Ligands weak interactions

Finally, the term steric stabihzation coifid be used to describe protective transition-metal colloids with traditional ligands or solvents [38]. This stabilization occurs by (i) the strong coordination of various metal nanoparticles with ligands such as phosphines [48-51], thiols [52-55], amines [54,56-58], oxazolines [59] or carbon monoxide [51] (ii) weak interactions with solvents such as tetrahydrofuran or various alcohols. Several examples are known with Ru, Ft and Rh nanoparticles [51,60-63]. In a few cases, it has been estab-hshed that a coordinated solvent such as heptanol is present at the surface and acts as a weakly coordinating ligand [61]. 

The X-ray structures of two ortho-metalated compounds, (166), have been discussed.310 Weak interactions between the hydride ligand and C—H protons of the PPh3 groups are recorded. 

The weak interactions that may exist between group 2 cations and anionic hydrocabyl ligands are demonstrated in the metal-in-a-box compounds such as [M(THF)6][Me3Si(fluorenyl)]2 (M = Ca 159 or Mg), which are formed by the addition of THF to solutions of the bis(fluorenyl) complexes in non-polar solvents. The box may be completed by the presence of aromatic molecules, as in 159 (Figure 84). The disruption of the metal-carbon bonds is thought to stem from a combination of robust M-THF interaction, the stability of the free [Me3Si(fluorcnyl)] ion, and the formation of numerous C-H- -7r interactions between THF and the anions. These and related examples are reviewed elsewhere. 

The temperature dependence of the molar magnetic susceptibility (x) of an assembly of paramagnetic spins without interaction is characterized by the Curie behavior with x = C/T where C = /Vy2( 2.S (.S + l)/3k. It is a very common situation in the organometallic chemistry of radical species when the spin density is essentially localized on the metal atom. Since, in most cases, this atom is surrounded by various innocent ligands, intermolecular interactions are very weak and in most cases are reflected by a small contribution described by a Curie-Weiss behavior, with x = C/(T 0) where 0 is the Curie-Weiss temperature. A positive value for 0 reflects ferromagnetic interactions while a negative value — the most common situation — reflects an antiferromagnetic interaction. 

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