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Fig. 2

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Top to bottom: electron distribution function f(v); the spectral energy density of Langmuir waves W(k); in-source harmonic radio brightness temperature TT(k) (for k/kDe = 0.0225 to 0.0235, corresponding to ω/ωpe = 2 to 2.08); spectral energy density of ion-sound waves WS(k); in-source fundamental radio brightness temperature TT(k) (for k/kDe = 0. to 0.01, corresponding to ω/ωpe = 1 to 1.1) for a collisionally relaxing electron beam in homogeneous plasma (left column) and in inhomogeneous plasma with τD ≃ 0.24 s (right column). Each coloured line shows the distribution at a different time, as shown in the colour bar.

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