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Volumn 105, Issue 2, 2001, Pages 416-425

G- and a-tensor calculations in the zero-order approximation for relativistic effects of Ni complexes Ni(mnt)2- and Ni(CO)3H as model complexes for the active center of [NiFe]-hydrogenase

Author keywords

[No Author keywords available]

Indexed keywords

APPROXIMATION THEORY; CALCULATIONS; COMPLEXATION; COMPUTER SIMULATION; ELECTRONS; ENZYMES; INTEGRATION; MAGNETIC RESONANCE; PROBABILITY DENSITY FUNCTION;

EID: 0035135780     PISSN: 10895639     EISSN: None     Source Type: Journal    
DOI: 10.1021/jp002455g     Document Type: Article
Times cited : (65)

References (64)
  • 36
    • 0003662656 scopus 로고    scopus 로고
    • Theoretical Chemistry, Vrije Universiteit: De Boelelaan 1083, NL-1081 HV Amsterdam, The Netherlands.
    • Amsterdam Density Functional (ADF), Rev. 1999; Theoretical Chemistry, Vrije Universiteit: De Boelelaan 1083, NL-1081 HV Amsterdam, The Netherlands.
    • (1999) Amsterdam Density Functional (ADF), Rev.
  • 49
    • 0000843253 scopus 로고    scopus 로고
    • von Ragué Schleyer, P., Ed.; Wiley and Sons: New York
    • Eriksson, L. A. In Encyclopedia of Computational Chemistry; von Ragué Schleyer, P., Ed.; Wiley and Sons: New York, 1998; pp 952-958.
    • (1998) Encyclopedia of Computational Chemistry , pp. 952-958
    • Eriksson, L.A.1
  • 54
    • 33645920485 scopus 로고    scopus 로고
    • note
    • 61Ni hyperfme interaction (see Table 3).
  • 63
    • 85088715208 scopus 로고    scopus 로고
    • 61Ni) = +69.85 MHz. The difference between spin-polarized SR ZORA and NR BP86 calculations still lies in the different basis sets (STOs vs GTOs) and/or the consideration of scalar-relativistic effects in the ZORA Hamiltonian.
    • 61Ni) = +69.85 MHz. The difference between spin-polarized SR ZORA and NR BP86 calculations still lies in the different basis sets (STOs vs GTOs) and/or the consideration of scalar-relativistic effects in the ZORA Hamiltonian.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.