Die Tieftemperatur-Synthese von Oxidhalogeniden,YOX (X = Cl,Br, I), als Quelle der Verunreinigung von Yttriumtrihalogeniden,YX3, bei der Gewinnung nach der Ammoniumhalogenid-Methode. Die Analogie von YOCl und YSCl

Low-Temperature Synthesis of Oxyhalides, YOX (X = Cl, Br, I), as the Source of Impurity in the Preparation of Trihalides, YX₃, via the Ammonium Halide Route. Analogy of YOCl and YSCl Ammonium halides, NH₄X (X = Cl, Br, I), react with Y₂O₃ and Y₂S₃, respectively, at temperatures as low as 230=C (X = Cl), 280=C (Br), and 360=C (I) (molar ratio 12:1) to yield (NH₄)₃YX₆, NH₃, and H₂O (H₂S). The choice of smaller ratios than 12:1 (for example 2:1) results in the formation of oxyhalides, YOX, via the reaction of (NH₄)₃YX₆ with surplus Y₂O₃. This reaction is therefore the actual source of impurity of rare-earth trihalides in their preparation via the ammonium halide routes.     

Phosphaniminato-Komplexe von Cobalt und Zink mit Heterocubanstruktur. Die Kristallstrukturen von [CoI(NPMe3)]4 und [ZnI(NPMe3)]4

Phosphoraneiminato Complexes of Cobalt and Zinc with Heterocubane Structure. Crystal Structures of [CoI(NPMe₃)]₄ and [ZnI(NPMe₃)]₄ The title compounds have been prepared from CoI₂ and ZnI₂, respectively, and Me₃SiNPMe₃ by fusion reactions at 180°C in the presence of sodium fluoride. They crystallize from dichloromethane as dark green (Co) or colourless (Zn) single crystals including three molecules CH₂Cl₂ per formula unit, which were characterized by crystal structure determinations. [CoI(NPMe₃)]₄ · 3 CH₂Cl₂: Space group P3m1, Z = 2, structure solution with 2376 independent reflections, R = 0.033. Lattice dimensions at ?50°C: a = b = 1455.8, c = 1270.5 pm. [ZnI(NPMe₃)]₄ · 3 CH₂Cl₂: Space group P3m1, Z = 2, structure solution with 2197 independent reflections, R = 0.043. Lattice dimensions at ?60°C: a = b = 1454.9, c = 1270.5 pm. Both complexes are isostructural with one another. They form heterocubane structures in which the metal atoms are linked via μ₃-N-bridges of the phosphoraneiminato groups with M₄N₄ bridge-type bond angles close to 90°.     

Two-dimensional Blue Native/sodium dodecyl sulfate gel electrophoresis for analysis of multimeric proteins in platelets

Two-dimensional (2-D) Blue Native/SDS gel electrophoresis combines a first-dimensional separation of monomeric and multimeric proteins in their native state with a second denaturing dimension. These high-resolution 2-D gels aim at identifying multiprotein complexes with respect to their subunit composition. We applied this method for the first time to analyze two human platelet subproteomes: the cytosolic and the microsomal membrane protein fraction. Solubilization of platelet membrane proteins was achieved with the nondenaturing detergent n-dodecyl-beta-D-maltoside. To validate native solubilization conditions, we demonstrated the correct assembly of the Na,K-ATPase, a functional multimeric transmembrane protein, when expressed in Xenopus oocytes. We identified 63 platelet proteins after in-gel tryptic digestion of 58 selected protein spots and liquid chromatography-coupled tandem mass spectrometry. Nine proteins were detected for the first time in platelets by a proteomic approach. We also show that this technology efficiently resolves several known membrane and cytosolic multiprotein complexes. Blue Native/SDS gel electrophoresis is thus a valuable procedure to analyze specific platelet subproteomes, like the membrane(-bound) protein fraction, by mass spectrometry and immunoblotting and could be relevant for the study of protein-protein interactions generated following platelet activation.     

