Structural and electronic effects involving pyridine rings in 4-methylpyridine Cu4OX6L4 complexes. I. Vibrational spectra of Cu4OBr n Cl(6−n)(4-Mepy)4 complexes

Gaussian analysis of bands between 500 cm⁻¹ and 600 cm⁻¹ attributed to the _as (Cu₄O) stretching vibration of the tetrahedral Cu₄O core in Cu₄OBr _n Cl_(6−n)(4-Mepy)₄ (n = 0–6) complexes showed two bands, symmetry reduction of the T ₂ mode of vibration towards the A ₁ and E modes and vibrational coupling with an R-sensitive in-plane pyridine ring bending. The Cu-O bond is considered as vibrationally coupled with the Cu-N bond and the pyridine ring through the donor-acceptor vibrational coupling and the corresponding equilibrium charge distribution. The linear correlation between _as(Cu₄O) and the number of bromides in Cu₄OBr _n Cl_(6−n)(4-Mepy)₄ complexes was used for the estimation of partial charges on the 4-Mepy ligands which were positive for the prevailing donors and negative for the prevailing acceptors thus evoking a π-back bonding between the Cu(II) atoms and the 4-Mepy ligands. Correlations involving selected bond lengths and bond angles in the molecular structure of the Cu₄OCl₆(4-Mepy)₄ complex with four symmetrically independent molecules present in the unit cell indicate a symmetry reduction of the T ₂ mode of vibration and the π-back bonding between the Cu(II) atoms and the 4-Mepy ligands.     

Synthesis and Re—refinement of Cu3PSe4

1 INTRODUCTION The chemistry of mixed 15/16 main group compounds has attracted great attentions over the last years[1]. The metal chalcogenophosphides synthesized by solid state reactions[2] are the potential candidates for a wide range of applications such as semiconducting properties, two-dimensional magnetic behavior, anisotropy of conductivity and charge density waves. Some of these compounds are of lamellar structure, which are good materials for the investigation of intercalatio…     

SYNTHESIS AND CRYSTAL STRUCTURE OF MoS4Cu4I2（Py）6

<正> C30H30Cu4I2S4MoN6,Mr=1206, orthorhombic, Fdd2, a = 22. 511(4), b= 22.946(4), c=30. 742(6)(?), Z = 16, Dc = 2. 019g/cm3, V = 15879.4 (?)3, μ = 41. 884cm-1, F (000) = 9280. The final R factor is 0. 0279 for 1884 observed reflections with I>3σ(I). Crystal structure analysis shows that the MoS4Cu4 aggregate is formed, each the four copper atoms is linked with two S atoms of the te-trahedral MoS42- core. The average distance between Mo and Cu atoms is 2. 678(?).     

新法合成Cu6(C5H4NS)6簇合物及其性质

新法合成Cu6(C5H4NS)6簇合物及其性质;六核铜(Ⅰ)簇合物;水热合成;晶体结构;热稳定性;荧光     

New 1D and 2D metal oxygen connectivities in Cu(II) succinato and glutarato coordination polymers: [Cu3(H2O)2(OH)2(C4H4O4)2] · 4H2O, [Cu4(H2O)2(OH)4(C4H4O4)2] · 5H2O and [Cu5(OH)6(C5H6O4)2] · 4H2O

Two Cu(II) hydroxo succinates [Cu₃(H₂O)₂(OH)₂(C₄H₄O₄)₂]?·?4H₂O (1) and [Cu₄(H₂O)₂(OH)₄(C₄H₄O₄)₂]?·?5H₂O (2) and one Cu(II) hydroxo glutarate [Cu₅(OH)₆(C₅H₆O₄)₂]?·?4H₂O (3) have been prepared and structurally characterized by single crystal X-ray diffraction methods. They feature 1D and 2D copper oxygen connectivity of elongated {CuO₆} octahedra in “4?+?1?+?1” and “4?+?2” coordination geometries. Within 1, linear trimers of three edge-sharing {CuO₆} octahedra are connected into copper oxygen chains, which are bridged by the anti conformational succinate anions to generate 2D layers with mono terminally coordinating gauche succinate anions on both sides. The layers are assembled into a 3D framework by interlayer hydrogen bonds with lattice H₂O molecules distributed in channels. Different from 1, the principal building units in 2 are linear tetramers of four edge-sharing {CuO₆} octahedra. The tetramers are condensed into copper oxygen chains and the succinate anions interlink them into a 3D framework with triangular channels filled by lattice H₂O molecules. The {CuO₆} octahedra in 3 are edge-shared to form unprecedented 2D inorganic layers with mono terminally coordinating glutarate anions on both sides. Interlayer hydrogen bonding interactions are responsible for supramolecular assembly of the layers into a 3D framework with lattice H₂O molecules in the channels. The inorganic layers in 3 can be described as hexagonal close packing of oxygen atoms with the Cu atoms in the octahedral cavities. The title compounds were further characterized by elemental analyses, IR spectra and thermal analyses.     

