Cerium masquerading as a group 4 element: synthesis, structure and computational characterisation of [CeCl(N(SiMe3)2)3].

Oxidation of the three-coordinate cerium amide [Ce(N-(SiMe3)2)3] with TeCl4 in toluene solution yields purple, diamagnetic [CeCl(N(SiMe3)2)3], whose structure has been examined by X-ray crystallographic and computational methods.

Does the Mode of Dioxygen Binding to Dinuclear Copper Complexes Depend on the Spectator Nitrogen-Containing Ligands? An ab Initio Theoretical Study.

Ab initio two-determinants GVB computations (required to get the appropriate representation of the lowest singlet states of such systems) have been carried out for (Cu(+)(NH(3))(n)())(2)-O(2) (n = 0-3) and [Cu(2)(&mgr;-pydz)(2)(cnge)(2)](2+)-O(2). Different dioxygen binding modes (ranging from perpendicular to parallel with respect to the Cu-Cu direction) on these complexes have been examined. The results obtained show unambiguously that the parallel arrangements are always the less stable ones. In the especially important case of (Cu(+)(NH(3))(3))(2)-O(2) complexes, both staggered and eclipsed conformations have been considered. They are found almost isoenergetic, and the optimized geometrical parameters are, for a perpendicular O(2) binding onto a staggered complex, in fine agreement with corresponding experimental data obtained from either oxyhemocyanin or its synthetic models. In the case of a (Cu(+)(NH(3))(4))(2)-O(2) complex, taken as a model for Karlin's [{(TMPA)Cu}(2)-O(2)](2+) complex, the computations tend to show that the experimental end-on (trans &mgr;-1,2) O(2) binding is due to the presence of four nitrogens in the copper's coordination shell. Regarding the complexes with [Cu(2)(&mgr;-pydz)(2)(cnge)(2)](2+), the results indicate that the dioxygen binding mode remains perpendicular even if the fixation of a third pyridazine is known to occur in a parallel manner on this complex.

DFT calculations of 29Si-NMR chemical shifts in Ru(II) silyl complexes: searching for trends and accurate values.

The (29)Si chemical shifts in a series of closely related Ru(II) silyl complexes have been calculated by DFT methods and compared to the experimental values. The factors that lead to possible discrepancies between experimental and calculated values have been identified. It is shown that it is necessary to include the spin-orbit coupling associated with the relativistic effects of the heavy atoms for quantitative agreement with observed chemical shifts but trends are reasonably reproduced when the calculations do not include this correction. An NBO analysis of the NMR contributions from the bonds to Si and the Si core shows the greater importance of the former and a fine tuning originating from the latter.

Catalytic hydrosilylation of olefins with organolanthanides: A DFT study. Part I: Hydrosilylation of propene by SiH4.

Investigation of the catalytic hydrosilylation of propene by primary silane in the presence of Cp(2)SmH has been carried out using DFT calculations. Using SiH(4) as a model, it is shown that a catalytic cycle based on the hydride complex is unlikely. The activation of silane after insertion of propene is not competitive compared to the allylic activation of propene or the silyl formation. An alternative catalytic cycle, based on a silyl complex, is proposed. This alternative pathway accounts for the experimental observation. The allylic activation of propene is shown to be one of the main routes for the catalyst deactivation.

Catalytic hydrosilylation of olefins with organolanthanide complexes: a DFT study. Part II: Influence of the substitution on olefin and silane.

The reaction mechanism of the catalytic hydrosilylation of olefins in the presence of the samarium hydride (η(5)-C(5)H(5))(2)SmH has been investigated for several silanes and olefins with DFT calculations. For any substrate, the active species is the silyl complex, formed in situ from the reaction of the metal hydride with the silane. In agreement with the experimental data, the substitution of hydrogen by methyl groups in the silane decreases the catalytic turn-over. This result is shown to have electronic origins: the methyl group decreases the electron density on the silicon atom, which weakens the Sm-Si bond and decreases the ability for the silyl group to stabilise the positively charged group in a σ-bond metathesis transition state. Substituting hydrogen by alkyl groups on the olefin modifies mostly steric effects, and, depending on the position of the substituting group, it can result in an increase or a decrease of the catalytic yield.

Dinitrogen dissociation on an isolated surface tantalum atom.