Does alpha-fluorination affect the structural trans-influence and kinetic trans-effect of an alkyl ligand? Molecular structures of Pd(TMEDA)(CH(3))(R(F)) and a kinetic study of the trans to cis isomerization of Pt(TMEDA)(CH(3))(2)I(R(F)) [R(F) = CF(2)CF(3), CFHCF(3), CH(2)CF(3)

Reaction of Pd(TMEDA)(CH(3))(2) [TMEDA = tetramethylethylenediamine] with fluoroalkyl iodides R(F)I affords a series of square planar Pd(II) complexes Pd(TMEDA)(CH(3))(R(F)) [R(F) = CF(2)CF(3) (9), CFHCF(3) (10), CH(2)CF(3) (11)], presumably by oxidative addition followed by reductive elimination of CH(3)I. The solid-state structures of each compound have been determined by single crystal X-ray diffraction studies, allowing the effect of increasing alpha-fluorination on the structural trans-influence of alkyl ligands to be examined. In these compounds there is no significant difference observed in the trans-influence of the three fluorinated alkyl ligands toward the trans-N atom, although a significant cis-influence on the neighboring methyl ligand is apparent. Oxidative addition of the same series of fluoroalkyl ligands to the corresponding Pt(TMEDA)(CH(3))(2) affords octahedral Pt(IV) complexes trans-Pt(TMEDA)(CH(3))(2)(R(F))I [R(F) = CF(2)CF(3) (12), CFHCF(3) (13), CH(2)CF(3) (14)] as the kinetic products. In each case, subsequent isomerization to the corresponding all cis-isomers is observed; in the case of 13, the stereocenter at the alpha-carbon results in two diastereomeric cis-isomers, which are formed at different rates. The molecular structures of 13 and its more stable all cis-isomer 16b have been crystallographically determined. Kinetic studies of the trans-cis isomerization reactions show the mechanism to involve a polar transition state, presumably involving iodide dissociation, followed by rearrangement of the cation, and iodide recombination. High dielectric solvents increase the rate, but solvent coordinating ability has no effect. Dissolved salts (LiI, LiOTf) show normal accelerative salt effects, with no inhibition in the case of added iodide, consistent with the formation of an intimate ion pair intermediate. The kinetic parameters show that the trans-effects of fluoroalkyl ligands in these compounds follow the order expected from the relative sigma-donor properties of the ligands, with CF(2)CF(3) < CFHCF(3) < CH(2)CF(3).     

The small momentum transfer k L o C→K S 0 C regeneration at high energies

Results of the first elastic K _S ^o regeneration experiment on carbon, using magnetic spark chamber spectrometer, are presented in the beam momentum interval 10p50 GeV/c. The d ifferentia cross section d/dt is reconstructed in the range 0·0025–t0·02 (GeV/c)² and its slopeB is found to be momentum independent with an average valueB=(65±11) (GeV/c)^–2. The results are in agreement with the calculations using the coherent production model.     

Experimental and theoretical studies of the Bi-excited collision systems He*(23 S) + He*(23 S, 21 S) at thermal and subthermal kinetic energies

We have carried out a comprehensive experimental and theoretical investigation of the autoionizing collision systems He*(2³ S, 2¹ S) + He*(2³ S). We present high resolution electron energy spectra, obtained with a single He* beam (average relative collision energy 〈E _rel〉=1.6 meV) and with crossed He* beams (〈E _rel〉> =61 meV). The spectra show substantial structure, and under single beam conditions fast oscillations due to the interference of incoming and outgoing heavy particle waves in the entrance channels are observed. Accurate ab initio potential curves for the seven lowest He*—He*(Σ) molecular states have been obtained from a Feshbach projection scheme, and width functions for He*(2³ S) + He*(2³ S) have been derived by Stieltjes imaging. Based on these ab initio data, detailed quantum mechanical calculations of the electron spectra have been carried out and provide a thorough understanding of the experimentally observed spectral features. Good overall agreement of the calculated spectra with the experimental data is observed. The close coincidence in the positions of the experimental and theoretical peaks, especially for He*(2³ S) + He*(2³ S), underlines the reliability of the ab initio potentials. In the He*(2¹ S) + He*(2³ S) electron spectrum, the dominant peak is traced to be due to autoionization from the 2³Σ⁺ _g molecular state accessed via an avoided crossing. We also present a detailed discussion of the total ionization cross sections σ_tot and of the fraction σ_AI/σ_tot for associative ionization together with a critical comparison with previous work. The ionization probabilities for close collisions in entrance channels, from which autoionization is spin-allowed, are near unity, and therefore the absolute values and the collision energy dependence of the total cross sections simply reflect the long-range behaviour of the excited state potentials.     

