Kristallstruktur von Cu10Sn3(m)

Zusammenfassung Cu₁₀Sn₃(m) hat eine hexagonale Struktur, die in enger Verwandtschaft zur Struktur des CuZn steht. Einer der Hauptunterschiede beider Strukturen ist eine Stapelvariation der Schichten parallel (111)_CuZn. Aus dieser folgen weitere Verschiebungen der Atome, so daß die Struktur auch als Variante der NiAs-Struktur beschrieben werden kann. Gründe für die Stapelvariation lassen sich aus Annahmen über die Ortskorrelation der Elektronen herleiten.

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Crystal structure of Cu₁₀Sn₃(m)

Cu₁₀Sn₃(m) has a hexagonal structure, which is closely related to the structure of Cuzn. One of the main differences of these structures is a stacking variation of the layers parallel (111)_CuZn, which implies further shifts of atoms so that the structure may also be described as a variant of the NiAs structure. Causes for the stacking variation may be derived from assumptions on the spatial correlation of the electrons.

     

The [Sn(9)Pt(2)(PPh(3))](2)(-) and [Sn(9)Ni(2)(CO)](3)(-) complexes: two markedly different Sn(9)M(2)L transition metal zintl ion clusters and their dynamic behavior

[Sn(9)Pt(2)(PPh(3))](2)(-) (2) was prepared from Pt(PPh(3))(4), K(4)Sn(9), and 2,2,2-cryptand in en/toluene solvent mixtures. The [K(2,2,2-cryptand)](+) salt is very air and moisture sensitive and has been characterized by ESI-MS, variable-temperature (119)Sn, (31)P, and (195)Pt NMR and single-crystal X-ray diffraction studies. The structure of 2 comprises an elongated tricapped Sn(9) trigonal prism with a capping PtPPh(3), an interstitial Pt atom, a hypercloso electron count (10 vertex, 20 electron) and C(3)(v)() point symmetry. Hydrogenation trapping experiments and deuterium labeling studies showed that the formation of 2 involves a double C-H activation of solvent molecules (en or DMSO) with the elimination of H(2) gas. The ESI-MS analysis of 2 showed the K[Sn(9)Pt(2)(PPh(3))](1)(-) parent ion, an oxidized [Sn(9)Pt(2)(PPh(3))](1)(-) ion, and the protonated binary cluster anion [HSn(9)Pt(2)](1)(-). 2 is highly fluxional in solution giving rise to a single time-averaged (119)Sn NMR signal for all nine Sn atoms but the Pt atoms remain distinct. The exchange is intramolecular and is consistent with a rigid, linear Pt-Pt-PPh(3) rod embedded in a liquidlike Sn(9) matrix. [Sn(9)Ni(2)(CO)](3)(-) (3) was prepared from Ni(CO)(2)(PPh(3))(2), K(4)Sn(9), and 2,2,2-cryptand in en/toluene solvent mixtures. The [K(2,2,2-cryptand)](+) salt is very air and moisture sensitive, is paramagnetic, and has been characterized by ESI-MS, EPR, and single-crystal X-ray diffraction. Complex 3 is a 10-vertex 21-electron polyhedron, a slightly distorted closo-Sn(9)Ni cluster with an additional interstitial Ni atom and overall C(4)(v)() point symmetry. The EPR spectrum showed a five-line pattern due to 4.8-G hyperfine interactions involving all nine tin atoms. The ESI-MS analysis showed weak signals for the potassium complex [K(2)Sn(9)Ni(2)(CO)](1-) and the ligand-free binary ions [K(2)Sn(9)Ni(2)](1)(-), [KSn(9)Ni(2)](1)(-), and [HSn(9)Ni(2)](1)(-).     

