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Volumn 6, Issue 17, 2000, Pages 3272-3280

Density-functional computation of 99Ru NMR parameters

Author keywords

Density functional calculations; Electric field gradients; NMR spectroscopy; Quadrupolar relaxation; Ruthenium

Indexed keywords

ORGANOMETALLIC COMPOUND; RUTHENIUM; RUTHENIUM DERIVATIVE;

EID: 0038748863     PISSN: 09476539     EISSN: None     Source Type: Journal    
DOI: 10.1002/1521-3765(20000901)6:17<3272::aid-chem3272>3.0.co;2-e     Document Type: Article
Times cited : (42)

References (88)
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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.
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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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    • 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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    • 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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    • zz and Δσ for the whole set of compounds.
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    • 2O at room temperature (cf. ref. [30a]).
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.