Visible light-induced electron transfer from di-mu-oxo-bridged dinuclear Mn complexes to Cr centers in silica nanopores

The compound (bpy) 2Mn (III)(mu-O) 2Mn (IV)(bpy) 2, a structural model relevant for the photosynthetic water oxidation complex, was coupled to single Cr (VI) charge-transfer chromophores in the channels of the nanoporous oxide AlMCM-41. Mn K-edge EXAFS spectroscopy confirmed that the di-mu-oxo dinuclear Mn core of the complex is unaffected when loaded into the nanoscale pores. Observation of the 16-line EPR signal characteristic of Mn (III)(mu-O) 2Mn (IV) demonstrates that the majority of the loaded complexes retained their nascent oxidation state in the presence or absence of Cr (VI) centers. The FT-Raman spectrum upon visible light excitation of the Cr (VI)-O (II) --> Cr (V)-O (I) ligand-to-metal charge transfer reveals electron transfer from Mn (III)(mu-O) 2Mn (IV) (Mn-O stretch at 700 cm (-1)) to Cr (VI), resulting in the formation of Cr (V) and Mn (IV)(mu-O) 2Mn (IV) (Mn-O stretch at 645 cm (-1)). All initial and final states are directly observed by FT-Raman or EPR spectroscopy, and the assignments are corroborated by X-ray absorption spectroscopy measurements. The endoergic charge separation products (Delta E o = -0.6 V) remain after several minutes, which points to spatial separation of Cr (V) and Mn (IV)(mu-O) 2Mn (IV) as a consequence of hole (O (I)) hopping as a major contributing mechanism. This is the first observation of visible light-induced oxidation of a potential water oxidation complex by a metal charge-transfer pump in a nanoporous environment. These findings will allow for the assembly and photochemical characterization of well-defined transition metal molecular units, with the ultimate goal of performing endothermic, multielectron transformations that are coupled to visible light electron pumps in nanostructured scaffolds.     

On the mechanism of dioxygen formation from a di-mu-oxo-bridged manganese dinuclear complex

Density functional theory (DFT) calculations, using the Becke-Perdew gradient-corrected functional with a triple-zeta-plus-polarization basis set, have been used to characterize the [(H(2)O)(H(3)N)(3)Mn(mu-O)(2)Mn(NH(3))(3)(OH(2))](q)(+) (q = 2-5) complexes. This structure has been proposed as a possible model for the oxygen-releasing site of the photosystem II (PSII) reaction center. We have performed full optimizations to locate stationary points in various spin states for each of the +2 to +5 charge states. Our calculations indicate that O(2) release from the vacuum-phase +5 charge state complex is barrier inhibited, in contrast to the results of a recent DFT study. We report several new di-mu-oxo-bridged stationary points with spin multiplicities of S = (1)/(2), (3)/(2), and (5)/(2) and effective metal oxidation states of Mn(IV)Mn(V) for the +5 charge state. Finally, calculations employing the 'conductorlike screening model' (COSMO), to address the inclusion of solvent effects, indicate that dissociative O(2) release from the +5 charge state model complex is inhibited by a major barrier and is therefore apparently highly disfavored.     

Temperature-induced formation of two dinuclear dysprosium complexes with different magnetic properties

A dinuclear Dy (III) complex [Dy₂( L ¹ )₂(NO₃)₄]·2CH₃CN ( 1 ) (H L ¹ = 1,3-bis{[(E)-pyridin-2-ylmethylene]amino}propan-2-ol) was obtained via the reaction of 1,3-diamino-2-propanol, 2-pyridyaldehyde and Dy (NO₃)₃·6H₂O at room temperature. In the structure of complex 1 , two Dy (III) ions are in the N₄O₆ coordination environment provided by NO₃⁻ and ( L ¹ )⁻, and both of these ions are in the sphenocorona configuration. [Dy₂( L ² )₂(NO₃)₄] ( 2 ) [H L ² = 2-(pyridin-2-yl)hexahydropyrimidin-5-ol] was obtained using the same reaction material only when the reaction temperature was changed to 60°C. Structural analysis of complex 2 showed that the two Dy (III) ions with the same coordination configuration are in the N₃O₆ coordination environment provided by NO₃⁻ and ( L ² )⁻ and are in the distorted spherical-capped square antiprism. Surprisingly, H L ² with the parent of bipyridine was synthesized by the Schiff base reaction of 1,3-diamino-2-propanol with 2-pyridoxaldehyde followed by the ring-closing reaction catalyzed by Dy (III) ions. Magnetic measurements of the Dy (III) complexes revealed no obvious frequency-dependent behavior of complex 1 . In contrast, complex 2 showed an obvious frequency dependence (U_eff = 0.49 K and τ₀ = 6.62 × 10⁻⁴ s) under the condition of zero field and a weak double relaxation behavior (U_eff = 9.25 K and τ₀ = 9.70 × 10⁻⁴ s) at 1500 Oe.     

