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For recent reviews see: a) M. Kaupp, V. G. Malkin, O. L. Malkina, in The Encyclopedia of Computational Chemistry (Eds.: P. v. R. Schleyer, N. L. Allinger, T. Clark, J. Gasteiger, P. A. Kollman, H. F. Schaefer, III, P. R. Schreiner), Wiley, Chichester, 1998, pp. 1857-1866;
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Sn and I basis sets are constructed from Huzinaga basis functions, contracted and augmented (no f functions have been included in the present work) to [12s 11p 9d]: a) U. Fleischer, unpublished; these basis sets are constructed analogously to those described in:
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Fleischer, U.1
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a) M. J. Frisch, G. W. Trucks, H. B. Schlegel, P. M. W. Gill, B. G. Johnson, M. A. Robb, J. R. Cheeseman, T. Keith, G. A. Petersson, J. A. Montgomery, K. Raghavachari, M. A. Al-Laham, V. G. Zakrzewski, J. V. Ortiz, J. B. Foresman, C. Y. Peng, P. Y. Ayala, W. Chen, M. W. Wong, J. L. Andres, E. S. Replogle, R. Gomperts, R. L. Martin, D. J. Fox, J. S. Binkley, D. J. DeFrees, J. Baker, J. J. P. Stewart, M. Head-Gordon, C. Gonzales, J. A. Pople, Gaussian94, Gaussian, Pittsburgh (PA), 1995;
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0001303258
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c) Compound 14: M. P. Aarnts, M. P. Wilms, K. Peelen, J. Fraanje, K. Goubitz, F. Hartl, D. J. Stufkens, E. J. Baerends, A. Vlcek, Inorg. Chem. 1996, 35, 5468-5477.
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18744407471
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(Eds: K. B. Lipkowitz, D. B. Boyd), VCH, New York
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Inclusion of diffuse functions on I (which could improve the description of this anionic system) has almost no effect on the optimized bond lengths. Scalar relativistic effects are included through the pseudopotentials on the heavier elements, which is usually sufficient (see for instance: G. Frenking, I. Antes, M. Böhme, S. Dapprich, A. W. Ehlers, V. Jonas, A. Neuhaus, M. Otto, R. Stegmann, A. Veldkamp, S. F. Vyboishchikov, in Reviews in Computational Chemistry, Vol. 8 (Eds: K. B. Lipkowitz, D. B. Boyd), VCH, New York, 1996, pp. 63-144).
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Frenking, G.1
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0001684777
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See for instance: Y. Zhang, W. Pan, W. Yang, J. Chem. Phys. 1997, 107, 7921-7925.
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0001305204
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Such effects are apparent e.g. in the thermochemistry of perchloroalkanes: J. Cioslowski, G. Liu, D. Moncrieff, J. Phys. Chem. A 1998, 102, 9965-9969.
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0348185852
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note
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In fact, an unconstrained NLMO search finds no bonds between Ru and I in 4a; rather, an ionic description results, with lone pairs on I containing small contributions (ca. 15%) from the metal. The s(Ru) contributions mentioned in the text are obtained when a Ru-I bonding MO is enforced using the CHOOSE keyword in Gaussian94; in this option, enforced NLMO populations of ca. 40% and 60% are assigned to Ru and I, respectively.
-
-
-
-
68
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-
85085720022
-
-
note
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4 is 31%, with a polarization of the MO towards C (total populations ca. 60% and 40% on C and I, respectively).
-
-
-
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69
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0001124388
-
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The relativistic effects of second-row transition-metal nuclei on their own shielding constants are noticeable, but cancel to a large extent when relative chemical shifts, i.e. shielding differences, are considered (see for instance: G. Schreckenbach, T. Ziegler, Int. J. Quantum. Chem. 1997, 61, 899-918), and can thus be neglected for the purposes of this study.
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0348185849
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-
note
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This value has been obtained by compressing and elongating the optimized Ru-I bonds by Δr = 5 pm each, leaving all other parameters unchanged, and by a linear fit of the resulting three [r,σ(r)] data points. The Ru nucleus becomes deshielded with increasing Ru-I bond lengths.
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81
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82
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In addition to possible shortcomings inherent to the DFT method employed, errors may be introduced by neglect of relativistic effects (which, apparently, amount to just a few percent for nuclei from the 5th period, cf. ref. [54]) and by uncertainties in the experimental nuclear quadrupole moments (see for instance P. Pyykkö, Z. Naturforsch 1992, 47a, 189-196).
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4N]: 1.570(7) Å, 2.310(1) Å, and 104.58(4)° (F. L. Phillips, A. C. Skapski, Acta Crystallogr. 1975, B31, 2667-2670).
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