Relaxation of weakly collisional plasma: continuous spectra, Landau eigenmodes, and transition from the collisionless to the fluid limit

The relaxation of a weakly collisional plasma is described by the Boltzmann-Poisson equations with the Lenard-Bernstein collision operator. We perform a perturbative analysis of these equations, and obtain, for the first time, exact analytic solutions, enabling definitive resolutions to long-standing controversies regarding the impact of weak collisions on continuous spectra and Landau eigenmodes. Unlike some previous studies, we retain both damping and diffusion terms in the collision operator. We find that the linear response is a temporal convolution of a continuum that depends on the continuous velocities of particles, and discrete normal modes that encapsulate coherent oscillations. The normal modes are exponentially damped over time due to collective effects (Landau damping) as well as collisional dissipation. The continuum is also damped by collisions but somewhat differently. Up to a collision time, which is the inverse of the collision frequency ν_c, the continuum decay is driven by velocity diffusion and occurs super-exponentially over a timescale ∼ν^-1/3_c. After a collision time, however, the continuum decay is driven by the collisional damping of particle velocities and diffusion of their positions, and occurs exponentially over a timescale ∼ν_c. This hitherto unknown, slow exponential decay causes perturbations to damp the most on scales comparable to the mean free path, but very slowly on larger scales, which establishes the local thermal equilibrium, the essence of the fluid limit. The long-term decay of the response is driven by the normal modes on scales smaller than the mean free path, but, on larger scales, is governed by the slowly decaying continuum and the least damped normal mode. Our analysis firmly establishes a long-sought connection between the collisionless and fluid limits of weakly collisional plasmas.