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Volumn 696, Issue 8, 2011, Pages 1647-1651

Novel carbonyl iron-bismuth clusters - Synthesis, structure, CO2 insertion and potential as molecular precursors for BiFeO3

Author keywords

BiFeO3; Bismuth alkoxide; Bismuth cluster; CO 2 insertion; Iron carbonyl

Indexed keywords

BIFEO3; CARBONYL IRON; CLUSTER CORES; CO 2 INSERTION; CORE STRUCTURE; H NMR SPECTROSCOPY; IRON CARBONYL; IRON CLUSTER; MOLECULAR PRECURSOR; MULTIFERROICS; SINGLE CRYSTAL X-RAY DIFFRACTION; STARTING MATERIALS;

EID: 79953652356     PISSN: 0022328X     EISSN: None     Source Type: Journal    
DOI: 10.1016/j.jorganchem.2011.01.028     Document Type: Article
Times cited : (15)

References (50)
  • 39
    • 79953667164 scopus 로고    scopus 로고
    • The geometry optimization has been carried out using the Turbomole program package
    • The geometry optimization has been carried out using the Turbomole program package:
  • 42
    • 36449007808 scopus 로고
    • For the NBO Analysis the B3-LYP functional and the Ahlrichs VTZ basis (using the Stuttgard RLC ECP (W. Kühle, M. Dolg, H. Stoll, and H. Preuss J. Chem. Phys. 100 1994 7535 ) for Bi) have been used as supplied in the NWChem package
    • (1994) J. Chem. Phys. , vol.100 , pp. 7535
    • Kühle, W.1    Dolg, M.2    Stoll, H.3    Preuss, H.4
  • 43
    • 0011083499 scopus 로고
    • The NBO analysis has been carried out using the NBO package (A.E. Reed, L.A. Curtiss, and F. Weinhold Chem. Rev. 88 1988 899 ) as interfaced to NWChem (NWChem, A Computational Chemistry Package for Parallel Computers, Version 5.1; Pacific Northwest National Laboratory: Richland, WA, 2007)
    • (1988) Chem. Rev. , vol.88 , pp. 899
    • Reed, A.E.1    Curtiss, L.A.2    Weinhold, F.3
  • 50
    • 79953655936 scopus 로고    scopus 로고
    • -3). Acoording to W. Massa (Kristallstrukturbestimmung, Teubner Studienbücher, Stuttgart, 1996) and W. Clegg (Crystal Structure Determination, Oxford University Press, 1998) this might be observed for heavy atoms for which remaining density peaks with ca. 10% of the electron density of the heavy atom are expected at distances between 0.6 and 1.2 Å. In addition, these unrefined electron density peaks might be attributed to large absorption effects. Repeated measurements of 1 with Mo-Kα radiation, however, did not give satisfying results as the number of observed reflections was always ca. 30% only
    • -3). Acoording to W. Massa (Kristallstrukturbestimmung, Teubner Studienbücher, Stuttgart, 1996) and W. Clegg (Crystal Structure Determination, Oxford University Press, 1998) this might be observed for heavy atoms for which remaining density peaks with ca. 10% of the electron density of the heavy atom are expected at distances between 0.6 and 1.2. In addition, these unrefined electron density peaks might be attributed to large absorption effects. Repeated measurements of 1 with Mo-Kα radiation, however, did not give satisfying results as the number of observed reflections was always ca. 30% only.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.