ABSTRACT
Electronic transport properties of conventional metals and semi-
conductors are described in terms of quasiparticle excitations,
electrons, and holes. Simple analytical models of Fermi gas and
Fermi liquid provide an illustrative depiction of various electronic
phenomena, and they also allow a deeper understanding the
properties of composite systems in terms of elementary excitations
(Abrikosov 1988). They include transport in the inhomogeneous
structures, like tunneling junctions and constrictions (Wolf 2012),
and also account for influence the external DC magnetic (Ando and
Seri 1997, Arimura and Ando 2012) and AC electromagnetic fields
(Shafranjuk 2009, Shafranjuk 2011) on the electron transport of
charged particles in the conducting materials.
