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The 20e and 21e electron counts are derived in the "usual" way that organometallic complexes of cyclohydrocarbyl ligands are derived. The electrons included in the count are the π electrons of the Ch ligands and the valence electrons of the An atom
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The 20e and 21e electron counts are derived in the "usual" way that organometallic complexes of cyclohydrocarbyl ligands are derived. The electrons included in the count are the π electrons of the Ch ligands and the valence electrons of the An atom.
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0 single-group orbital. We expect that the inclusion of these effects would not cause any significant change in the geometries calculated in this paper.
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Because the calculations on the two-open-shell configurations have been carried out in the restricted Kohn-Sham (RKS) formalism, the spin quantum numbers for the resultant states are ambiguous. The state energies are multiplet averages of the pure singlet and triplet states. In principle, the pure triplet state energy could be obtained from unrestricted Kohn-Sham (UKS) calculations. However, upon the inclusions of spin-orbit coupling, the notion of singlet and triplet state becomes less relevant so we report only the RKS results for these configurations.
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For an approach to the near-degenerate problem in density functional methods, see: (a) Dunlap, B. I. In Ab initio Methods in Quantum Chemistry II; Lawley, K. P., Ed.; Wiley: New York, 1987. (b) Wang, S. G.; Schwarz, W. H. E. J. Chem. Phys. 1996, 105, 4641 and references cited therein.
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2 is 0.9 ± 0.3 kcal/mol. See: (a) Haaland, A.; Nilsson, J. E. Acta Chem. Scand. 1968, 22, 2653. (b) Laane, J. J. Coord. Chem. 1971, 1, 75. (c) Carter, S.; Murrell, J. N. J. Organomet. Chem. 1980, 192, 399. (d) Bencivenni, L.; Ferro, D.; Pelino, M.; Teghil, R. J. Indian Chem. Soc. 1980, 57, 1062. (e) Marverick, E.; Dunitz, J. D. Mol. Phys. 1987, 62, 451.
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2 is 0.9 ± 0.3 kcal/mol. See: (a) Haaland, A.; Nilsson, J. E. Acta Chem. Scand. 1968, 22, 2653. (b) Laane, J. J. Coord. Chem. 1971, 1, 75. (c) Carter, S.; Murrell, J. N. J. Organomet. Chem. 1980, 192, 399. (d) Bencivenni, L.; Ferro, D.; Pelino, M.; Teghil, R. J. Indian Chem. Soc. 1980, 57, 1062. (e) Marverick, E.; Dunitz, J. D. Mol. Phys. 1987, 62, 451.
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2 is 0.9 ± 0.3 kcal/mol. See: (a) Haaland, A.; Nilsson, J. E. Acta Chem. Scand. 1968, 22, 2653. (b) Laane, J. J. Coord. Chem. 1971, 1, 75. (c) Carter, S.; Murrell, J. N. J. Organomet. Chem. 1980, 192, 399. (d) Bencivenni, L.; Ferro, D.; Pelino, M.; Teghil, R. J. Indian Chem. Soc. 1980, 57, 1062. (e) Marverick, E.; Dunitz, J. D. Mol. Phys. 1987, 62, 451.
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2 is 0.9 ± 0.3 kcal/mol. See: (a) Haaland, A.; Nilsson, J. E. Acta Chem. Scand. 1968, 22, 2653. (b) Laane, J. J. Coord. Chem. 1971, 1, 75. (c) Carter, S.; Murrell, J. N. J. Organomet. Chem. 1980, 192, 399. (d) Bencivenni, L.; Ferro, D.; Pelino, M.; Teghil, R. J. Indian Chem. Soc. 1980, 57, 1062. (e) Marverick, E.; Dunitz, J. D. Mol. Phys. 1987, 62, 451.
