably monosulphide. In the melt of Cs₂S₆, quenched to room temperature, a double branched chain structure, the thio-analogue of dithionite, S₂S₄^2?, is suggested. All polysulphides have a mean valence frequency, which is independent of the cation and decreases with increasing chainlength.     

Verbindungen A3M5 (A = Erdalkalimetall,M = Triel/Tetrel): Eine Fallstudie zur strukturellen und elektronischen Stabilität polarer intermetallischer Phasen

Compounds A₃M₅ (A = alkaline earth, M = triel/tetrel): A Case Study on Structural and Electronic Factors Stabilizing Polar Intermetallics Starting from the non electron precise binary compounds Ca₃Ga₅/Sr₃In₅ (Hf₃Ni₂Si₃ type) and Ba₃Al₅ at one hand and Ba₃Pb₅ (Pu₃Pd₅ type) at the other hand, a series of new ternary intermetallics of the general formula A₃M₅ (A: alkaline earth, M: triel/tetrel) has been synthesized, structurally characterized and studied by band structure calculations. The chemical substitution of M in A₃M₅ allows, via the continous variation of the radius ratio (r_A:r_M) and the valence electron number (VE/M) the detection of the geometrically and electronically determined stability ranges of the three structure types formed by the binary compounds. At values of r_A:r_M between 1.30 and 1.52 in the triel rich region of A₃M′_xM″_5?x the Hf₃Ni₂Si₃ type (orthorhombic, space group Cmcm) is formed: In Ca₃Ga₅ up to 1.8 Ga can be substituted by Al, in Sr₃In₅ similar amount of In can be replaced by either Al or Ga. The mixed trielide Sr₃Al_2.6Ga_2.4 (a = 468.4(1), b = 1132.5(1), c = 1570.0(2) pm, R1 = 0.0261) can be obtained, although both corresponding binary phases are not known. At larger values of the ratio r_A/r_M as in Ba₃Al₃Ga₂ (Ba₃Al₅ type, hexagonal, space group P6₃/mmc, a = 598.9(1), c = 1456.0(3) pm, R1 = 0.0353) layers of condensed M₅ building blocks with Al‐Al partial bonds are formed. Substituting one In position in Sr₃In₅ against Pb results in the isotypic, but electron precise Zintl compound Sr₃In₄Pb (a = 506.1(1), b = 1191.8(3), c = 1650.2(4) pm, R1 = 0.0286), where the Fermi level in shifted into a distinct minimum of the density of states. Conversely, at the tetrele rich end of the series A₃In_xPb_5?x, characterized by compounds of the Pu₃Pd₅ type (orthorhombic, space group Cmcm) with almost isolated nido clusters M₅, a minimum of the DOS can be reached, if Pb is partially substituted by In (A₃In_xPb_5?x with A = Sr/Ba: x = 0.7/0.6; a = 1084.6(2)/1118.6(2), b = 867.1(2)/904.4(1), c = 1104.8(2)/1133.9(2) pm, R1 = 0.0394/0.0434).