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The stationary point for 6 turned out be a transition state; we discuss it here because it has the same orientations of the OR groups as in 2a. The true minimum with an additional intramolecular H bridge is 0.65 kcal/mol lower in energy and it has a δ = -630.
-
The stationary point for 6 turned out be a transition state; we discuss it here because it has the same orientations of the OR groups as in 2a. The true minimum with an additional intramolecular H bridge is 0.65 kcal/mol lower in energy and it has a δ = -630.
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In each case, the mean values over the entire trajectories correspond closely to the mean values over the snapshots selected for the NMR computations
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According to TDDFT computations at the B3LYP/AE1+ level, the lowest excited state in 9 (at λ, 720 nm) can to a large extent be described as a HOMO-LUMO transition. Despite the known deficiencies of TDDFT for charge-transfer states (see, e.g, Dreuw, A, Head-Gordon, M. J. Am. Chem. Soc. 2004, 126, 4007, this number compares reasonably well to experiment, λ, 870 nm ref 2, A much higher excitation energy, corresponding to λ, 552 nm, is predicted for the innocent complex 11
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According to TDDFT computations at the B3LYP/AE1+ level, the lowest excited state in 9 (at λ = 720 nm) can to a large extent be described as a HOMO-LUMO transition. Despite the known deficiencies of TDDFT for charge-transfer states (see, e.g., Dreuw, A.; Head-Gordon, M. J. Am. Chem. Soc. 2004, 126, 4007), this number compares reasonably well to experiment, λ = 870 nm (ref 2). A much higher excitation energy, corresponding to λ = 552 nm, is predicted for the innocent complex 11.
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69
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We have also looked at other systems related to 9 and 11 that contained different tridendate ligands and/or alkyl-substituted catechols and which afforded results very similar to the ones reported here
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We have also looked at other systems related to 9 and 11 that contained different tridendate ligands and/or alkyl-substituted catechols and which afforded results very similar to the ones reported here.
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70
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For pictorial rationalizations of such paramagnetic contributions in transition-metal complexes see, e.g, a Berger, S, Bock, W, Frenking, G, Jonas, V, Müller, V. J. Am. Chem. Soc. 1995, 117, 3820
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For pictorial rationalizations of such paramagnetic contributions in transition-metal complexes see, e.g.: (a) Berger, S.; Bock, W.; Frenking, G.; Jonas, V.; Müller, V. J. Am. Chem. Soc. 1995, 117, 3820.
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Ruiz-Morales, Y.; Ziegler, T. J. Phys. Chem. A 1998, 102, 3970. Unfortunately, the Gaussian program employed in the present study does not allow for a detailed analysis of such individual MO contributions.
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(b) Ruiz-Morales, Y.; Ziegler, T. J. Phys. Chem. A 1998, 102, 3970. Unfortunately, the Gaussian program employed in the present study does not allow for a detailed analysis of such individual MO contributions.
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51V) value of, e.g., 9, closer to experiment, the overall performance for a larger set of normal vanadium complexes deteriorates significantly (Geethalakshmi, K. R.; Bühl, M. unpublished results).
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51V) value of, e.g., 9, closer to experiment, the overall performance for a larger set of normal vanadium complexes deteriorates significantly (Geethalakshmi, K. R.; Bühl, M. unpublished results).
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Such an extensive validation is beyond the scope of this study. In context with the catechol complexes scrutinized here, we verified that one of the more deshielded compounds included in Figure 5 (VO-(SALIMH)DBC with δobs, 600 ppm, cf. entry 2 in Table S4 in the Supporting Information) still has a singlet ground state at the B3LYP level (the ΔES-T values (in eV) are +1.14/+0.34/-0.63 at BP/B3LYP/ BHandH, respectively, i.e, somewhat lower than those of compound 9 in Table 4, If a triplet ground state would have been predicted with B3LYP erroneously, because the 51V NMR spectrum can be recorded, then the amount of HF exchange would certainly have to be reduced below the 20% contained in the standard version of this functional, down to a value at which a singlet ground state would be obtained
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51V NMR spectrum can be recorded), then the amount of HF exchange would certainly have to be reduced below the 20% contained in the standard version of this functional, down to a value at which a singlet ground state would be obtained.
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Even though such single-reference BS solutions do not provide an appropriate description of the true open-shell wavefunction, they can be used to estimate magnetic exchange couplings in transition-metal complexes, cf: (a) Noodleman, L. J. Chem. Phys. 1981, 74, 5737
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Even though such single-reference BS solutions do not provide an appropriate description of the true open-shell wavefunction, they can be used to estimate magnetic exchange couplings in transition-metal complexes, cf: (a) Noodleman, L. J. Chem. Phys. 1981, 74, 5737.
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For a recent review see: b
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For a recent review see: (b) Ciofini, I.; Daul, C. Coord. Chem. Rev. 2003, 238-239, 187.
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Coord. Chem. Rev
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Ciofini, I.1
Daul, C.2
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In that case, the observed resonances should shift strongly with temperature. To our knowledge, no such temperature-dependent NMR studies have been performed yet for the complexes in question. Admixture of paramagnetic states should also lead to substantial line broadening, and indeed, very broad lines (half-width 2-4 kHz) have been reported for some of the catchol complexes in ref 2.
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In that case, the observed resonances should shift strongly with temperature. To our knowledge, no such temperature-dependent NMR studies have been performed yet for the complexes in question. Admixture of paramagnetic states should also lead to substantial line broadening, and indeed, very broad lines (half-width 2-4 kHz) have been reported for some of the catchol complexes in ref 2.
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80
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34247562867
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Kaupp, M, Bühl, M, Malkin, V. G, Eds, Wiley-VCH: Weinheim, Germany
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Moon, S.; Patchkovskii, S. In Calculation of NMR and EPR Parameters. Theory and Applications; Kaupp, M.; Bühl, M.; Malkin, V. G., Eds.; Wiley-VCH: Weinheim, Germany, 2004; p 325.
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Calculation of NMR and EPR Parameters. Theory and Applications
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Moon, S.1
Patchkovskii, S.2
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Hrobarik, P.; Reviakine, R.; Arbuznikov, A. V.; Malkina, O. L.; Malkin, V. G.; Köhler, F. H.; Kaupp, M. J. Chem. Phys. 2007, 126, 024107.
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Hrobarik, P.1
Reviakine, R.2
Arbuznikov, A.V.3
Malkina, O.L.4
Malkin, V.G.5
Köhler, F.H.6
Kaupp, M.7
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It cannot be excluded, however, that the good performance of the restricted B3LYP method in systems with an unstable closed-shell wavefunction is to some extent fortuitous.
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It cannot be excluded, however, that the good performance of the restricted B3LYP method in systems with an unstable closed-shell wavefunction is to some extent fortuitous.
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