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2 is 0.9 ± 0.3 kcal/mol. See: (a) Haaland, A.; Nilsson, J. E. Acta Chem. Scand. 1968, 22, 2653. (b) Laane, J. J. Coord. Chem. 1971, 1, 75. (c) Carter, S.; Murrell, J. N. J. Organomet. Chem. 1980, 192, 399. (d) Bencivenni, L.; Ferro, D.; Pelino, M.; Teghil, R. J. Indian Chem. Soc. 1980, 57, 1062. (e) Marverick, E.; Dunitz, J. D. Mol. Phys. 1987, 62, 451.
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5h conformer has been found to be more stable in the gas phase by electron diffraction and in the solid state by X-ray or neutron diffraction. See: (a) Dunitz, J. D.; Orgel, L. E.; Rich, A. Acta Crystallogr. 1956, 9, 373 and references cited therein. (b) Bohn, R. K.; Haaland, A. J. Organomet. Chem. 1966, 5, 470. (c) Seiler, P.; Dunitz, J. D. Acta Crystallogr. 1979, B35, 1068. (d) Seiler, P.; Dunitz, J. D. Acta Crystallogr. 1982, B38, 1741. (e) Takusagawa, F.; Koetzle, T. F. Acta Crystallogr. 1979, B35, 1074.
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5h conformer has been found to be more stable in the gas phase by electron diffraction and in the solid state by X-ray or neutron diffraction. See: (a) Dunitz, J. D.; Orgel, L. E.; Rich, A. Acta Crystallogr. 1956, 9, 373 and references cited therein. (b) Bohn, R. K.; Haaland, A. J. Organomet. Chem. 1966, 5, 470. (c) Seiler, P.; Dunitz, J. D. Acta Crystallogr. 1979, B35, 1068. (d) Seiler, P.; Dunitz, J. D. Acta Crystallogr. 1982, B38, 1741. (e) Takusagawa, F.; Koetzle, T. F. Acta Crystallogr. 1979, B35, 1074.
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5h conformer has been found to be more stable in the gas phase by electron diffraction and in the solid state by X-ray or neutron diffraction. See: (a) Dunitz, J. D.; Orgel, L. E.; Rich, A. Acta Crystallogr. 1956, 9, 373 and references cited therein. (b) Bohn, R. K.; Haaland, A. J. Organomet. Chem. 1966, 5, 470. (c) Seiler, P.; Dunitz, J. D. Acta Crystallogr. 1979, B35, 1068. (d) Seiler, P.; Dunitz, J. D. Acta Crystallogr. 1982, B38, 1741. (e) Takusagawa, F.; Koetzle, T. F. Acta Crystallogr. 1979, B35, 1074.
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2 is more stable in both the crystalline and gas phases. See: (a) Cotton, F. A.; Dollase, W. A.; Wood, J. S. J. Am. Chem. Soc. 1963, 85, 1543. (b) Haaland, A. Acta Chem Scand. 1965, 19, 41. (c) Keullen, E.; Jellinck, F. J. Organomet. Chem. 1966, 5, 490. (d) Schaefer, L.; Southern, J. F.; Cyvin, S. J.; Brunvoll, J. J. Organomet. Chem. 1970, 24, 913.
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The Madelung potentials of the crystal field could have a considerable influence on the bond lengths of charged molecules. See, for example: Li, J.; Irle, S.; Schwarz, W. H. E. Inorg. Chem. 1996, 36, 100.
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(a) See, for example: Huheey, J. E.; Keiter, E. A.; Keiter, R. L. Inorganic Chemistry: Principles of Structure and Reactivity, 4th ed.; Harper Collins: New York, 1993; Chapter 14.
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and references therein
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(b) For a recent theoretical analysis of actinide contraction and its comparison with the lanthanide contraction, see: Seth, M.; Dolg, M.; Fulde, P.; Schwerdtfeger, P. J. Am. Chem. Soc. 1995, 117, 6597 and references therein.
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An electron diffraction experiment produces a bigger bent angle, 3.7(9)°: Haaland, A.; Lusztyk, J.; Novak, D. P.; Brunvoll, J.; Starowieyski, K. B. J. Chem. Soc., Chem. Commun. 1974, 54.
