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For atoms, single bonds and molecules electron displacement is characterized by electronic potential, absolute hardness, electronegativity and electron gap.
In addition, dissociation, bonding, atomization, formation, ionization, affinity and lattice enthalpies are required to quantify the electron displacement in solids.
The space charge polarization resulting from electron displacement on application of electric field and the subsequent charge build up at the insulating grain boundary is a major contributor to the dielectric constant in ferrites.
In this review the foundations of different acid-base parameters relating to electron displacement within and between (probe) molecules, liquids and (semiconducting) solids are thoroughly investigated and their mutual relationships are evaluated.
Electron displacement due to interaction between (probe) molecules, liquids and solids are characterized by parameters such as Hamaker constant, solubility parameter, exchange energy density, surface tension, work of adhesion and immersion.
Similar(54)
The light energy released is derived from electron displacements within the crystal lattice of such a substance caused by previous exposure to high-energy radiation.
The effect of substituents on the acid base properties of organic molecules has been very extensively studied and is one of the main methods of investigating the nature of the electron displacements produced by substitution in these molecules.
Specific dipolar, acid-base and charge interactions involve electron displacements.
The charge-induced electron "plate" displacement is calculated variationally within the density functional formalism.
It was possible to recognize electron density displacement in barbituric acid molecule towards those two resonant forms, which influence the type of hydrogen bonds formed in each polymorphic form and therefore results in different packing topology.
The consequence is that the ultraclean harmonic motion (electron orbit center displacement) behaves as if the electrons were driven by the radiation of half frequency.
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