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Fig. 4


Variation of the imaginary part of the frequency (ω) for pseudo-body (—) and n = 1 (⋅ ⋅) body mode with respect to dimensionless wave-number, kz0. We fix the wavenumber at k = 5 × 10−6 m−1 with the slabwidth varying. For each separate diagram the background flow speed has been taken to be u0 = 16.0 km s−1 and u0 = 28.0 km s−1, respectively. Panels a and b correspond to ρr = 0.01, while panels c and d to ρr = 0.02. All panels ad use a viscosity coefficient of ν = 1010 m2 s−1. Black lines denote an ionisation degree of μ = 0.5, red and blue lines correspond to μ = 0.75 and μ = 0.95, respectively.

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