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Then, it is observed that there is displacement of electron shell against positive nucleus.
By electronic exchange, Fe2 + ↔ Fe3 + + e−, one obtains the local displacement of electron in the direction of the applied electric field.
That can be a result of electrostatic interactions between lithium cations Li+ and the macromolecular chain of DEG-1 with forming of coordinative complexes, which are accompanied by displacement of electron density of the oxygen atoms and their partial polarization.
This can be a result of the electrostatic interactions between lithium cations Li+ and the macromolecular r chain of DEG with immediate forming of coordinative complexes, such as {ether oxygen-lithium cations-ether oxygen} (Figure 2), which are accompanied by displacement of electron density of the oxygen atoms and their partial polarization [5, 21, 25].
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The increase of the low dielectric constant is provided due to the influence of the electronic exchange that occurs in ferrite as a result of local displacement of electrons in the direction of the applied electric field Fe 2 + ⇔ Fe 3 + [5].
Thus, the strong growth of the dielectric constant at low frequencies is caused mainly by two mechanisms, namely dipole-orientation caused by local displacement of electrons under the influence of the applied field and in between one.
The electron exchange Fe2+ ↔ Fe3+ results in a local displacement of electrons in the direction of applied electric field which determines the extent of polarization so as the dielectric constants of ferrites.
In the applied electric field, the displacement of an electron from the atom nucleus causes electronic polarization, while the increase of the ionic separation between positive and negative ions in the ion type of connection provides ionic polarization.
This convergence semi-angle is ~16 mrad, resulting in the displacement of the electron trajectory from the straight-line path by ~2.5 nm at the exit of the groove (under the assumption that the focus point of the beam is at the front plane of the groove).
The existence of the quantum capacitance is due to the displacement of the electron wave function at the CNT insulator interface.
The appearance of the O 1s peak at lower energy is due to the effects of TiO2 and ZrO2 with a large displacement of the electron density to the O atoms than that in silica.
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