Magnetic oscillations of in-plane conductivity in quasi-two-dimensional metals

We develop the theory of transverse magnetoresistance in layered quasi-two-dimensional (Q2D) metals. Using the Kubo formula and harmonic expansion, we calculate intralayer conductivity in a magnetic field perpendicular to conducting layers. The analytical expressions for the amplitudes and phases of magnetic quantum oscillations (MQO) and of the so-called slow oscillations (SO) are derived and applied to analyze their behavior as a function of several parameters: magnetic field strength, interlayer transfer integral, and Landau-level width. Both the MQO and SO of intralayer and interlayer conductivities have approximately opposite phase in weak magnetic field and the same phase in strong field. The amplitude of SO of intralayer conductivity changes sign at ${\ensuremath{\omega}}_c{\ensuremath{\tau}}₀=\sqrt{3}$. There are several other qualitative differences between magnetic oscillations of in-plane and out-of-plane conductivity. The results obtained are useful to analyze experimental data on magnetoresistance oscillations in various strongly anisotropic Q2D metals.