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Although the spectrum of sodide in Fig. appears to show a diat ∼2.2 eV between the optically bright -like states and the higher-lying states, we do not believe that this diis a genuine feature as indicated by the overlapping error bars in the diregion and "peak" at 2.5 eV.
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Although the spectrum of sodide in Fig. appears to show a dip at ∼2.2 eV between the optically bright p -like states and the higher-lying states, we do not believe that this dip is a genuine feature as indicated by the overlapping error bars in the dip region and "peak" at 2.5 eV.
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The computational cost of evaluating Eq. limited us to calculating average projections for only the s,and d SHs.
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The computational cost of evaluating Eq. limited us to calculating average projections for only the s,p and d SHs.
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The VBE is defined relative to the vacuum level. Although it would be useful to also know the location of the solvent conduction band relative to the vacuum, determining the precise onset of the conduction band is complicated by the presence of solvent-supported disjoint electronic states below THF's conduction band (Refs.). As we show in Sec., our calculations reveal that these disjoint states mix with sodide's CTTS states, suggesting that the conduction band lies higher in energy than our calculated CTTS states.
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The VBE is defined relative to the vacuum level. Although it would be useful to also know the location of the solvent conduction band relative to the vacuum, determining the precise onset of the conduction band is complicated by the presence of solvent-supported disjoint electronic states below THF's conduction band (Refs.). As we show in Sec., our calculations reveal that these disjoint states mix with sodide's CTTS states, suggesting that the conduction band lies higher in energy than our calculated CTTS states.
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The smoothing Gaussian width was chosen by considering the largest reciprocal-space vector supported by a Fourier-grid of N=24 in a simulation cell of 32.5 Å [the simulation parameters used in previous THF studies (Refs.)].
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The smoothing Gaussian width was chosen by considering the largest reciprocal-space vector supported by a Fourier-grid of N=24 in a simulation cell of 32.5 Å [the simulation parameters used in previous THF studies (Refs.)].
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Although the Mulliken charges on the THF sites differ from the partial charges used in the OPLS model (Ref.), the dipole moments resulting from both sets of charges agree to within 2%.
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Although the Mulliken charges on the THF sites differ from the partial charges used in the OPLS model (Ref.), the dipole moments resulting from both sets of charges agree to within 2%.
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