
Journal of the American Chemical Society p. 6471 - 6475 (1985)
Update date:2022-08-05
Topics:
Sowa, Takayoshi
Kawamura, Takashi
Yamabe, Tokio
Yonezawa, Teijiro
Re2(μ-H)2(CO)8-., Re2(μ-D)2(CO)8-., and Re2(μ-H)2(CO)6(μ-dppm)-. have been examined with electron spin resonance spectroscopy.They have planar Re2H2 rhomboids and their odd-electron orbitals are the ?*ReRe orbital lying in the rhomboid.Rhenium hyperfine splitting tensors are interpreted most reasonable with the ?*ReRe orbital consisting of rhenium 5d and 6p AO's.The odd-electron density on the 5d AO is estimated to be around 0.26 for Re2(μ-H)2(CO)8-..The anisotropy of the rhenium hyperfine interaction due to the odd-electron density on the 6p AO is estimated as 42 * 10-4 cm-1, a magnitude similar to that due to the 5d odd-electron density, 57 * 10-4 cm-1.This large 5d-6p mixing is likely to arise from contraction and stabilization of 6p AO's and expansion and destabilization of 5d AO's due to relativistic effects.
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Doi:10.1002/jhet.5570220242
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