Fig. 1.

Two-dimensional density structure (left) for a clumped model set-up over a 90° wedge (in our HERACLES simulations, this wedge straddles the equatorial plane at θ = π/2 and thus extends from θ = π/4 to θ = 3π/4). The black line corresponds to the photosphere. Quantities other than density vary only with radius initially. The plot on the right shows the velocity in units of 1000 km s−1 (V8), the temperature in units of 104 K (T4), the normalized smooth density in the log, the radial variation of clumping (ξ), and the normalized 56Ni distribution versus radius R. The model corresponds to the case of a 20 d old type II-P SN ejecta with the following model parameters: Mej = 12 M⊙, Ekin = 1.2 × 1051 erg, k = 9, Thigh = 50 000 K, Tlow = 100 K, RT = 7 × 1014 cm, ΔRT = 3 × 1014 cm, σcl = 0.02, ξ0 = 0.1, Vcl = 4000 km s−1, ΔVcl = 3000 km s−1, M(56Ni) = 0.05 M⊙, VNi = 2000 s−1, and ΔVNi = 1000 km s−1.
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