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The quasi-two-dimensional nature of the charge carriers energy spectrum inlayered conductors leads to specific effects in an external magnetic field. Themagnetoresistance of layered conductors in a wide range of strong magneticfields directed in the plane of the layers can increase proportionally to amagnetic field value. The electromagnetic impedance and the sound attenuationrate depend essentially on the polarization of normal to the layers.Propagation of electromagnetic and acoustic waves in these conductors involvesvirtually all charge carriers in the transfer of acoustic pulses andelectromagnetic field spikes to the bulk of the conductor. The orbits of Fermielectrons in a magnetic field are virtually indistinguishable, which allows theinclusion of large number of conduction electrons in the formation of peculiaroscillatory and resonant effects which are absent in the case of ordinarymetals. Investigation of these effects introduce the possibilities for detailedstudy of the dissipative processes in electron systems of layered conductorsand the charge carriers energy spectrum. Point contact investigations oflayered metals allow us to obtain the information about electron and phononspectra. The electron focusing signal and the point contact spectrum areextremely sensitive to the orientation of the magnetic field vector $\bs{H}$ inrelation to the layers with a high electrical conductivity. The values of$\bs{H}$ for which the electron focusing signal has peaks can be used fordetermining velocities and extremal diameters for the open Fermi surface. Thedependence of the point contact spectra on the magnitude and the relaxation ofelectrons at various types of phonon excitations.

Electron phenomena in layered conductors