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Volumn 26, Issue 3, 2007, Pages 469-471

Tin analogues of alkynes. Multiply bonded structures vs singly bonded structures

Author keywords

[No Author keywords available]

Indexed keywords

CHEMICAL BONDS; ORGANOMETALLICS; TIN COMPOUNDS;

EID: 33847239952     PISSN: 02767333     EISSN: None     Source Type: Journal    
DOI: 10.1021/om060993v     Document Type: Article
Times cited : (39)

References (44)
  • 1
    • 0042736413 scopus 로고    scopus 로고
    • For recent reviews, see: a
    • For recent reviews, see: (a) Power, P. P. Chem. Commun. 2003, 2091.
    • (2003) Chem. Commun , pp. 2091
    • Power, P.P.1
  • 23
  • 26
    • 33847207051 scopus 로고    scopus 로고
    • Gaussian, Inc, Wallingford, CT
    • Gaussian 03, Revision C.01; Gaussian, Inc.: Wallingford, CT, 2004.
    • (2004) Gaussian 03, Revision , Issue.C.01
  • 29
    • 18244396953 scopus 로고    scopus 로고
    • In a donor, acceptor bond model Figure 1, the Sn, Sn bond is regarded as consisting of two dative bonds and one π bond. For example, see refs 2a and 2b as well as recent papers: Lein, M, Krapp, A, Freaking, G. J. Am. Chem. Soc. 2005, 127, 6290
    • In a donor - acceptor bond model (Figure 1), the Sn - Sn bond is regarded as consisting of two dative bonds and one π bond. For example, see refs 2a and 2b as well as recent papers: Lein, M.; Krapp, A.; Freaking, G. J. Am. Chem. Soc. 2005, 127, 6290.
  • 31
    • 33847233534 scopus 로고    scopus 로고
    • An isoenergetic twisted form (Sn, Sn, 2.681Å, B, 126.0°, ω= 163.8°) was also located as a minimum. However, it was calculated at the MP2 level16 that the twisted form is 5.2 kcal/mol less stable than the planar form in Figure 2
    • 16 that the twisted form is 5.2 kcal/mol less stable than the planar form in Figure 2.
  • 32
    • 33644902900 scopus 로고    scopus 로고
    • Because of the size of the molecules, the MP2 calculations were carried out using a high-speed parallel algorithm developed recently. For this algorithm and installation in the GAMESS program, see: Ishimura, K.; Pulay, P.; Nagase, S. J. Comput. Chem. 2006, 27, 407.
    • Because of the size of the molecules, the MP2 calculations were carried out using a high-speed parallel algorithm developed recently. For this algorithm and installation in the GAMESS program, see: Ishimura, K.; Pulay, P.; Nagase, S. J. Comput. Chem. 2006, 27, 407.
  • 33
    • 0001094755 scopus 로고    scopus 로고
    • This is not very surprising, since the planar structure S of RSnSnR corresponds to the transition state for the inversion of the doubly bridged structure when R is small. In this context, see: Chen, Y, Hartmann, M, Diedenhofen, M, Frenking, G. Angew. Chem, Int. Ed. 2001, 40, 2052. As is apparent from Figure 2 of ref 9, the planar structure S of MeSnSnMe is not the global minimum
    • This is not very surprising, since the planar structure S of RSnSnR corresponds to the transition state for the inversion of the doubly bridged structure when R is small. In this context, see: Chen, Y.; Hartmann, M.; Diedenhofen, M.; Frenking, G. Angew. Chem., Int. Ed. 2001, 40, 2052. As is apparent from Figure 2 of ref 9, the planar structure S of MeSnSnMe is not the global minimum.
  • 34
    • 33847207701 scopus 로고    scopus 로고
    • In contrast, it seems that structure M was not considered by Power and coworkers in ref 9.
    • In contrast, it seems that structure M was not considered by Power and coworkers in ref 9.
  • 35
    • 33847194914 scopus 로고    scopus 로고
    • Similar results were also obtained using relativistic effective core potentials
    • Similar results were also obtained using relativistic effective core potentials.
  • 37
    • 33847230472 scopus 로고    scopus 로고
    • The [433111/43111/4] basis set augmented by two d polarization functions (d exponents 0.382 and 0.108) was used for Ge.12 Geometrical parameters optimized for Ar′GeGeAr′ are Ge, Ge, 2.257 Å, θ, 129.4°, and ω, 172.9° for structure M and Ge, Ge, 2.757 Å, θ, 105.2°, and ω, 171.7° for structure S. For Ar′GeGeAr′, structure M is 14.7 kcal/mol more stable than structure S
    • 12 Geometrical parameters optimized for Ar′GeGeAr′ are Ge - Ge = 2.257 Å, θ = 129.4°, and ω = 172.9° for structure M and Ge - Ge = 2.757 Å, θ = 105.2°, and ω = 171.7° for structure S. For Ar′GeGeAr′, structure M is 14.7 kcal/mol more stable than structure S.
  • 38
    • 33847213794 scopus 로고    scopus 로고
    • - anion.
    • - anion.
  • 41
    • 33847205272 scopus 로고    scopus 로고
    • The 6-31G(d) basis set was used for Si.
    • The 6-31G(d) basis set was used for Si.
  • 43
    • 0035897431 scopus 로고    scopus 로고
    • For the effect of packing forces on the structures of Na 2-[Ar*GaGaAr*] and Na2[Ar′GaGaAr′, see ref 2g and Takagi, N, Schmidt, M. W, Nagase, S. Organometallics 2001, 20, 1646
    • 2[Ar′GaGaAr′] , see ref 2g and Takagi, N.; Schmidt, M. W.; Nagase, S. Organometallics 2001, 20, 1646.
  • 44
    • 33847220641 scopus 로고    scopus 로고
    • 3 resemble those of Ar′SnSnAr′, except that Ar*SnSnAr* (ω = 154.7°) is more twisted around the Sn - Sn bond than Ar′SnSnAr′ (ω = 179.7°) for structure M.
    • 3 resemble those of Ar′SnSnAr′, except that Ar*SnSnAr* (ω = 154.7°) is more twisted around the Sn - Sn bond than Ar′SnSnAr′ (ω = 179.7°) for structure M.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.