“…However, there is no spectral gap on the whole space, so one can study the linearized operator in Fourier space with fixed spatial frequency ξ in order to construct a projector Π satisfying (22). Furthermore, the splitting (22) allows to develop a Cauchy theory near an equilibrium, but in the context of asymptotic analysis, that is to say when Λ and thus Σ(Λ), Π, σ depend on a small parameter ε, one also needs to know their behavior as ε goes to zero (see for instance [2,8,9,10]). This is why we perform a precise study of the spectrum for |ξ| 1, and the diffusive limit of the Boltzmann equation requires a second order expansion of the eigenvalues.…”