Both industrial and biochemical ammonia syntheses are thought to rely on the cooperation of multiple metals in breaking the strong triple bond of dinitrogen. Such multimetallic cooperation for dinitrogen cleavage is also the general rule for dinitrogen reductive cleavage with molecular systems and surfaces. We have observed cleavage of dinitrogen at 250 degrees C and atmospheric pressure by dihydrogen on isolated silica surface-supported tantalum(III) and tantalum(V) hydride centers [(identical with Si-O)2Ta(III)-H] and [(identical with Si-O)2Ta(V)H3], leading to the Ta(V) amido imido product [(identical with SiO)2Ta(=NH)(NH2)]: We assigned the product structure based on extensive characterization by infrared and solid-state nuclear magnetic resonance spectroscopy, isotopic labeling studies, and supporting data from x-ray absorption and theoretical simulations. Reaction intermediates revealed by in situ monitoring of the reaction with infrared spectroscopy support a mechanism highly distinct from those previously observed in enzymatic, organometallic, and heterogeneous N2 activating systems.

DFT study of H--H activation by Cp(2) LnH d(0) complexes.

The energy required to activate the H--H bond in the entire series of Cp(2)LnH complexes has been calculated by DFT (B3PW91) methods. The activation energies have been calculated to vary from 0.5 to 8.0 kcal x mol(-1), indicating an overall facile reaction. The electronegativity of the lanthanide in its most stable oxidation state is suggested to be a leading factor for interpreting the trends in activation energy. The geometry of the transition state is best viewed as an almost linear H(3)(-) ligand with short H--H distances and strong M--H interaction, through the wingtip H centers, with Ln. The exchange reaction is thus established to be a sigma bond metathesis reaction.

Are the carbon monoxide complexes of Cp(2)M (M = Ca, Eu, or Yb) carbon or oxygen bonded? An answer from DFT calculations.

DFT calculations have been performed on the CO adducts of the bivalent lanthanides, Cp(2)M(CO)(x), where M is Eu or Yb and x is 1 or 2, the alkaline earth metallocene Cp(2)Ca(CO), and the methylisocyanide adducts of Yb. The calculated nu(CO) values are in agreement with experiment for Cp(2)M(CO) when M is Ca or Eu, but in striking disagreement when the CO is bound to the metal by way of the carbon atom in CO in the case of Yb. The calculated nu(CO) values for M = Yb are brought into agreement with experiment when the CO is allowed to bond to Cp(2)Yb by way of the oxygen atom.

Hypothetical strain-free oligoradicals.

Several new classes of oligoradicals free of angle strain are suggested and examined by means of molecular orbital calculations. The collapse products of these hypothetical radicals are highly strained molecules. Various electronic strategies for the stabilization of these oligoradicals have been explored.

Theoretical study of oxyhemocyanin active site: a possible insight on the first step of phenol oxidation by tyrosinase.

Extended Huckel theory calculations have been carried out on a model of the oxyhemocyanin active site that includes six imidazoles, the two copper cations, and a dioxygen molecule. The results obtained for the very likely mu-eta 2:eta 2 arrangement of the dioxygen molecule show that the most favorable orientation of O2 is such that the two long Cu-N coordination bonds are perpendicular to the plane formed by the two metal atoms and O2. This arrangement leads to pentacoordinated coppers with a distorted square pyramidal geometry. The molecular electrostatic potential maps of the complexes exhibit a potential well located close to the peroxo anion midbond. The dependence of the energy and of the molecular electrostatic maps on the precise orientation and location of the imidazole rings has been investigated. These results, which show the important role played by the third remote imidazole ligand, are discussed in relation with the first step of tyrosinase-mediated phenol oxidation.

Unsaturated Ru(0) species with a constrained bis-phosphine ligand: [Ru(CO)2(tBu2PCH2CH2PtBu2)]2. Comparison to [Ru(CO)2(PtBu2Me)2].

The synthesis of Ru(C2H4)(CO)2(dtbpe) (dtbpe = tBu2PC2H4PtBu2), then green [Ru(CO)2(dtbpe)]n is described. In solution, n = 1, while in the solid state, n = 2; the dimer has two carbonyl bridges. DFTPW91, MP2, and CCSD(T) calculations show that the potential energy surface for bending one carbonyl out of the RuP2C(O) plane is essentially flat. Ru(CO)2(dtbpe) reacts rapidly in benzene solution to oxidatively add the H-E bond of H2, HCl, HCCR (R = H, Ph), [HOEt2]BF4, and HSiEt3. The H-C bond of C6HF5 oxidatively adds at 80 degrees C. CO adds, as does the C=C bond of H2C=CHX (X = H, F, Me). The following do not add: N2, THF, acetone, H3COH, and H2O.

Computed ligand electronic parameters from quantum chemistry and their relation to Tolman parameters, Lever parameters, and Hammett constants.

The calculated (DFT, B3PW91) A(1) nu(CO) frequency in LNi(CO)(3) defines an electronic parameter that reliably predicts the relative donor powers of a wide variety of cationic, neutral, and negatively charged ligands. These calculated parameters correlate very well with the available Tolman and Lever parameters, and also with Hammett's sigma(m), where available. The method avoids any experimental limitations and, in particular, can be used for proposed ligands not yet experimentally available.

