Perfluormethyl-Element-Liganden. IX.. Synthese und Eigenschaften von (CF3)2EMn(CO)5 (E = P,As)

Preparation and Properties of (CF₃)₂EMn(CO)₅ (E ? P, As) The complexes (CF₃)₂EMn(CO)₅ (E ? P, As) are formed by the reaction of E₂(CF₃)₄ with HMn(CO)₅. They can be converted quantitatively to the binuclear compounds [Mn(CO)₄E(CF₃)₂]₂ in a thermal (E ? P) or photochemical (E ? P, As) process. u. v. irradiation of a 1:1 mixture gives the mixed derivative Mn₂(CO)₈As(CF₃)₂P(CF₃)₂ together with the symmetrical systems. The Mn? E bond is less reactive with HBr and Me₃SnBr than the M? E bond in derivatives of the type Me₃ME(CF₃)₂ (M ? Si, Ge, Sn; Me ? CH₃). The terminal (CF₃)₂E groups are found to be strong π-acceptor ligands.     

Die Molekül- und Kristallstrukturen von (CO)4 W(μ-S-t-C4H9)2W(CO)4, η7-C7H7W(μ-SC6H4CH3)3W(CO)3 und η7-C7H7W(μ-S-n-C4H9)3W(CO)(μ-S-n-C4H9)2W(CO)4

Molecular and Crystal Structures of (CO)₄W(μ-S-t-C₄H₉)₂W(CO)₄, η⁷-C₇H₇W(μ-SC₆H₄CH₃)₃W(CO)₃ and η⁷-C₇H₇W(μ-S-n-C₄H₉)₃W(CO)(μ-S-n-C₄H₉)₂W(CO)₄ The molecular structures of the two binuclear complexes (CO)₄W(μ-S-t-C₄H₉)₂W(CO)₄ and η⁷-C₇H₇W(μ-SC₆H₄CH₃)₃W(CO)₃ and of the tungsten cluster η⁷-C₇H₇W(μ-S-n-C₄H₉)₃W(CO)-(μ-S-n-C₄H₉)₂W(CO)₄ respectively are described. In the nonlinear trinuclear cluster the central tungsten atom is connected to the two tungsten atoms by two and three μ-S-n-C₄H₉ bridges respectively and additionally by one W? W bond each. The coordination sphere of the W atoms is completed by a η⁷-C₇H₇ ring and four CO groups respectively; the central tungsten carries an additional CO group.     

Decarbonation curves and associated thermodynamic data for synthetic Cd-dolomites CdMg(CO3)2, CdMn(CO3)2 and CdZn(CO3)2

Decarbonation curve for the synthetic dolomite analogues; (Cd-dolomites) were determined for CdMg(CO₃)₂, CdMn(CO₃)₂ and CdZn(CO₃)₂ under CO₂ pressure of up to 2.5 kbar. All the three double carbonates were completely disordered at the decomposition temperatures and hence the thermodynamic data (Standard enthalpy; ΔH _f ^o, Standard free energy; ΔG _f ^o) retrieved from the univariant decarbonation curve corresponds to the disordered phases. They are: The mixing enthalpies and free energies for the formation of the disordered 1∶1 solid solution phases are: The thermodynamic data (ΔH _f ^o, ΔG _f ^o and ΔH _r ^o, ΔG _r ^o) showed a positive correlation with the decomposition temperatures. The mixing energies of the disordered double carbonates also show a direct correlation with the cationic size differences.     

Design and Syntheses of Three Novel Carbonate Halides: Cs3Pb2(CO3)3I,KBa2(CO3)2F,and RbBa2(CO3)2F

Three new carbonate halides, Cs₃Pb₂(CO₃)₃I, KBa₂(CO₃)₂F and RbBa₂(CO₃)₂F have been synthesized with hydrothermal and solid‐state methods. Cs₃Pb₂(CO₃)₃I is the first product in the lead carbonate iodides family; KBa₂(CO₃)₂F and RbBa₂(CO₃)₂F are the first two centrosymmetric compounds found in the alkaline–alkaline earth carbonate fluorides family. Cs₃Pb₂(CO₃)₃I crystallizes in a centrosymmetric space group C2/m, and exhibits a two‐ dimensional layered structure which is formed by [Cs₄Pb₄(CO₃)₆I₂]_∞ double‐layers consisting of [Pb₂(CO₃)₃I]_∞ single‐layers bridged by the Cs atoms. KBa₂(CO₃)₂F and RbBa₂(CO₃)₂F, which are isostructural, crystallize in a trigonal crystal system with a centric space group of R featuring a honeycomb‐like framework. First principle calculations indicate that Cs₃Pb₂(CO₃)₃I has a moderate birefringence and explain the difference between the band gaps of the title compounds from electron structures. The effects of cations and halogens on the structures and properties of the title compounds are also discussed.     

