Nonlinear mode coupling theory of the lower-hybrid-drift instability

Abstract

A nonlinear mode coupling theory of the lower‐hybrid‐drift instability is presented. A two‐dimensional nonlinear wave equation is derived which describes lower‐hybrid‐drift wave turbulence in the plane transverse to B (k⋅B=0), and which is valid for finite β, collisional and collisionless plasmas. The instability saturates by transferring energy from growing, long wavelength modes to damped, short wavelength modes. Detailed numerical results are presented which compare favorably to both recent computer simulations and experimental observations. Applications of this theory to space plasmas, the earth’s magnetotail, and the equatorial F region ionosphere are discussed.