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Volumn 4, Issue 9, 2008, Pages 1449-1459

Geometries of third-row transition-metal complexes from density-functional theory

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Indexed keywords


EID: 58149236843     PISSN: 15499618     EISSN: None     Source Type: Journal    
DOI: 10.1021/ct800172j     Document Type: Article
Times cited : (426)

References (116)
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    • The equilibrium distance, re, is the distance between the positions of the nuclei on the potential energy surface, as obtained from standard geometry optimizations; rg is the average internuclear distance at temperature T; and reo is the average internuclear distance at 0 K. It is the latter value that our computed effective geometries refer to. Typical quantities derived experimentally are r a (the effective internuclear distance as derived from electron scattering intensity, rα (the distance between average nuclear positions in the thermal equilibrium at temperature T, rz (the distance between average nuclear positions in the ground vibrational state, or ro the effective internuclear distance obtained from the rotational constants, see e.g, Hargittai, I. In Stereochemical Applications of Gas-Phase Electron Diffraction, Part A: The Electron Diffraction Technique; Hargittai, I, Hargittai, M
    • z (the distance between average nuclear positions in the ground vibrational state), or ro (the effective internuclear distance obtained from the rotational constants), see e.g.: Hargittai, I. In Stereochemical Applications of Gas-Phase Electron Diffraction, Part A: The Electron Diffraction Technique; Hargittai, I., Hargittai, M., Eds.; VCH Publisher: Weinheim, 1988; pp 1-54.
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    • E.g., the eclipsed form is more stable than the staggered one by 3.7 and 4.3 kcal/mol at BP86/SDD and B3LYP/SDD levels, respectively.
    • E.g., the eclipsed form is more stable than the staggered one by 3.7 and 4.3 kcal/mol at BP86/SDD and B3LYP/SDD levels, respectively.
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    • A notable underestimation of this bond length has also been noted at the MP2/LANL/6-3+G* level, from which some geometrical and force-field parameters have been used during refinement of the GED data, cf. ref 47. In that paper an unusually high vibrational amplitude has been noted for this bond and has been attributed to a fluxional process exchanging bridging and terminal H atoms. If the potential energy surface for this process were highly anharmonic with a very low barrier, a theoretical description of the light H atoms might require quantum dynamical methods; however, we could find no evidence for this, because a notable barrier of 6.9 and 5.9 kcal/mol is indicated at the BP86/SDD and B3LYP/SDD levels, respectively (including zero-point energies, proceeding via a Hf(η3-BH4)3(η2-BH 4) transition state
    • 4) transition state.
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    • Only minor improvements are brought about by the use of an f-function on the metal taken from the following:Hollwart, A.; Böhme, M.; Dapprich, S.; Ehlers, A. W.; Gobbi, A.; Jonas, V.; Kohler, K. F.; Stegmann, R.; Veldkamp, A.; Frenking, G. Chem. Phys. Lett. 1993, 208, 237-240. Chem. Phys. Lett. 1994, 224, 603.
    • Only minor improvements are brought about by the use of an f-function on the metal taken from the following:Hollwart, A.; Böhme, M.; Dapprich, S.; Ehlers, A. W.; Gobbi, A.; Jonas, V.; Kohler, K. F.; Stegmann, R.; Veldkamp, A.; Frenking, G. Chem. Phys. Lett. 1993, 208, 237-240. Chem. Phys. Lett. 1994, 224, 603.
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    • Very recently, and after this work was started, more flexible basis sets have been devised for the Hay-Wadt ECPs, the combination thereof denoted LANL2TZ: Roy, L. E.; Hay, P. J.; Martin, R. L. J. Chem. Theory Comput. 2008, 4, 1029-1031.
    • Very recently, and after this work was started, more flexible basis sets have been devised for the Hay-Wadt ECPs, the combination thereof denoted LANL2TZ: Roy, L. E.; Hay, P. J.; Martin, R. L. J. Chem. Theory Comput. 2008, 4, 1029-1031.
  • 107
    • 58149263037 scopus 로고    scopus 로고
    • Because we had not tested the PBE1 functional, which performs so well for the geometries of the heavier metal complexes, in our initial study on the 3d congeners, we have now reoptimized the latter set at the PBE1/AE1 level. For this set alone, this level affords mean and standard deviations of-1.4 and 1.8 pm, respectively, for the equilibrium geometries, and-0.9 and 1.8 pm, respectively, for the effective geometries.
    • Because we had not tested the PBE1 functional, which performs so well for the geometries of the heavier metal complexes, in our initial study on the 3d congeners, we have now reoptimized the latter set at the PBE1/AE1 level. For this set alone, this level affords mean and standard deviations of-1.4 and 1.8 pm, respectively, for the equilibrium geometries, and-0.9 and 1.8 pm, respectively, for the effective geometries.
  • 108
    • 58149252027 scopus 로고    scopus 로고
    • 3(NO) were erroneously given as zero in Table 1 of ref 7b, whereas they should read 0.45 and 0.64 pm for the Co-N and Co-C bonds, respectively. We apologize for this oversight, which affects the final assessment of the whole set only marginally, and does not alter any of the qualitative conclusions.
    • 3(NO) were erroneously given as zero in Table 1 of ref 7b, whereas they should read 0.45 and 0.64 pm for the Co-N and Co-C bonds, respectively. We apologize for this oversight, which affects the final assessment of the whole set only marginally, and does not alter any of the qualitative conclusions.
  • 110
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    • in press, DOI: 10.1016/j.ccr.2008.05.014
    • (b) Neese, F. Coord. Chem. Rev. 2008, in press, DOI: 10.1016/j.ccr.2008.05.014.
    • (2008) Coord. Chem. Rev
    • Neese, F.1


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