Syntheses,crystal structures,and magnetic properties of a series of double end-on azido-bridged dinuclear manganese(II) complexes

Four azido-bridged dinuclear Mn(II) complexes, [Mn₂(phen)₄ μ-₁,₁-N₃)₂][Fe^III(bpmb)(CN)₂]₂·H₂O (1), [Mn₂(phen)₄(μ-₁,₁-N₃)₂][Fe^III(bpClb)(CN)₂]₂·H₂O (2), and [Mn₂(phen)₄(μ-₁,₁-N₃)₂][M^III(bpdmb)(CN)₂]₂·3H₂O [M = Fe (3) or Cr (4); phen = 1,10-phenanthroline, bpmb^2– = 1,2-bis(pyridine-2-carboxamido)-4-methyl-benzenate, bpClb^2– = 1,2-bis(pyridine-2-carboxamido) 4-chloro-benzenate, bpdmb^2– = 1,2-bis(pyridine-2-carboxamido)-4,5-dimethyl-benzenate], have been synthesized using the synthetic strategy of large anion inducement. Single-crystal X-ray diffraction analysis reveals that all four complexes are doubly end-on (EO) azido-bridged binuclear Mn(II) complexes with two large [M(L)(CN)₂]^– (L = bpmb^2?, bpClb^2?, or bpdmb^2?) building blocks acting as charge-compensating anions. The magnetic properties of the complexes have been investigated, and the results indicate that the magnetic coupling between two Mn(II) centers through the EO azide bridges is ferromagnetic, with J = 0.64(1) cm^?1 for 1, 0.43(1) cm^?1 for 2, 0.50(1) cm^?1 for 3, and 0.66(2) cm^?1 for 4. The magneto-structural relationships of EO azido-bridged Mn(II) systems are discussed.     

Synthesis and magnetic properties of tetrabromophthalato-bridged manganese(II) binuclear complexes

Summary Four novel Mn^II binuclear complexes have been prepared and characterized, namely: [Mn₂(TBPHTA)(L)₄](ClO₄)₂ [L = 2,2-bipyridyl (bipy), 1,10-phenanthroline (phen), 4,4-dimethyl-2,2-bipyridyl (Me₂bipy) and 5-nitro-1,10-phenanthroline (NO₂-phen), respectively], and TBPHTA = the tetrabromophthalate dianion. Based on i.r. spectra, elemental analyses and conductivity measurements, extended tetrabromophthalato-bridged structures consisting of two Mn^II ions, in which each Mn^II ion has a distorted octahedral environment, are proposed for these complexes. The temperature dependence of the magnetic susceptibility for [Mn₂(TBPHTA)(phen)₄] (ClO₄)₂·H₂O was measured over the 4–300 K range and the observed data were successfully simulated by an equation based on the spin Hamiltonian operator ( = -2J _{1 2}), giving the exchange integral J = -1.22 cm^–1. This result indicates a weak antiferromagnetic spin exchange interaction between the metal ions.     

Synthesis and magnetic properties of chloroanilato-bridged manganese(II) binuclear complexes