Similar K@Au10Sn10 polyhedra in the markedly different structures of KAu4Sn6 and KAu3Sn3. syntheses and characterization

These compounds were synthesized by high-temperature reactions of the elements in welded Ta tubes and characterized by X-ray diffraction methods and linear muffin-tin orbital (LMTO) calculations. AAu4Sn6 (A = K, Rb) have a new structural type (Fddd, Z = 8), and KAu3Sn3 (Pmmn, Z = 2) is isostructural with SrAu3In3. Both orthorhombic structures contain similar condensed K@Au10Sn10 polyhedral building blocks, which can be described as overall 6-8-6 arrangements of planar rings or, alternatively, as hexagonal prisms centered by K and augmented about the waists by 8-rings of Au and Sn. However, the 3D Au-Sn networks differ appreciably in both composition and the modes of condensation. In KAu3Sn3, the prisms stack by sharing both hexagonal faces with like neighbors along a, whereas those in KAu4Sn6 condense in a complex zigzag network. Compared with related indium systems, the structure change from KAu4In6 ( P_6m2, Z = 1) to KAu4Sn6 apparently illustrates the effect of complex factors such as atom size and valence electron counts on structure, whereas the SrAu3In3 and KAu3Sn3 pair are isotypic. Both compounds are Pauli-paramagnetic and inert to water at room temperature for several days. Tight-binding electronic structure (LMTO) calculations emphasize the dominance and strength of the heteroatomic Au-Sn bonding.     

Structure and vibrations of BenOn (n=3-10) clusters

The structure and harmonic vibrations of Be(n)O(n) (n=3-10) clusters have been investigated using density functional theory. All structures are found to be cumulenic D(nh) rings (equal bonds, alternating angles), with one intense out of plane mode and three infrared-active degenerate modes, of which the highest one is extremely intense and asymptotically increases to 1597 cm(-1) for n=10. Comparisons with C(2n) clusters and B(n)N(n) clusters, the structure and bonding type for the Be(n)O(n) clusters are consistent with those of the C(2n) (n=3, 5, 7, ...) clusters and the B(n)N(n) clusters.     

A model for binding of inhalation anesthetics to membranes: two dose-dependent distinctly different binding modes

Inhalation anesthetics currently in clinical use, such as halothane, methoxyflurane, enflurane, isoflurane, etc., are polar hydrophobic molecules, except nitrous oxide, which is an apolar and weak anesthetic, incapable of inducing surgical stage anesthesia. Experimental data are accumulating that these potent amphipathic inhalation anesthetics preferentially bind membranes and macromolecules on the surface at clinical concentrations. The anesthetic binding to lipid membranes in the low concentration range is characterized by a saturable curve approaching to a limiting value. When the anesthetic concentration s greatly increased above the clinical range, the binding starts to exceed the limiting saturation value. Our model for anesthetic binding to membranes consists of two parts: Langmuir-type adsorption to the membrane surface at the low concentration range and penetration into the hydrophobic core at the high concentration range. The present communication provides a statistical-thermodynamic basis to analyze this twostep interaction. An expression is derived for membrane capacitance as a function of anesthetic concentration, which explains the experimental data well. Binding parameters of anesthetics are estimated according to the theory.This study was supported by NIH grants GM 25716 and GM 26950, and by the Medical Research Service of the Veterans Administration.     

Synthesis of palladium-tin carbonylphosphine clusters and X-ray study of the Pd3Sn2(acac)4(CO)2(PPh3)3 cluster

It has been shown for the first time that the reaction of bi-valent tin acetyl-acetonate with palladium carbonylphosphine clusters, Pd₄(CO)₅(PPh₃)₄ (I), Pd₄(CO)₅(PEt₃)₄ (II) and Pd₃(CO)₃(PPh₃)₄ (III), results in the formation of heterometal pentanuclear clusters of general formula Pd₃Sn₂(acac)₄(CO)₂(PR₃)₃; R  Ph (IV), Et (V). X-ray analysis of Pd₃Sn₂(acac)₄(CO)₂(PPh₃)₃ at 20°C (λ(Mo), 4396 reflections, space group P2₁/n, Z = 4, R = 0.037) shows that IV in the form of the crystalline hydrate, Pd₃Sn₂(acac)₄(CO)₂(PPh₃)₃ · χH₂O (χ ∼ 1), contains a distorted “propeller”-shaped Pd₃Sn₂ metal frame with PdSn distances of 2.679–2.721(1) Å; two short PdPd bonds, 2.708 and 2.720(1) Å, bridged by μ₂-CO ligands, and an elongated central Pd(1)Pd(2) bond of 2.798 Å. Sn atoms have distorted octahedral coordination, the dihedral angles formed by Pd₃ moieties and two Pd₂Sn triangles are 127.6 and 106.5°; and the angle between Pd₂Sn moieties is 126.0°.     