Calix[4]dithiacrown-6 and Its Platinum Complex

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Tetramers Cu4(μ4-O)(η-X)6(L4): Analysis of structural data

This review summarizes structural parameters for forty five Cu₄(μ₄-O)(η-X)₆(L₄) tetramers. There are four types of structurally equal core units, CuCl₃ON, CuCl₃OO, CuCl₃OCl and CuBr₃ON. There are also tetramers which contain structurally unequal core units: CuCl₃ON (x2) and CuCl₂BrON (x2); CuCl₃ON (x1), CuCl₂BrON (x2) and CuCl₃OCl (x1). There is a tendency for an elongated Cu?Cu separation as well as Cu–L bond distances with increase of the covalent radius of the coordinating atom(s). Tetrahedral distortion around oxygen atom (OCu₄) increases in the order: 1.67° (CuCl₃OCl) < 2.10° (CuCl₃ON) < 2.11° (CuCl₃OO′) < 2.27° (CuBr₃ON). The mean Cu–Cl–Cu bridge angle of 80.5° is about 4.0° more open than that of a Cu–Br–Cu (76.5°). The cluster Cu₁₆O₄Br₇Cl₁₇(4-Mepy)₁₆ (4-Mepy = 4-methylpyridine) contains four crystallographically independent tetramers: Cu₄OBrCl₅(4-Mepy)₄ (1), Cu₄OBrCl₅(4-Mepy)₄ (2) Cu₄OBr₂Cl₄(4-Mepy)₄ (3) and Cu₄OBr₃Cl₃(4-Mepy)₄ (4), which is a unique example of stereoisomerism. There are other examples which exist in two isomeric forms. Another contains two or even four crystallographically independent tetramers within the same crystal, differing mostly by degree of distortion and is an examples of distortion isomerism. Pairs of Cu₄OCl₆(n-Meim)₄ (n-Meim = n-methylimidazole) (n = 1 or 2) are examples of ligand isomerism.     

A near-infrared and Raman spectroscopic study of the mineral richelsdorfite Ca2Cu5Sb[Cl|(OH)6|(AsO4)4]·6H2O

Raman spectroscopy has enabled insights into the molecular structure of the richelsdorfite Ca(2)Cu(5)Sb[Cl|(OH)(6)|(AsO(4))(4)]·6H(2)O. This mineral is based upon the incorporation of arsenate or phosphate with chloride anion into the structure and as a consequence the spectra reflect the bands attributable to these anions, namely arsenate or phosphate and chloride. The richelsdorfite Raman spectrum reflects the spectrum of the arsenate anion and consists of ν(1) at 849, ν(2) at 344 cm(-1), ν(3) at 835 and ν(4) at 546 and 498 cm(-1). A band at 268 cm(-1) is attributed to CuO stretching vibration. Low wavenumber bands at 185 and 144 cm(-1) may be assigned to CuCl TO/LO optic vibrations.     

The structure of the mineral leogangite Cu10(OH)6(SO4)(AsO4)4·8H2O--implications for arsenic accumulation and removal

The objective of this research is to determine the molecular structure of the mineral leogangite. The formation of the types of arsenosulphate minerals offers a mechanism for arsenate removal from soils and mine dumps. Raman and infrared spectroscopy have been used to characterise the mineral. Observed bands are assigned to the stretching and bending vibrations of (SO₄)²⁻ and (AsO₄)³⁻ units, stretching and bending vibrations of hydrogen bonded (OH)⁻ ions and Cu²⁺-(O,OH) units. The approximate range of O–H?O hydrogen bond lengths is inferred from the Raman spectra. Raman spectra of leogangite from different origins differ in that some spectra are more complex, where bands are sharp and the degenerate bands of (SO₄)²⁻ and (AsO₄)³⁻ are split and more intense. Lower wavenumbers of δ H₂O bending vibration in the spectrum may indicate the presence of weaker hydrogen bonds compared with those in different leogangite samples. The formation of leogangite offers a mechanism for the removal of arsenic from the environment.     

