Die Massenspektren von Pd6Cl12, Pt6Cl12 und PdnPt6−nCl12

Mass Spectra of Pd₆Cl₁₂, Pt₆Cl₁₂, and Pd_nPt_6?nCl₁₂ Pd₆Cl₁₂, and Pt₆Cl₁₂ and both together are volatilised in a mass spectrometer. 3 Cl and 1 Pd have approximately the same mass, therefore isotopes of Pd and Pt are used (¹⁰⁸Pd, ₁₉₄Pt). With an ionisation energy of 50 eV part of the vapourised molecules is strongly fragmented. With a lower ionisation energy the molecule ions Pd₆Cl₁₂⁺, Pt₆Cl₁₂⁺ and Pd_nPt_6?nCl₁₂⁺ are only observed.     

Die thermodynamische Stabilität der Molekeln Pd6Cl12, Pd6Br12 und Pt6Cl12

Thermodynamic Stability of Pd₆Cl₁₂, Pd₆Br₁₂, and Pt₆Cl₁₂ Molecules Vapour pressure data of PdCl₂ and PdBr₂ taken from the literature have been used to get new informations regarding the vapourization of Pd₆Cl₁₂ molecules. Using mixtures of PdCl₂ and AgBr as source materials, besides Pd₆Cl₁₂ molecules the vapourization of Pd₆Cl_12-nBr_n with n = 1 – 8 has been observed in a mass spectrometer. Semi quantitative observations concerning the vapourization of Pt₆Cl₁₂ molecules from a PtCl₂ solid are reported. Heats of formation and standard entropy data for the molecules Pd₆Cl₁₂, Pd₆Br₁₂ and Pt₆Cl₁₂ are given.     

Pt6Cl12·(1,2,4‐C6H3Cl3), a Structurally Characterized Cocrystallization Product of Pt6Cl12

The reaction of platinum(II) chloride with 1,2,4‐trichlorobenzene gives the novel platinum complex Pt₆Cl₁₂·(1,2,4‐C₆H₃Cl₃). It is the first example of an cocrystallization product of platinum(II) chloride and organic molecules whose crystal structure has been established.     

Synthesis and structures of Sc7Cl12 and Zr6Cl15

The indicated nine-electron clusters of scandium and zirconium are formed in transport reactions at 880/900°C and 750/600°C, respectively. Sc₇Cl₁₂ (R¯3, a – 12.959(2), c – 8.825(2), Z – 3) can be described as c.c.p. Sc₆Cl₁₂ clusters with isolated metal atoms in all octahedral interstices or as Sc³⁺(Sc₆Cl₆ⁱCl₆^i?a) ^3? with Sc³⁺ in Clⁱ octahedra between Sc₆Cl sheets. Metal-metal distances within the cluster are 3.201?3.230(2) Å. Zr₆Cl₁₂ⁱCl crystallizes in the Ta₆Cl₁₅ structure (Ia3d, a – 21.141(3) Å, Z – 16) with d(Zr? Zr) = 3,199–3.214(4) Å. Apparent residual electron density is found in the center of both clusters, amounting to Z～7.6 (Sc) and ～6 (Zr) based of refinement of oxygen in these positions. The effect is thought to probably arise from errors in the diffraction data rather than partial incorporation of light nonmetal atoms such as oxygen or fluorine. Observed metal-metal distances are compared with those in other clusters.     

Drei Wege zur Oxydation von [Ta6Cl12]2+ ([Ta6Br12]2+ und [Nb6Cl12]2+)

Three Oxidation Paths of [Ta₆Cl₁₂]²⁺ ([Ta₆Br₁₂]²⁺ and [Nb₆Cl₁₂]²⁺) [Ta₆Cl₁₂]²⁺ is oxidized autocatalytically to [Ta₆Cl₁₂]⁴⁺ by HNO₃. The titration of [Ta₆Cl₁₂]²⁺ with KBrO₃ (in HBr-containing solutions) or with Ce⁴⁺ or K₂Cr₂O₇ (in HNO₃-containing solutions) leads to a clear [Ta₆Cl₁₂]³⁺ step. The further titration leads beside [Ta₆Cl₁₂]⁴⁺ to the formation of Ta₂O₅(· xH₂O). [Ta₆Cl₁₂]²⁺ behaves with KBrO₃(+ HBr) equally, but the formation of [Ta₂O₅](· xH₂O) is only small. [Nb₆Cl₁₂]²⁺ (22°C) titrated with Ce(ClO₄)₄ in 2n HClO₄ gives the first potential step nearby exact ([Nb₆Cl₁₂]³⁺) and at a very slow titration in a second step a precipitation of Nb₂O₅(· xH₂O) occurs, which adsorbed Ce⁴⁺ additionally. At ?15°C with Ce(ClO₄)₄ the first potential step was exactly at [Nb₆Cl₁₂]^2+→3+, while the second step needs a distinct additional consumption of titer. (Formation of [Nb₆Cl₁₂]⁴⁺ and beside it [Nb₂O₅](· xH₂O)). From the titration curves and sections of its normal progress in all cases we get the normal potentials 2+/3+ and 3+/4+ with an accuracy of ± 0.01 volt. In alkaline solution the complexes are oxidized with air-oxygen to [M₆X₁₂](OH)₆^2?, while the Br-containing complexes suffer hydrolysis afterwards.     