Equilibria between alpha- and beta-agostic stabilized rotamers of secondary alkyl niobium complexes.

The isopropyl chloro complex Tp(Me2)NbCl(i-Pr)(PhC&tbd1;CMe) (2) [Tp(Me2) = hydrotris(3,5-dimethylpyrazolyl)borate] exhibits a beta-agostic structure in the crystal. The conformation of the alkyl group is such that the agostic methyl group lies in the Calpha-Nb-Cl plane and the nonagostic one, in a wedge formed by two pyrazole rings. As observed by solution NMR spectroscopy, restricted rotation about the Nb-C bond allows the observation of an equilibrium between this species, 2beta, and a minor alpha-agostic rotamer 2alpha. A putative third rotamer which would have the secondary hydrogen in the wedge is not observed. Similar behavior is observed for related Tp'NbCl(i-Pr)(R(2)C=CMe) [Tp' = Tp(Me2), R(2) = Me (3); Tp' = Tp(Me2,4Cl), R(2) = Ph (4)]. The two diastereomers of the sec-butyl complex Tp(Me2)NbCl(sec-Bu)(MeC=CMe) (5) have been separated. In the crystal, 5CR-AS has a beta-agostic methyl group with the ethyl group located in the wedge formed by two pyrazole rings. The same single beta-agostic species is observed in solution. The other diastereomer, 5AR-CS has a beta-agostic methylene group in the solid state, and the methyl group sits in the wedge. In solution, an equilibrium between this beta-agostic methylene complex 5AR-CSbeta and a minor alpha-agostic species 5AR-CSalpha, where the ethyl substituent of the sec-Bu group is located in the wedge between two pyrazole rings, is observed. NMR techniques have provided thermodynamic parameters for these equilibria (K = 2beta/2alpha = 4.0 +/- 0.1 at 193 K, DeltaG(o)(193) = -2.2 +/- 0.1, DeltaH(o) = -7.4 +/- 0.1 kJ mol(-)(1), and DeltaS(o) = -27 +/- 1 J K(-)(1) mol(-)(1)), as well as kinetic parameters for the rotation about the Nb-C bond (at 193 K, DeltaG(2)= 47.5 +/- 2.5, DeltaH= 58.8 +/- 2.5 kJ mol(-)(1), and DeltaS = 59.0 +/- 10 J K(-)(1) mol(-)(1)). Upon selective deuteration of the beta-methyl protons in Tp(Me2)NbCl[CH(CD(3))(2)](PhC=CMe) (2-d(6)), an expected isotope effect that displaces the equilibrium toward the alpha-agostic rotamer is observed (K = 2-d(6)beta/2-d(6)alpha = 3.1 +/- 0.1 at 193 K, DeltaG(o)(193) = -1.8 +/- 0.1, DeltaH(o) = -8.3 +/- 0.4 kJ mol(-)(1) and DeltaS(o)= -34 +/- 2 J K(-)(1) mol(-)(1)). The anomalous values for DeltaH(o) and DeltaS(o) are discussed. Hybrid quantum mechanics/molecular mechanics calculations (IMOMM (B3LYP:MM3)) on the realistic model Tp(Me2)NbCl(i-Pr)(HC=CMe) have reproduced the energy differences between the alpha- and beta-agostic species with remarkable accuracy. Similar calculations show that Tp(Me2)NbCl(CH(2)Me)(HC=CMe) is alpha-agostic only and that Tp(5)(-)(Me)NbCl(CH(2)Me)(HC=CMe), which has no methyl groups at the 3-positions of the pyrazole rings, is beta-agostic only. Analysis and discussion of the computational and experimental data indicate that the unique behavior observed for the secondary alkyl complexes stems from competition between electronic effects favoring a beta-agostic structure and steric effects directing a bulky substituent in the wedge between two pyrazole rings of Tp(Me2). All of the secondary alkyl complexes thermally rearrange to the corresponding linear alkyl complexes via a first-order reaction.

Facile C(sp(2))/OR bond cleavage by Ru or Os.

Os(H)(3)ClL(2) (L = P(i)Pr(3) or P(t)Bu(2)Me) are shown to be useful "precursors" to "OsHClL(2)", which react with vinyl ethers to form first an eta(2)-olefin adduct and then isomerize to the carbenes, OsHCl[CMe(OR)]L(2). Subsequent R- and L-dependent reactions involve C(sp(2))-OR bond cleavage, to make either carbyne or vinylidene complexes. The mechanisms of these reactions are explored, and the thermodynamic disparity of Ru versus Os and the influence of the OR group and the spectator phosphine ligands are discussed based on DFT (B3PW91) calculations.