Applied-Field Effects on Benzene Transmission
Abstract
By expressing the discrete Schrodinger equation as a second-order finite-difference equation with constant coefficients, the renormalization equations for substituted benzene dimers are derived via the cn-coefficient elimination procedure. On subjecting the benzene molecule to a linear applied field, the resulting field-modified site energies are obtained, by projecting the site-energy locations onto a corresponding benzene dimer axis. Incorporating these modified site energies into the Lippmann-Schwinger scattering theory, enables the field effect to manifest itself in the substituted benzene electron transmission spectral function T(E). Variations in the T(E) energy spectra, arising from increases in the applied field gradient f, are described for each substituted benzene, and comparison made between their various patterns' behaviours. A common feature of the T(E) curves is their shifts to lower energies, as f increases to a calculated limiting value.