Five chloroanilato-bridged manganese(II) binuclear complexes, [Mn₂(CA)L₄](ClO₄)₂, where L = 4,4′-dimethyl-2,2′-bipyridine (Me₂-bpy), 5-methyl-1,10-phenanthroline (Me-phen), 5-chloro-1,10-phenanthroline (Cl-phen), 5-nitro-1,10-phenanthroline (NO₂-phen) and 2,9-dimethyl-1,10-phenanthroline (Me₂-phen), and CA represents the dianion of chloroanilic acid, have been synthesized and characterized by elemental analyses, molar conductivity and room temperature magnetic moment measurements, and by spectroscopy. It is proposed that these complexes have CA-bridged structures and consist of two manganese(II) ions in a distorted-octahedral environment. The complexes [Mn₂(CA)(Me₂-bpy)₄](ClO₄)₂ (1) and [Mn₂(CA)(Me-phen)₄](ClO₄)₂ (2) were characterized by variable temperature magnetic susceptibility measurements (4–300 K) and the observed data were successfully simulated by an equation based on the spin Hamiltonian operator, Ĥ = −2JŜ ₁ Ŝ ₂, giving the exchange integral J = −1.98 cm⁻¹ for (1) and J = −2.41 cm⁻¹ for (2). This result indicates that there is a weak antiferromagnetic spin-exchange interaction between the two Mn^II ions within each molecule. This revised version was published online in June 2006 with corrections to the Cover Date.     

Formation and characterization of mononuclear and dinuclear manganese oxide-dioxygen complexes in solid argon

A manganese atom reacts with dioxygen to form the previously characterized MnO 2 molecule in solid argon under UV-visible light irradiation. Subsequent sample annealing allows the dioxygen molecules to diffuse and to react with MnO 2 to give the (eta (2)-O 2)MnO 2 complex, which is characterized to be a side-on bonded peroxo manganese dioxide complex. The manganese tetraoxide MnO 4, which was predicted to be less stable than the (eta (2)-O 2)MnO 2 isomer, was not observed. However, the (eta (2)-O 2)MnO 2 complex reacts with another weakly coordinated dioxygen to give the (eta (2)-O 2)MnO 4 complex via visible light irradiation, in which the manganese tetraoxide is coordinated and stabilized by a side-on bonded O 2 molecule. Manganese dimer reacts with dioxygen to form the cyclic Mn(mu-O) 2Mn cluster spontaneously upon annealing, which further reacts with dioxygen to give the (eta (2)-O 2) 2Mn(mu-O) 2Mn cluster, a side-on bonded disuperoxide complex with a planar D 2 h structure.     

Decomposition of dinuclear manganese complexes for the preparation of nanostructured oxide materials

The crystal structures of several dinuclear complexes of manganese are reported, and the decomposition and analysis of the nanostructured products derived from them are presented. 1,4,7,10-Tetraazacyclododecane (cyclen) forms dinuclear complexes 1-4 containing doubly oxo-bridged or oxo-acetato bridging ligands depending on the manganese salt used for the reaction. Doubly oxo-bridged 1 crystallizes in the orthorhombic space group Pnma, a = 22.3850(14) A, b = 9.1934(5) A, c = 13.2424(10) A, V = 2725.2(3) A(3). 2, containing [Mn(SCN)5](3-) conteranions, crystallizes in monoclinic space group I2/a with a = 18.2699(10) A, b = 11.2384(6) A, c = 18.6432(9) A, alpha = 90.00 degrees, beta = 114.510(6) degrees, gamma = 90.00 degrees, V = 3483.0(3) A(3). Oxo-acetato-bridged 3 crystallizes in orthorhombic space group Pca21, a = 13.9322(11) A, b = 16.2332(13) A, c = 14.6794(8) A, V = 3320.0(4) A(3). Compound 4 consists of a templated quasi-one-dimensional manganese oxalate crystallized in the triclinic space group P1, a = 9.5442(11) A, b = 10.3758(10) A, c = 21.851(2) A, alpha = 83.720(12) degrees, beta = 80.106(13) degrees, gamma = 85.457(13) degrees, V = 2114.9(4) A(3). Compounds 1, 3, and 4 decompose to nanostructured oxide materials, which may be isolated in bulk as lamellar-structured particles or microspheres or deposited on substrates.     

Role of the electron transfer and magnetic exchange interactions in the magnetic properties of mixed-valence polyoxovanadate complexes