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The mass-velocity effect for s-type orbitals is partially cancelled by the Darwin effects. See, for example: Schwarz, W. H. E. In Theoretical Models of Chemical Bonding; Maksić, Z., Ed.; Springer: Berlin, 1990; p 595.
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For qualitative and quantitative discussions of direct and indirect relativistic effects, see, for example: (a) Pitzer, K. S. Acc. Chem. Res. 1979, 12, 271. (b) Pyykkö, P.; Desclaux, J.-P. Acc. Chem. Res. 1979, 12, 276. (c) Pyykkö, P. Chem. Rev. 1988, 88, 563. (d) Schwarz, W. H. E.; van Wezenbeek, E. M.; Baerends, E. J.; Snijders, J. G. J. Phys. 1989, B22, 1515.
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A numerical relativistic Dirac-Fock calculation for the uranium atom indicates that the spin-orbit averaged radii of the maximum radial density are 0.86, 0.56, and 1.30 Å for the 6p, 5f, and 6d orbitals, respectively: Desclaux, J. P. At. Data Nucl. Data Tables 1973, 12, 311.
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0010262728
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Unlike the Hartree-Fock method, in which virtual orbitals are artificially destabilized, in DFT methods, the Kohn-Sham virtual orbitals are generally "too low" in energy, and the addition of an electron to a molecular orbital tends to increase its energy. See: (a) Cook, D. B. Int. J. Quantum Chem. 1996, 60, 793. (b) Slater, J. C.; Mann, J. B.; Wilson, T. M.; Wood, J. H. Phys. Rev. 1969, 184, 672. (c) Slater, J. C. Quantum Theory for Molecules and Solids. The Self-Consistent Field for Molecules and Solids; McGraw-Hill: New York, 1974; Vol. 4.
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36049055044
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Unlike the Hartree-Fock method, in which virtual orbitals are artificially destabilized, in DFT methods, the Kohn-Sham virtual orbitals are generally "too low" in energy, and the addition of an electron to a molecular orbital tends to increase its energy. See: (a) Cook, D. B. Int. J. Quantum Chem. 1996, 60, 793. (b) Slater, J. C.; Mann, J. B.; Wilson, T. M.; Wood, J. H. Phys. Rev. 1969, 184, 672. (c) Slater, J. C. Quantum Theory for Molecules and Solids. The Self-Consistent Field for Molecules and Solids; McGraw-Hill: New York, 1974; Vol. 4.
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0003460779
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McGraw-Hill: New York
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Unlike the Hartree-Fock method, in which virtual orbitals are artificially destabilized, in DFT methods, the Kohn-Sham virtual orbitals are generally "too low" in energy, and the addition of an electron to a molecular orbital tends to increase its energy. See: (a) Cook, D. B. Int. J. Quantum Chem. 1996, 60, 793. (b) Slater, J. C.; Mann, J. B.; Wilson, T. M.; Wood, J. H. Phys. Rev. 1969, 184, 672. (c) Slater, J. C. Quantum Theory for Molecules and Solids. The Self-Consistent Field for Molecules and Solids; McGraw-Hill: New York, 1974; Vol. 4.
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Bursten, B. E.; Rhodes, L. F.; Strittmatter, R. J. J. Am. Chem. Soc. 1989, 111, 2756.
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Bursten, B.E.1
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140
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1842312549
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-
2′ are all ca. 0.30
-
2′ are all ca. 0.30.
-
-
-
-
142
-
-
1842273110
-
-
note
-
e(homo) + 3082, in kcal/mol.
-
-
-
-
143
-
-
1842383781
-
-
note
-
2 molecule are lowered by nearly the same amount. Thus, the effect of spin-orbit coupling on the calculated bond energy is small. We expect that the trend in the bond energies presented in Figure 9 would be qualitatively the same if spin-orbit effects were included.
-
-
-
-
147
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36849131708
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Mulliken, R. S. J. Chem. Phys. 1955, 23, 1833; 1962, 36, 3428.
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