Synthesen,Eigenschaften und Kristallstrukturen der Cluster‐Salze Bi6[PtBi6Cl12] und Bi2/3[PtBi6Cl12]

Syntheses, Properties and Crystal Structures of the Cluster Salts Bi₆[PtBi₆Cl₁₂] and Bi_2/3[PtBi₆Cl₁₂] Melting reactions of Bi with Pt and BiCl₃ yield shiny black, air insensitive crystals of the subchlorides Bi₆[PtBi₆Cl₁₂] and Bi_2/3[PtBi₆Cl₁₂]. Despite the substantial difference in the bismuth content the two compounds have almost the same pseudo‐cubic unit cell and follow the structural principle of a CsCl type cluster salt. Bi₆[PtBi₆Cl₁₂] consists of cuboctahedral [PtBi₆Cl₁₂]^2? clusters and Bi₆²⁺ polycations (a = 9.052(2) Å, α = 89.88(2)°, space group P 1, multiple twins). In the electron precise cluster anion, the Pt atom (18 electron count) centers an octahedron of Bi atoms whose edges are bridged by chlorine atoms. The Bi₆²⁺ cation, a nido cluster with 16 skeletal electrons, has the shape of a distorted octahedron with an opened edge. In Bi_2/3[PtBi₆Cl₁₂] the anion charge is compensated by weakly coordinating Bi³⁺ cations which are distributed statistically over two crystallographic positions (a = 9.048(2) Å, α = 90.44(3)°, space group ). Bi₆[PtBi₆Cl₁₂] is a semiconductor with a band gap of about 0.1 eV. The compound is diamagnetic at room temperature though a small paramagnetic contribution appears towards lower temperature.     

Zur Kenntnis von Ba6Ru2PtO12Cl2

About Ba₆Ru₂PtO₁₂Cl₂ Single crystals of Ba₆Ru₂PtO₁₂Cl₁₂ were prepared by a BaCl₂ flux and investigated by X-ray methods (D? P3 M1; a = 5,805; c = 15.006 Å; Z = 1). The characteristic face shared M₃O₁₂-octahedratriples show an ordered (Ru/Pt/Ru) occupation. Calculation of the Coulomb term of lattice energy support the charge distribution (5⁺/4⁺/5⁺) ions engage three point sites with different coordinations. The connection to other compounds are discussed.     

Synthesis and Structure of the Ordered Modification of Ba6EuF12Cl2

Crystals of ordered Ba₆EuF₁₂Cl₂ were found to form during high temperature flux growth. The structure was refined in the hexagonal space group P 6 to R^F(R ) = 0.024(0.024) for 326 reflections and 46 parameters. Lattice parameters are a = b = 1059.27(8) pm and c = 416.36(2) pm; Z = 1. The structure is isotypic to Ba₇F₁₂Cl₂. No solid solution of Ba/Eu was observed, the Eu²⁺ ions are located in the channels formed by 3 + 6 fluorine ions, occupying only one of the three metal sites of the Ba₇F₁₂Cl₂ structure.     

Isolation of Reduced Zirconium Chloride Clusters [(Zr6CCl12)Cl6]4− and [(Zr6BCl12)Cl6]5− from Acidic Aqueous Solution

Crystallizable from concentrated hydrochloric acid : Compounds containing [(Zr₆BCl₁₂)Cl₆]⁵⁻ and [(Zr₆CCl₁₂)Cl₆]⁴⁻ clusters survive dissolution in deoxygenated water, and this enabled the study of reduced zirconium compounds in aqueous solution for the first time. In the solid state, the clusters are surrounded by novel hydrogen-bonded water networks that interact with the terminal chloride ligands (see graphic; black circles: Zr, smaller circle: B, gray circles: Cl, open circles: O of H₂O).     

Der Ligandenaustausch im Kristallgitter von (PyH)2[Ta6Br12]Cl6

Ligand Replacement in the Crystal Lattice of (PyH)₂[Ta₆Br₁₂]Cl₆ Solid (PyH)₂[Ta₆Br₁₂ⁱ]Cl₆^a transforms exothermically at 210°C. In this way the Cl^a atoms outside of the complex are going instead of Brⁱ into the inside position; e.g. [Ta₆Br₁₂]Cl₆^2? → [Ta₆Br₆Cl₆]Br₆^2?. After each transformation Cl is brought in the outside position of the complex by recrystallization from a solution containing HCl. One gets in the following transformation step [Ta₆Br₃Cl₉]⁴⁺ and finally in the third step [Ta₆Br_1.5Cl_10.5]⁴⁺. Both formula are empirical formula. They consist of [Ta₆Br₆Cl₆]⁴⁺ and [Ta₆Br₂Cl₁₀]⁴⁺; and [Ta₆Br₆Cl₆]⁴⁺, [Ta₆Br₂Cl₁₀]⁴⁺ and [Ta₆Cl₁₂]⁴⁺, respectively. This result is in agreement with the theory.     

Observation of quadrupole hyperfine structure in the v6 RQ3 (6) transition of 12CH335Cl

Quadrupole hyperfine structure has been observed in the v₆^RQ₃(6) transition of ¹²CH₃³⁵Cl using a stable CO₂ laser oscillating on the 9.4 μm P(26) line. By heterodyning this laser with another which is locked to the 4.3 μm fluorescence dip of the 00⁰1-00⁰ CO₂ transition, an accurate measurement of the hyperfine splittings has been made. The observed spectrum agrees, within experimental error, to the theoretical values evaluated without the need for a vibrational correction to the quadrupole interaction in the excited vibrational state. The hyperfine component closest to the center of the CO₂ P(26) transition is determined to be 5.6 ± 0.1 MHz from the P(26) line center.