Detection of NO2 Based on 4-Carboxyl-4'-hydroxy Azobenzene and Its Cu(Ⅱ) Complex

<正>An organic ligand and its Cu(II) complex formulated as (C_(13)H_(10)N_2O_3)·5H_2O (H_2L·5H_2O, 1) and Cu(HL)_2(phen)·0.125H_2O (2, H2L = 4-carboxyl-4′-hydroxy azobenzene, phen = 1,10-phenanthroline) have been synthesized and structurally characterized by single-crystal X-ray diffraction. In the two compounds, H_2L and HL exhibit a trans-conformation. Complex 2 shows a mononuclear Cu(II) structure with the hydroxyl group of HL uncoordinated. Complex 2 is assembled into a three-dimensional (3D) supramolecular architecture by hydrogen bonds and π-π stacking interactions. H_2L and compound 2 can detect NO_2 via reversible and irreversible color changes, respectively. The mechanism for the color changes is investigated.     

Structural and electronic properties of γ-Tl2Cu(SO4)2

The compound Tl₂Cu(SO₄)₂, belonging to the dehydrated copper Tutton salts [Cat₂Cu(SO₄)₂, where Cat stands for cation], and especially its glassy γ-modification was investigated. The results of X-ray diffraction analysis, electron paramagnetic resonance, differential thermal analysis, electrical conductivity, and thermostimulated depolarization measurements are presented and discussed. An evident correlation among the results of various experimental techniques was found.     

A Solvothermal Route to Cu2O Nanocubes and Cu Nanoparticles

IntroductionSynthesis of Cu2O and Cu nanostructures has beenactively researched for many decades because bothCu2O and Cu are important industrial materials on ac-count of their novel physical and chemical properties.In particular,Cu2O is a p-type metal ox…     

BaLa4Cu5O13+δ, an oxygen-deficient perovskite built up from corner-sharing CuO6 octahedra and CuO5 pyramids

The structure of an oxygen-deficient perovskite BaLa₄Cu₅O_13+δ has been determined by neutron powder diffraction and high-resolution electron microscopy. It has been resolved in the space groupP4m(a ∼ a_p√5, c ∼ a_p). The framework [Cu₅O₁₃] is built up from corner-sharing CuO₅ pyramids and CuO₆ octahedra forming hexagonal tunnels and perovskite cages where the La³⁺ and Ba²⁺ ions are located in an ordered manner. The barium ions are located in the perovskite tunnels whereas the lanthanum ions are located in the hexagonal tunnels. One typical feature of the host lattice [Cu₅O₁₃] deals with the geometry of the hexagonal tunnels which is rather different from the ideal model derived from the stoichiometric perovskite. O-O-O angles are close to 70° (instead of 90°) and O(5)-O(5) distances are close to 3A˚(instead of 3.8A˚). A great number of crystals exhibit a single oxygen-deficient perovskite which can be considered as having the stoichiometry BaLa₄Cu₅O₁₃; the excess of oxygen, δ, corresponds to the formation in other crystals of superstructures (∼ a_p√10 × a_p√10 × a_p) and of microdomains which are interpreted as the result of a distortion of the [Cu₅O₁₃] matrix induced by the introduction of oxygen in half of the hexagonal tunnels.     

FTIR spectra of the 2ν4, ν4 + ν6 and 2ν6 bands of formaldehyde

High resolution IR spectra of the overtones and the combination band of the ν₄ and ν₆ modes of formaldehyde (2ν₄, ν₄ + ν₆ and 2ν₆) were measured in the region of 2200–2650 cm⁻¹ using FTIR. The combination band ν₄ + ν₆, whose dipole transition is forbidden from molecular symmetry, was observed due to the intensity borrowed from the other bands. The observed frequencies were analysed by a Hamiltonian in which A-type Coriolis interactions and Darling—Dennison interaction were taken into account. The ratio and the relative signs of the transition dipole moments of the overtone bands, μ_2ν4 and μ_2ν6, have been determined by analysing the intensity distribution of the vibration—rotation lines.     