Modeling the properties of high-nuclearity, high-electron-population, mixed-valence (MV) magnetic systems remains one of the open challenges in molecular magnetism. In this work, we analyze the magnetic properties of a series of polyoxovananadate clusters of formula [V 18O 42] (12-) and [V 18O 42] (4-). The first compound is a fully localized spin cluster that contains 18 unpaired electrons located at the metal sites, while the second one is a MV cluster with 10 unpaired electrons largely delocalized over the 18 metal sites. A theoretical model that takes into account the interplay between electron transfer and magnetic exchange interactions is developed to explain the unexpected enhancement of the antiferromagnetic coupling when the number of unpaired electrons is reduced from 18 to 10 in these clusters. In the MV area, these systems represent the most complex magnetic clusters studied theoretically so far. Because of the high complexity of the systems, the number of relevant parameters is too large for a conventional model Hamiltonian approach. We therefore perform a theoretical study that combines ab initio calculations with the model Hamiltonian. In this way, we use ab initio calculations performed on small fragments of the cluster to lower the degrees of freedom of the parameter set of the model Hamiltonian that operates in the whole MV cluster. This approach shows the usefulness of combining ab initio calculations with model Hamiltonians in order to explore the magnetic properties of large and complex molecular systems, emphasizing the key role played by the electron transfer in these model magnetic materials.     

Synthesis,crystal structure and magnetic properties of a dinuclear manganese(III) tetradentate Schiff-base complex

A dinuclear manganese(III) tetradentate Schiff-base complex, [Mn₂(salophen)₂(4,4′-bipy)₃](BPh₄)₂ (1) (salophen = N,N′-o-phenylene-bis(salicylideneaminato)), has been synthesized and structurally characterized. Compound 1 crystallized in the triclinic, P 1 space group, a = 13.431(4), b = 13.791(4), c = 13.886(4) Å, α = 73.599(5)°, β = 80.410(6)°, γ = 71.241(5)°, V = 2328.3(12) ų. Complex 1 contains two Mn(salophen) moieties bridged by 4,4′-bipy to form a dinuclear unit, with two terminal 4,4′-bipy ligands. Variable temperature magnetic susceptibility (2–300 K) shows very weak ferromagnetic interactions between the Mn(III) ions.     

Catalytic properties of dinuclear copper(II) complexes in the oxidation of two electron donors by dioxygen

Summary Dinuclear copper(II) complexes of differing magnetic and redox properties derived from various dinucleating ligands were investigated for their catalytic activity in the oxidation of 3,5-di-t-butylcatechol (3,5-DTBC) and ascorbic acid by oxygen. Poor activity was exhibited by di--hydroxocopper(II) complexes of 2,2-bypyridyl, 1,10-phenanthroline and N,N,N,N-tetramethylethylenediamine(TMEDA). Dicopper(II) complexes of Schiff base ligands, obtained from 2,6-diformyl-4-methylphenol and diamines, are relatively less active compared with ligands derived from monoamines. The difference is explained on the basis of redox behaviour.     

Computational modeling of structure and magnetic properties of dinuclear di-o-benzoquinone iron complexes with linear polycyclic linkers

Density functional theory (DFT UTPSSh/6-311++G(d,p)) quantum chemical modeling of geometry, energy and magnetic characteristics of binuclear iron complexes, in which iron atoms coordinated by 2,11-diaza[3.3](2,6)pyridinophane bases are connected by di-o-benzoquinone ligands with acene linkers, was performed. It is established that the energy diff erence between electromeric forms of the studied compounds is determined by the type of the alkyl substituents at the nitrogen atoms of the tetraazamacrocyclic ligand and does not depend on the structure of the polycyclic chain. The possibility of controlling magnetic properties of the molecules of this type by means of external influences is predicted based on the facts that terminal metal-containing fragments are capable of undergoing thermally induced spin-state switching rearrangements, while the singlet-triplet transition of the acene linker can be induced by light irradiation.

     

Synthesis,crystal structures,and catalytic properties of phenoxo-bridged dinuclear manganese(III) complexes with bis-Schiff bases

Two structurally similar centrosymmetric phenoxo-bridged dinuclear manganese(III) complexes, [Mn₂(L¹)₂(N₃)₂] (1) and [Mn₂(L²)₂(NCS)₂] (2), were prepared from the tetradentate bis-Schiff base ligands, N,N’-bis(salicylidene)propane-1,2-diamine (H₂L¹) and N,N’-bis(salicylidene)ethane-1,2-diamine (H₂L²), respectively, in the presence of pseudohalides. The complexes have been characterized by FTIR, elemental analyses, and molar conductivity. Structures of the complexes have been confirmed by single-crystal X-ray determination. The bis-Schiff base ligands coordinate with Mn through their phenolate oxygen and imino nitrogen. Each Mn is an octahedral. The complexes showed that they exhibit high activity in catalytic olefin oxidation.     

