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Free H2 Rotation vs Jahn鈥揟eller Constraints in the Nonclassical Trigonal (TPB)Co鈥揌2 Complex
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文摘
Proton exchange within the M鈥揌2 moiety of (TPB)Co(H2) (Co鈥揌2; TPB = B(o-C6H4PiPr2)3) by 2-fold rotation about the M鈥揌2 axis is probed through EPR/ENDOR studies and a neutron diffraction crystal structure. This complex is compared with previously studied (SiPiPr3)Fe(H2) (Fe鈥揌2) (SiPiPr3 = [Si(o-C6H4PiPr2)3]). The g-values for Co鈥揌2 and Fe鈥揌2 show that both have the Jahn鈥揟eller (JT)-active 2E ground state (idealized C3 symmetry) with doubly degenerate frontier orbitals, (e)3 = [|mL 卤 2>]3 = [x2 鈥?y2, xy]3, but with stronger linear vibronic coupling for Co鈥揌2. The observation of 1H ENDOR signals from the Co鈥揌D complex, 2H signals from the Co鈥揇2/HD complexes, but no 1H signals from the Co鈥揌2 complex establishes that H2 undergoes proton exchange at 2 K through rotation around the Co鈥揌2 axis, which introduces a quantum-statistical (Pauli-principle) requirement that the overall nuclear wave function be antisymmetric to exchange of identical protons (I = 1/2; Fermions), symmetric for identical deuterons (I = 1; Bosons). Analysis of the 1-D rotor problem indicates that Co鈥揌2 exhibits rotor-like behavior in solution because the underlying C3 molecular symmetry combined with H2 exchange creates a dominant 6-fold barrier to H2 rotation. Fe鈥揌2 instead shows H2 localization at 2 K because a dominant 2-fold barrier is introduced by strong Fe(3d)鈫?H2(蟽*) 蟺-backbonding that becomes dependent on the H2 orientation through quadratic JT distortion. ENDOR sensitively probes bonding along the L2鈥揗鈥揈 axis (E = Si for Fe鈥揌2; E = B for Co鈥揌2). Notably, the isotropic 1H/2H hyperfine coupling to the diatomic of Co鈥揌2 is nearly 4-fold smaller than for Fe鈥揌2.

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