Synthesis and structure of tetra-p-tolylantimony complexes [(4-MeC6H4)4Sb] 2 + [Hg2I6]2−, [(4-MeC6H4)4Sb] 2 + [HgI4]2−, [(4-MeC6H4)4Sb] 3 + [Sb3I12]2−, and [(4-MeC6H4)4Sb]+[ReO4]−

Complexes [(4-MeC₆H₄)₄Sb] ₂ ⁺ [Hg₂I₆]^2? (I), [(4-MeC₆H₄)₄Sb] ₂ ⁺ [HgI₄]^2? (II), [(4-MeC₆H₄)₄Sb] ₃ ⁺ [Sb₃I₁₂]^2? (III), were synthesized by reactions of tetra-p-tolylantimony iodide with mercury iodide and antimony iodide, respectively. Tetra-p-tolylantimony perrhenate [(4-MeC₆H₄)₄Sb]⁺[ReO₄]^? (IV) was prepared from tetra-p-tolylantimony chloride and sodium perrhenate in acetone. Crystal structures of complexes I, II, and IV were determined by X-ray crystallography. Mercury and rhenium atoms have tetrahedral coordinations in these complexes. The Hg-I and Re-O distances in the structures of I, II, and IV vary within 2.7719(13)–2.7908(12)Å, 2.7028(3)–2.9163(3) Å, and 1.693(3)–1.744(3) Å, respectively. Antimony atoms in two crystallographically independent trinuclear centrosymmetric [Sb₃I₁₂]^2? anions of complex III have an octahedral environment. Each terminal SbI₃ fragment (Sb-I_t, 2.8265(9)–2.8333(10)Å) is bound to the central atom through tree bridging iodine atoms (Sb(2)-I_br, 3.2275(9)–3.3620(10)Å). The distances between the central Sb atom and bridging iodine atoms are much shorter (Sb(1)-I_br, 3.0153(6)–3.0316(6) Å; Sb(3)-I_br, 2.9926(6)–3.0074(6) Å).     

从固相反应产物[NEt4]4[Mo2O2S6Cu6I4Br2]合成原子簇[MoOS3Cu3I(3,5-diMePy)4]·CH3CN和(EtN)4[Mo4Cu8O4S12{(Ph2PS)2}4](英文)

Treatment of iodide-bridged dimer [NEt4] 4[Mo2O2S6Cu6I4Br2] 1 with 3, 5-bimethylpyridine or with K[(Ph2PS) 2N] in CH3CN afforded the tetranuclear cluster [MoOS3Cu3I(3,5-diMePy)4]·CH3CN 2 and dodecanuclear cluster (Et4N)4[Mo4Cu8O4S12{(Ph2PS)2N}4] 3. Monomeric 2 possess a nest-shaped skeleton.The structure of oligomeric 3 can be regarded as a tetramer of nest-shaped MoCu3OS3[(Ph2PS)aN]groups co-polymerized by sharing the limbic Cu atoms.     

Thermal decomposition and reducibility of silica-supported precursors of Cu,Fe and Cu–Fe nanoparticles

Journal of Thermal Analysis and Calorimetry - Poly(butylene succinate) (PBS) nanocomposites filled with nanoprecipitated calcium carbonate (NPCC) were prepared via melt blending. The hybrid...     

Separation of CO2/CH4 and CH4/N2 mixtures using MOF-5 and Cu3（BTC）2

In this paper we used MOF-5 and Cu3（BTC）2 to separate CO2/CH4 and CI-I4/N2 mixtures under dynamic conditions. Both materials were synthesized and pelletized, thus allowing for a meaningful characterization in view of process scale-up. The materials were characterized by X-ray diffraction （XRD） and scanning electron microscopy （SEM）. By performing breakthrough experiments, we found that Cu3（BTC）2 separated CO2/CH4 slightly better than MOF-5. Because the crystal structure of Cu3 （BTC）2 includes unsaturated accessible metal sites formed via dehydration, it predominantly interacted with CO2 molecules and more easily captured them. Conversely, MOF-5 with a suitable pore size separated CH4/N2 more efficiently in our breakthrough test.