氧桥联稀土钆双核配合物磁学性质的密度泛函理论研究

采用密度泛函理论结合对称性破损态方法,选用氧桥联稀土钆双核配合物为研究对象,通过与实验值比较,探讨了不同泛函与基组对计算磁耦合常数的影响.结果表明,在B3LYP/TZV水平下(Gd为SARC-TZV),相对论效应采用DHK2方法,计算结果与实验测量值-0.022 5cm~(-1)最接近.不同体系测试结果显示,可在该水平下预测新合成稀土钆双核配合物的磁学性质.Mulliken自旋密度分析可知磁中心Gd以自旋极化为主.键级分析表明,2个磁中心之间的磁耦合作用通过桥联氧原子的超交换作用实现.分子磁轨道分析显示2个磁中心间存在较强的轨道相互作用,其磁轨道主要是由钆原子的4f_z~3,4f_z~2_x轨道和桥联氧原子的2pz轨道组成.     

基于氮氧自由基配体的锰和钴双核配合物的分子结构和磁性

合成了2个基于氮氧自由基配体且结构类似的双核配位化合物,其分子式分别为[Mn₂(hfac)₄(NIT-mo-pmy)₂](1)和[CO₂(hfac)₄(NIT-mo-pmy)₂](2),其中hfac=六氟乙酰丙酮,NIT-mo-pmy=2-(2-甲氧基-5′-嘧啶基)-4,4,5,5-四甲基咪唑啉基-3-氧-1-氧自由基。2个配合物均属于三斜晶系P1空间群,其双核配位单元进一步构筑为中心对称的平行四边形分子阵列。变温磁化率的测试表明,在2个配合物中,中心离子和氮氧自由基单元之间存在反铁磁交换作用。借助构效关系研究,分析了磁作用强度的差异。通过适当近似的磁化学模型,对Mn(Ⅱ)配合物的磁性行为进行了定量拟合,并与相关化合物磁作用强度进行了比对、分析。     

基于氮氧自由基配体的锰和钴双核配合物的分子结构和磁性

合成了2个基于氮氧自由基配体且结构类似的双核配位化合物,其分子式分别为[Mn₂(hfac)₄(NIT-mo-pmy)₂](1)和[Co₂(hfac)₄(NIT-mo-pmy)₂](2),其中hfac=六氟乙酰丙酮,NIT-mo-pmy=2-(2-甲氧基-5′-嘧啶基)-4,4,5,5-四甲基咪唑啉基-3-氧-1-氧自由基。2个配合物均属于三斜晶系P1空间群,其双核配位单元进一步构筑为中心对称的平行四边形分子阵列。变温磁化率的测试表明,在2个配合物中,中心离子和氮氧自由基单元之间存在反铁磁交换作用。借助构效关系研究,分析了磁作用强度的差异。通过适当近似的磁化学模型,对Mn (Ⅱ)配合物的磁性行为进行了定量拟合,并与相关化合物磁作用强度进行了比对、分析。     

Synthesis characterization and magnetic properties of μ-iodanilato dinuclear oxovanadium(IV) complexes

Five oxovanadium(IV) dinuclear complexes described by the overall formula [(VO)₂(IA)L₂SO₄, where IA repents the dianion of iodanilic acid and L denotes 2, 2′-bipyridine (bpy); 4,4′-dimethy12,2′-bipyridine (Meo-bpy); 1,10-phenanthroline (phen); 4,7-diphenyl-l, 10-phenanthroline (Ph₂-phen) and 5-nitro-1, 10-phenanthroline (NO₂-phen), have been synthesized and characterized by elemental analyses, molar conductivity and roomtemperature magnetic moment measurements, IR and electronic spectral studies. It is proposed that these complexes have IA-bridged structures and consist of two oxovanadium(IV) ions each in a square pyramidal environment. The complexes (VO)₂(IA) (bpy)₂]SO₄, (1) and[(VO)₂( IA) (phen)₂ ]SO₄ (2) were further characterized by variable temperature (4.2–300 K) magnetic susceptibility measurements and the observed data were fitted to the modified Bleaney-Bowers equation by the least-squares method, giving the exchange integral J = - 2.15 m^?1 for 1 and J = - 9.88 cm^?1 for 2. This result indicates that there is a weak antiferromagnetic spin-exchange interaction between the two VO²⁺ ions within each molecule.