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70349240543
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int) is the difference between the energy of the complex (ML) and that of the constituting metal and ligand fragments (M and L), computed employing the frozen geometry of the complex. A stronger metal-ligand interaction corresponds to a more negative interaction energy value
-
int) is the difference between the energy of the complex (ML) and that of the constituting metal and ligand fragments (M and L), computed employing the frozen geometry of the complex. A stronger metal-ligand interaction corresponds to a more negative interaction energy value.
-
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-
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17
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70349254238
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int, -288 and -293 kJ mol(1, respectively). More details can be found in the Supporting Information (Table S2)
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int, -288 and -293 kJ mol(1, respectively). More details can be found in the Supporting Information (Table S2).
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18
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70349241852
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In the previous study it was shown that the position of the reduction peaks is well rationalized in terms of Hammett constants of the diazine substituents, giving a neat linear relationship with a rather high slope, on which the novel data here acquired nicely fit (Figure S1, Supporting Information)
-
In the previous study it was shown that the position of the reduction peaks is well rationalized in terms of Hammett constants of the diazine substituents, giving a neat linear relationship with a rather high slope, on which the novel data here acquired nicely fit (Figure S1, Supporting Information).
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21
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70349257480
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In particular, the dEp/dlog v slopes (Table S1, Supporting Information) are small but significant and the half-peak widths are higher than the expected 30 mV
-
In particular, the dEp/dlog v slopes (Table S1, Supporting Information) are small but significant and the half-peak widths are higher than the expected 30 mV.
-
-
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24
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70349255844
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s for 1) and all the transitions described are indeed symmetry allowed. A list of all the excitations contributing to the bands discussed in the paper for compound 0, 1, and 4 are reported in the Supporting Information (Table S3), along with their description in terms of singly excited configurations. Both gas-phase and solution values are reported
-
s for 1) and all the transitions described are indeed symmetry allowed. A list of all the excitations contributing to the bands discussed in the paper for compound 0, 1, and 4 are reported in the Supporting Information (Table S3), along with their description in terms of singly excited configurations. Both gas-phase and solution values are reported.
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The data for this compound have already been published [6] and are reported here for comparison
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