Synthesis and Structure of the New Compound La2O(CN2)2 Possessing an Interchanged Anion Proportion Compared to the Parent La2O2(CN2). Synthese und Kristallstruktur der neuen Verbindung La2O(CN2)2 mit einem vertauschten Anionenverhältnis gegenüber der Bezugsverbindung La2O2(CN2)

La₂O(CN₂)₂ was synthesized from a 1:1:2 molar reaction mixture of LaCl₃, LaOCl, and Li₂(CN₂) at 650 °C. Well developed single crystals were grown from a LiCl‐KCl flux. The crystal structure was refined as monoclinic (space group C2/c, Z = 2, a = 13.530(2) Å, b = 6.250(1) Å, c = 6.1017(9) Å, β = 104.81(2)°) from single crystal X‐ray diffraction data. The La³⁺ and (CN₂)^2— ions in the crystal structure of La₂O(CN₂)₂ can be compared to Fe³⁺ and S₂^2— ions in the cubic pyrite structure, being arranged like in a distorted NaCl type structure with their centers of gravity. In addition, the O^2— ions in La₂O(CN₂)₂ are occupying 1/4 of the tetrahedral voids formed by the arrangement of metal ions.     

Ternäre Halogenide der Seltenen Erden vom Typ A2MX5 (A = K,In, NH4, Rb,Cs; X = Cl,Br, I)

Ternary Rare-Earth Halides of the A₂MX₅ Type (A = K, In, NH₄, Rb, Cs; X = Cl, Br, I) Ternary rare-earth (=M) chlorides, bromides, and iodides In₂MCl₅, (NH₄)₂MCl₅, Rb₂MCl₅, Cs₂MCl₅, CsRbMCl₅, K₂MBr₅, Rb₂MBr₅, K₂MI₅, and Rb₂MI₅ have been synthesized. Single crystals of In₂PrCl₅, Rb₂PrCl₅, K₂PrBr₅, and K₂PrI₅ were grown and the structures refined. The other halides were characterized by x-ray powder patterns. They are isotypic either with K₂PrCl₅(orthorhombic, Pnma, Z = 4, hexagonal arrangement of chains of edge-connected polyhedra [PrX₇]) or with Cs₂DyCl₅ (orthorhombic, Pbnm, Z = 4, hexagonal arrangement of cis-corner-connected octahedra [DyCl₆]) which may be discriminated in structure field diagrams. The thermal expansion was investigated für Cs₂LuCl₅ and Rb₂PrX₅ (X = Cl, Br, I).     

Bestimmung von Spurenelementen in Silber und Silberverbindungen nach Abtrennung der Matrix

Zusammenfassung Es wird ein Verfahren zur Spurenbestimmung in Reinstsilber und Reinstsilberverbindungen beschrieben, das besonders für Routineanalysen geeignet ist. Das Verfahren beruht auf der hochselektiven Abtrennung des Matrixelementes von sämtlichen elektropositiveren Begleitspuren durch Reduktion mit Ameisensäure aus salpetersaurer Lösung, wobei das Silber als Amalgam abgeschieden wird. In der Spurenanreicherungslösung werden die für die Reinheitskontrolle von Silber und dessen Verbindungen wichtigsten Begleitelemente Pb, Cu, Cd, Zn amalgamvoltammetrisch, Tl, Ga, In, Fe, Ni, Mn flammenspektrometrisch und As photometrisch bestimmt. Die relativen Standardabweichungen liegen zwischen 2 und 13%, die Nachweisgrenzen zwischen 10^–6 und 10^–5%. Die prinzipiellen Möglichkeiten der Bestimmung weiterer Elemente sowie der Anwendung anderer Bestimmungsmethoden werden erörtert.über bisher bekannte Verfahren zur Spurenbestimmung in Silber wird berichtet.

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Summary A method for the determination of trace amounts of metallic impurities in high-purity silver and silver salts is described. The procedure is based on an extremely selective separation of the silver matrix from all accompanying trace elements more electropositive than silver. The silver is separated by reducing a nitric acid solution of the sample with formic acid and depositing the silver as an amalgam. In the solution containing the enriched traces the elements being most important for the purity control of silver and its salts are detected voltammetrically (Pb, Cu, Cd, Zn), flame-spectrometrically (Tl, Ga, In, Fe, Ni, Mn) and photometrically (As). The relative standard deviations for the different elements were found to be between 0.02 and 0.13, the limits of detection between 10^–6 and 10^–5%. The possibilities to detect further elements and to apply other determination methods are pointed out.Previously known procedures for detecting trace amounts of impurities in silver are reported.