Darstellung und Kristallstrukturanalyse von Cl10Sn4(NCNSiMe3)6

Preparation and X-ray Structure Determination of Cl₁₀Sn₄(NCNSiMe₃)₆ Tin tetrachloride and Me₃Si? N?C?N? SiMe₃ (Me = CH₃) forms the thermally not very stable carbodiimide derivative Cl₁₀Sn₄(NCNSiMe₃)₆, which has been characterized by spectroscopic methods (IR, Raman, ¹H-NMR). The X-ray structure determination shows the orthorhombicspace group Pnnm with two [Cl₁₀Sn₄(NCNSiMe₃)₆ · C₇H₈] units per cell. The centrosymmetric Sn₄N₆-skeleton of the carbodiimide molecule has a well known “open-cage” form, the structure was refined to an R-value of 0.038.     

Pyridine-incorporated cyclo[6]aramide for recognition of urea and its derivatives with two different binding modes

Abstract

A novel pyridine-incorporated cyclo[6]aramide is designed and synthesised for recognition of urea and its derivatives. Analysis of its single crystal structure reveals the presence of introverted amide NH protons and amide carbonyl groups that are supposed to contribute to the subsequent accommodation of neutral urea-related guest molecules via multiple hydrogen bonding interactions. Thiourea is found to be superior to urea in binding to the receptor. Particularly interesting is the observation of two binding modes in complexing urea/thiourea (contact mode) and ethylurea/diethylurea (threading mode) as supported by both NMR experiments and computational simulations. The finding of the threading mode may open up new opportunities for the development of pesudorotaxanes and related mechanically interlocked structures.     

Structure and vibrations of Ga(n)N(n) (n = 3-10) clusters

The structure and harmonic vibrations of Ga(n)N(n) (n = 3-10) clusters have been investigated using the B3LYP (Becke 3-parameter-Lee-Yang-Parr) density functional theory. All structures are found to be cumulenic D(nh) rings (equal bonds, alternating angles), with one intense out of plane mode and three infrared-active degenerate modes, of which the highest one is extremely intense and asymptotically increases to 1029 cm(-1) for n = 10. Comparisons with C2n, B(n)N(n), and Al(n)N(n) clusters, the structure and bonding type for the Ga(n)N(n) (n=3-10) clusters are consistent with those of the C2n (n = 3, 5, 7, ...) clusters, the B(n)N(n) (n = 3-10), and Al(n)N(n) (n = 3-9) clusters.     

Synthesis and characterization of the largest isolated clusters of tin, [Sn12](12-), in (AE)Na10Sn12 (AE = Ca or Sr)

Reported are two isostructural Zintl compounds, CaNa(10)Sn(12) and SrNa(10)Sn(12), with mixed alkali and alkaline-earth cations and isolated clusters of Sn(12)(12-) with the shape of giant truncated tetrahedra. The compounds were synthesized by heating the corresponding mixtures of elements at 950 degrees C. The structures were solved and refined from single-crystal X-ray diffraction data in the cubic space group I43m (No. 217), where Z = 2 with a = 11.1847(6) and 11.2176(4) A for CaNa(10)Sn(12) and SrNa(10)Sn(12), respectively. Both compounds are diamagnetic and therefore electronically balanced.     

