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Electrodonating and Electroaccepting Powers

The Journal of Physical Chemistry A · 2007 · Vol. 111(10) · pp. 1966–1970
José L. GázquezAndrés CedilloAlberto Vela

Abstract

By introducing an electron bath that represents the chemical environment in which a chemical species is immersed, and by making use of the second-order Taylor series expansions of the energy as a function of the number of electrons in the intervals between N - 1 and N, and N and N + 1, we show that the electrodonating (omega-) and the electroaccepting (omega+) powers may be defined as omega-/+ = (mu-/+)2/2eta-/+, where mu-/+ are the chemical potentials and eta-/+ are the chemical hardnesses, in their corresponding intervals. Approximate expressions for omega- and omega+ in terms of the ionization potential I and the electron affinity A are established by assuming that eta- = eta+ = eta = mu+ - mu-. The functions omega-/+(r) = omega-/+f -/+(r), where f -/+(r) are the directional Fukui functions, derived from a functional Taylor series for the energy functional truncated at second order, represent the local electrodonating and electroaccepting powers.

Electrochemical Analysis and ApplicationsMolecular Junctions and NanostructuresInorganic and Organometallic ChemistryOmegaChemistryElectronOrder (exchange)Taylor seriesSeries (stratigraphy)Energy (signal processing)Function (biology)Atomic physicsMathematical physics
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