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35848942032
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An additional geometry optimization on the μ3-1,1,2-O 22--bridged PI structure was performed with a larger basis set, with triple-ζ 6-311G* on Cu and coordinated N/O atoms and 6-31G* on the rest, to verify that the structures obtained in this study with the double-ζ quality basis set, with 6-31G* on Cu and coordinated N/O atoms and 3-21G* on the rest, are sound. As a result, it is found that the overall structure of PI remains the same and the geometric parameters are very similar to those obtained with the double-ζ basis set, as indicated in Table 1
-
2--bridged PI structure was performed with a larger basis set, with triple-ζ 6-311G* on Cu and coordinated N/O atoms and 6-31G* on the rest, to verify that the structures obtained in this study with the double-ζ quality basis set, with 6-31G* on Cu and coordinated N/O atoms and 3-21G* on the rest, are sound. As a result, it is found that the overall structure of PI remains the same and the geometric parameters are very similar to those obtained with the double-ζ basis set, as indicated in Table 1.
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35848942711
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These energies are based on calculations using B3LYP functional with 6-3IG* basis set on Cu and coordinated N/O atoms and 3-21G* basis set on the rest.
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These energies are based on calculations using B3LYP functional with 6-3IG* basis set on Cu and coordinated N/O atoms and 3-21G* basis set on the rest.
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35848946905
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-1).
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-1).
-
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56
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35848931785
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-1) quenches the fluorescence in this region, allowing the resonance Raman spectrum to be obtained.
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-1) quenches the fluorescence in this region, allowing the resonance Raman spectrum to be obtained.
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57
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35848942923
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Unpublished results
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Unpublished results.
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58
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35848947327
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To compare the energy difference between the direct proton transfer from a proton donor to a proton acceptor and the indirect proton transfer via a water molecule, we have modeled the proton-transfer process between a formate ion and a formic acid at the B3LYP/6-31++G** level. As a result, energy barriers for the proton-transfer process directly between a formate and a formic acid and that mediated by a water molecule were estimated with relatively similar values of ∼7.9 and ∼12.0 kcal/mol, respectively, The distance between O atoms accepting and donating the proton was fixed at 2.80 Å. See Figures S2, S3 and figure legends for details of the calculations
-
To compare the energy difference between the direct proton transfer from a proton donor to a proton acceptor and the indirect proton transfer via a water molecule, we have modeled the proton-transfer process between a formate ion and a formic acid at the B3LYP/6-31++G** level. As a result, energy barriers for the proton-transfer process directly between a formate and a formic acid and that mediated by a water molecule were estimated with relatively similar values of ∼7.9 and ∼12.0 kcal/mol, respectively. (The distance between O atoms accepting and donating the proton was fixed at 2.80 Å. See Figures S2, S3 and figure legends for details of the calculations.)
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59
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35848950110
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Note that three possible broken-symmetry states, with |βαα, αβα, and |ααβ) spin configurations, have very similar energies and contribute equivalently to the spin-frustrated ground state of NI.28 Thus, while the |βαα) spin configuration contributes significantly in me early stage of O-O bond cleavage which includes the transition state, vide infra, the other two spin configurations become equally important as all three Cu centers in the trinuclear cluster become oxidized
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28 Thus, while the |βαα) spin configuration contributes significantly in me early stage of O-O bond cleavage (which includes the transition state, vide infra), the other two spin configurations become equally important as all three Cu centers in the trinuclear cluster become oxidized.
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60
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As indicated in footnote 58, the energy barrier in the proton-transfer process is estimated to be higher when it is mediated by a water molecule. However, the relative stability of PI+e+H, compared to that of PI+e, can provide enough thermodynamic driving force to make the energy barrier in the proton-transfer process still small relative to the overall transition-state energy.
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As indicated in footnote 58, the energy barrier in the proton-transfer process is estimated to be higher when it is mediated by a water molecule. However, the relative stability of PI+e+H, compared to that of PI+e, can provide enough thermodynamic driving force to make the energy barrier in the proton-transfer process still small relative to the overall transition-state energy.
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61
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