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64849087550
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Note that the different appearance of the contour levels around bromine in parts a and b of Figure 5 is due to the noncoplanarity of the two molecular modules. The two parts are in fact plotted in different molecular planes
-
Note that the different appearance of the contour levels around bromine in parts a and b of Figure 5 is due to the noncoplanarity of the two molecular modules. The two parts are in fact plotted in different molecular planes.
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The values of molecular charge reported here and in Table 8 refer in all cases to full molecules, but integration of course has been done on only the independent half molecule.
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The values of molecular charge reported here and in Table 8 refer in all cases to full molecules, but integration of course has been done on only the independent half molecule.
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63
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Note that there is not an equal and opposite charge on dimer B, which in fact lacks 1.04(2) e (0.52(2) e on the asymmetric unit), owing to the error connected to the integration procedure (see section 2 (Methods: Evaluation of Atomic Charges).
-
Note that there is not an equal and opposite charge on dimer B, which in fact lacks 1.04(2) e (0.52(2) e on the asymmetric unit), owing to the error connected to the integration procedure (see section 2 (Methods: Evaluation of Atomic Charges).
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64
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2 to the other one prompted us to perform further multipole refinements of this structure where the core and the spherical valence populations of each atom of a dimer were constrained to be equal to those of the corresponding atoms of the other dimer of the asymmetric unit. This refinement did not imply any significant variation in the topological properties at BCPs and, obviously, no charge transfer between dimers has been obtained. In this case, charge transfer within each dimer was virtually zero.
-
2 to the other one prompted us to perform further multipole refinements of this structure where the core and the spherical valence populations of each atom of a dimer were constrained to be equal to those of the corresponding atoms of the other dimer of the asymmetric unit. This refinement did not imply any significant variation in the topological properties at BCPs and, obviously, no charge transfer between dimers has been obtained. In this case, charge transfer within each dimer was virtually zero.
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