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The first calculation (LARGE-I) employed the Wachters basis on iron as before; however, the aug-TZVPP basis was applied to the oxo-oxygen and the TZVPP basis to the remaining heavy atoms. The hydrogens were described with the TZVP basis. The second calculation (LARGE-II) replaced the Wachters basis with a quadruple-ζ basis from the TurboMole library (Weigend F.; Furche, F.; Ahlrichs, R. J. Chem. Phys. 2003, 119, 12753). In addition, a second set of polarizing p-functions were added to the hydrogens. All polarization exponents were taken from the TurboMole library accessible at ftp://ftp.chemie.uni- karlsruhe.de/pub/basen (March 2005).
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The first calculation (LARGE-I) employed the Wachters basis on iron as before; however, the aug-TZVPP basis was applied to the oxo-oxygen and the TZVPP basis to the remaining heavy atoms. The hydrogens were described with the TZVP basis. The second calculation (LARGE-II) replaced the Wachters basis with a quadruple-ζ basis from the TurboMole library (Weigend F.; Furche, F.; Ahlrichs, R. J. Chem. Phys. 2003, 119, 12753). In addition, a second set of polarizing p-functions were added to the hydrogens. All polarization exponents were taken from the TurboMole library accessible at ftp://ftp.chemie.uni- karlsruhe.de/pub/basen (March 2005).
-
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75
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17744396270
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note
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6 were variationally treated. At this level, the quintet state is predicted to be 0.14 eV lower than the triplet state.
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-1, respectively. It is evident that the splitting is a sensitive function of the selection threshold and requires tight values for convergence.
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0033652655
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∥). Experimentally, this species shows g-values that depend markedly on the environment of the radical and vary between 2.004 and 2.01 and thus confirm our statement. See, for example: (a) Dave, P. C.; Srivinas, D. J. Porphyrins Phthalocyanines 2000, 4, 192. (b) Dave, P. C.; Srivinas, D. J. Porphyrins Phthalocyanines 1997, 2, 243 and references therein.
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∥). Experimentally, this species shows g-values that depend markedly on the environment of the radical and vary between 2.004 and 2.01 and thus confirm our statement. See, for example: (a) Dave, P. C.; Srivinas, D. J. Porphyrins Phthalocyanines 2000, 4, 192. (b) Dave, P. C.; Srivinas, D. J. Porphyrins Phthalocyanines 1997, 2, 243 and references therein.
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17744371417
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note
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Judging from the results obtained for 4 and 5, this prediction should be viewed with some caution.
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95
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17744362627
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This should not be confused with the spin contamination present in spin-unrestricted Hartree-Fock or DFT calculations. The mixing of different spin states is brought about by the SOC which is parametrized through the ZFS tensor in the spin-Hamiltonian treatment. Thus, this mixing represents a real physical effect and not an artifact of a computational method.
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96
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