A three‐dimensional tin(II) phosphonatobenzenesulfonate with Sn4O12 clusters

The hydrothermal reaction of SnCl₂·2H₂O with 4‐phosphonobenzenesulfonic acid (H₃L) and sodium hydroxide has yielded the title compound, poly[μ‐hydroxido‐μ₇‐(4‐phosphonatobenzenesulfonato)‐ditin(II)], [Sn₂(C₆H₄O₆PS)(OH)]_n. The inorganic building unit is an Sn₄O₁₂ cluster which is composed of edge‐sharing SnO₄ and SnO₅ polyhedra. The clusters are interconnected via P and S atoms from the organic acid to form layers in the ab plane. These layers are linked to each other through pillaring benzene groups parallel to the c axis to form a three‐dimensional structure.     

Der chemische Transport von Ni3Ge,Ni5Ge3, Ni(Ge)-Mischkristall,CoSn, Co3Sn2, Cu41Sn11 (δ-Phase), Cu10Sn3 (ζ-Phase) und Cu(Sn)-Mischkristall

Chemical Vapour Transport of Intermetallic Systems. 7. Chemical Transport of Ni₃Ge, Ni₅Ge₃, Ni(Ge)-mixed Crystal, CoSn, Co₃Sn₂, Cu₄₁Sn₁₁ (δ-phase), Cu₁₀Sn₃ (ζ-phase), and Cu(Sn)-mixed Crystals By means of GaI₃ as transport agent some intermetallics in the Ni/Ge- and Co/Sn-system can be prepared by CVT-methods. Using Iodine Cu–Sn-compounds can be deposited in a similiar way.     

Dissociation of energy selected Sn(CH3)4(+), Sn(CH3)3Cl+, and Sn(CH3)3Br+ ions: evidence for isolated excited state dynamics

The dissociation dynamics of Sn(CH(3))(4)(+), Sn(CH(3))(3)Cl(+), and Sn(CH(3))(3)Br(+) were investigated by threshold photoelectron photoion spectrometry using an electron imaging apparatus (iPEPICO) at the Swiss Light Source. The tetramethyltin ion was found to dissociate via Sn(CH(3))(4)(+) → Sn(CH(3))(3)(+) + CH(3) → Sn(CH(3))(2)(+) + 2CH(3), while the trimethyltin halide ions dissociated via methyl loss at low energies, and a competitive halogen loss at somewhat higher energies. The 0 K methyl loss onset for the three ions was found to be 9.410 ± 0.020 eV, 10.058 ± 0.020 eV, and 9.961 ± 0.020 eV, respectively. Statistical theory could not reproduce the observed onsets for the halogen loss steps in the halotrimethyltin ions. The halide loss signal as a function energy mimicked the excited state threshold photoelectron spectrum, from which we conclude that the halide loss from these ions takes place on an isolated excited state potential energy surface, which we describe by time dependent density functional calculations. The sequential loss of a second methyl group in the Sn(CH(3))(4)(+) ion, observed at about 3 eV higher energies than the first one, is also partially non-statistical. The derived product energy distribution resulting from the loss of the first methyl group is two-component with about 50% being statistical and the remainder associated with high translational energy products that peak at 2 eV. Time dependent DFT calculations show that a dissociative ?B state lies in the vicinity of the experimental measurements. We thus propose that 50% of the Sn(CH(3))(4)(+) ions produced in this energy range internally convert to the ?X state, on which they dissociate statistically, while the remainder dissociate directly from the repulsive ?B state leading to high kinetic energy products.     

Bridging versus chelating diphosphine in clusters: Isomers of Os3(CO)10(diphosphine)

Isomers of Os₃(CO)₁₀(diphosphine) (diphosphine = Ph₂P(CH₂)_nPPh₂; n = 2 (dppe), n = 3 (dppp), and n = 4 (dppb)) have been prepared in which the diphosphine is chelating (1,1-isomer) or bridging (1,2-isomer), respectively, by displacing butadiene or acetonitrile from the complexes Os₃(CO)₁₀(cis- or trans-C₄H₆) or Os₃(CO)₁₀(MeCN)₂. Ph₂PCH₂PPh₂ (dppm) gives only the known bridging (1,2-isomer) whichever starting material is used. Structures have been established by infrared, ³¹P and ¹³C NMR methods.     