Synthesis of (CH3C(CH2PPh2)3)CoL complexes (L = O2CO,S2CO,O2SO) through metal-assisted CO2, CS2, SO2 oxidation. Crystal structure of (CH3C(CH2PPh2)3)CO(O2SO)

The solution obtained by reduction of [(triphos)CO(μ-Cl)₂Co(triphos)]⁺² (triphos = CH₃C(CH₂PPh₂)₃) with Na/Hg reacts with CO₂, CS₂ and SO₂ to give (triphos)Co(O₂CO), (triphos)Co(S₂CO), and (triphos)Co(O₂SO), respectively. The molecular structure of the last has been established by X-ray difraction.     

Mineral formation from aqueous solution. Part III. The stability of aurichalcite, (Zn,Cu)5(CO3)2(OH)6, and rosasite (Cu,Zn)2(CO3)(OH)2

Summary The stabilities of rosasite, (Cu, Zn)₂ (CO₃)(OH)₂, and aurichalcite, (Zn, Cu)₅(CO₃)₂(OH)₆, have been determined by solution experiments with computer calculations of aqueous species in equilibrium with the solid phases. G _f ^o values for rosasite and aurichalcite have been calculated as –1100 and –2766 kJ mol^–1 respectively for specific samples of the two minerals. Most of the difference between the free energies of the compounds and those of malachite, Cu₂(CO₃)(OH)₂, and hydrozincite, Zn₅(CO₃)₂(OH)₆ arises from substitution of the minor cation in the crystal lattice. Malachite, zincian malachite and rosasite should be considered as a single isomorphous series.Part II: A. K. Alwan and P. A. Williams,Transition Acct. Chem., 4, 319 (1979).     

Synthesis,structures and reactivities of poly(pyrazol-1-yl) alkane tetracarbonylmolybdenum (tungsten):x-ray crystal structures of (CH2)2(3,5-Me2Pz)2W(CO)4 and CH2(3,5-Me2Pz)2W(Cl)(CO)3(SnCl3)(Pz:pyrazolyl)

Since S. Trofimenko introduced these isosteric and isoelectronic ligands with poly(1-pyrazolyl)borates^[1],the poly (pyrazolyl)alkane ligands have attracted much attention. Their coordinating behaviour with transition and main group metals has been extensively investigated in recent years^[2]. The coordinating behaviour of bis(3,5-dimethylpyrazol-1-yl)ethane is often different from other poly(pyrazolyl) alkanes^[3]. The VIB metals carbonyl complexes bonded with poly (pyrazolyl)alkanes have novel structures and unusual reactivities^[4,5,6],which encourages us to investigate M-Sn bimetallic complexes with poly(pyrazolyl)alkanes. In this paper, we report the synthesis, characterization and reactivities of poly (pyrazol-1-yl)alkane tetracarbonylmolybdenum (tungsten) with R'SnCl₃(R'=Ph,Cl).     

Adsorption of CO and O2 on W2C(0001)

CO, O(2), and H(2) adsorption on a clean W(2)C(0001)√13×√13 R ± 13.9° reconstructed surface at room temperature (RT) were investigated using high-resolution electron energy loss spectroscopy (HREELS). The W(2)C(0001) adsorbs CO molecularly and adsorbs O(2) dissociatively, but does not adsorb H(2) at RT. In the CO adsorption system, two C-O stretching (antisymmetric CCO stretching) modes were found at 242.3 meV (1954 cm(-1)) and at 253.0 meV (2041 cm(-1)). The low-frequency site is occupied at first with subsequent conversion to the high-frequency site with increasing coverage. Additionally, a small peak was apparent at 104.5 meV (843 cm(-1)), and a middle peak at 50-51 meV (400-410 cm(-1)), which are assignable to a symmetric stretching mode and a hindered translational mode, respectively, of a CCO (ketenylidene) species. These observations are consistent with the CO adsorption model on top of the surface carbon. For oxygen adsorption, two adsorption states were found at 65.2-68.1 meV (526-549 cm(-1)) and 73.6 meV (594 cm(-1)): typical frequencies to oxygen adsorption on metal surfaces. Results suggest that atomic oxygen adsorption occurred on a threefold hollow site of the second W layer.