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We show how the linearized equations of motion of any dissipative current are determined by the analytical structure of the associated retarded Green's function.
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Even though we only show terms up to order 𝒪 ( Kn 3 ) \mathcal{O}\left(\mathrm{Kn}^{3}\right) in Eq. ( 21
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Note that this result was derived using a different metric signature, i.e., η μ ν = diag ( − , + , + , + ) \eta_{\mu\nu}=\mathrm{diag}\,(-,+,+,+) . See Ref. [ 15 ] for details
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