Microscopic modes and free energies of 3-phosphoinositide-dependent kinase-1 (PDK1) binding with celecoxib and other inhibitors

Celecoxib, also known as Celebrex (approved by FDA in 1998) and remembered as the fastest-selling drug in history, was used as a cyclooxygenase-2 (COX-2) selective inhibitor having both anti-inflammatory and anticancer activities. Most recent studies have revealed that the apoptotic activity of celecoxib (and its derivatives) is actually independent of the COX-2 inhibitory activity and that celecoxib also inhibits the kinase activity of 3-phosphoinositide-dependent protein kinase-1 (PDK1), suggesting that the well-known anticancer activity of celecoxib is not due to the inhibition of COX-2, but possibly is due to the inhibition of PDK1. It is highly desirable to develop new celecoxib derivatives as PDK1-specifc inhibitors to avoid the side effects of COX-2 inhibitors. To understand how PDK1 binds with celecoxib and its derivatives, we have performed extensive molecular docking and combined molecular dynamics (MD) simulations and molecular mechanics/Poisson-Boltzmann surface area (MM-PBSA) binding free energy calculations on eight representative PDK1 inhibitors, leading to the finding of a new, more favorable binding mode which is remarkably different from the previously proposed binding mode. Based on the determined most stable binding structures, the calculated binding free energies are all in good agreement with the corresponding experimental data, and the biological activity data available for celecoxib and its derivatives can be better interpreted. The obtained new insights, concerning both the binding mode and computational protocol, will be valuable not only for future rational design of novel, more potent PDK1-specific inhibitors as promising anticancer therapeutics, but also for rational design of drugs targeting other proteins.     

Bonding modes of stanna-closo-dodecaborate: eta1(Sn) to eta3(BH) rearrangement reactions in zwitterionic stanna-closo-dodecaborate ruthenium complexes

Reaction of the stanna-closo-dodecaborate salt [Bu3MeN]2[SnB11H11] with the dimeric ruthenium complex [Ru2(mu-Cl)3(triphos)2]Cl (triphos = {MeC(CH2PPh2)3}) in refluxing acetonitrile yields the zwitterionic compound [Ru(SnB11H11)(MeCN)2(triphos)] (4) which has been characterized by single-crystal X-ray diffraction analysis and solid-state NMR spectroscopy. Refluxing the zwitterion in acetone leads to an eta1(Sn) to eta3(BH) rearrangement with formation of [Ru(SnB1)H11)(triphos)] (5) whose structure has been confirmed by X-ray diffraction and multinuclear NMR spectroscopy in solution and in the solid state. Furthermore, two isomeric zwitterions fac- and mer-[Ru(SnB11H11)(dppb)(MeCN)3] (6a, 6b) and their rearrangement reactions as well as their NMR properties are described.     

Incremental binding energies of gold(I) and silver(I) thiolate clusters

Density functional theory is used to find incremental fragmentation energy, overall dissociation energy, and average monomer fragmentation energy of cyclic gold(I) thiolate clusters and anionic chain structures of gold(I) and silver(I) thiolate clusters as a measure of the relative stability of these systems. Two different functionals, BP86 and PBE, and two different basis sets, TZP and QZ4P, are employed. Anionic chains are examined with various residue groups including hydrogen, methyl, and phenyl. Hydrogen and methyl are shown to have approximately the same binding energy, which is higher than phenyl. Gold-thiolate clusters are bound more strongly than corresponding silver clusters. Lastly, binding energies are also calculated for pure Au(25)(SR)(18)(-), Ag(25)(SR)(18)(-), and mixed Au(13)(Ag(2)(SH)(3))(6)(-) and Ag(13)(Au(2)(SH)(3))(6)(-) nanoparticles.