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Table 1

Summary of radiative transfer simulations in both 1D (upper part) and 2D (lower part).

1D simulations with CMFGEN

Dim. Model Ekin (1050 erg) M(56Ni)core (M) M(56Ni)shell (M)
1D e1ni1 2.0 0.009 0.0
1D e1ni2 2.0 0.050 0.0
1D e1ni1b1 2.0 0.009 0.02
1D e1ni1b2 2.0 0.009 0.05

1D e2ni1 4.0 0.009 0.0
1D e2ni2 4.0 0.050 0.0
1D e2ni1b1 4.0 0.009 0.02
1D e2ni1b2 4.0 0.009 0.05
2D simulations with LONG_POL

Dim. 2D Model Y/e1ni1 Geometrical setup Model Y for | θ | ≲ 28.13°, e1ni1 elsewhere

Dim. Model Y Pcont,max (%) Sign Flip?
50 days Max 300 days
2D e1ni2 0.10 1.03 0.93 Yes
2D e1ni1b1 0.05 1.72 0.81 Weak
2D e1ni1b2 0.09 1.83 1.24 No
2D e2ni1 0.57 1.90 0.21 Marginal
2D e2ni2 0.59 1.86 1.41 Marginal
2D e2ni1b1 0.98 4.06 0.80 Marginal
2D e2ni1b2 1.19 2.71 1.11 No

Notes. The first column lists the dimensionality of the simulation. The 1D spherically symmetric non-LTE time-dependent simulations with CMFGEN are used as initial conditions for the 2D axially symmetric polarized radiative transfer simulations with LONG_POL. The second column lists the model name. The following columns provide some characteristics of each simulation. For the 1D simulations, we list the ejecta kinetic energy and the total mass of 56Ni (it may be present in the core and in an external shell; see Fig. 1). For the 2D simulations, we list the continuum polarization at 50 and 300 days, as well as the maximum value it attained. We also indicate whether the continuum polarization exhibits a sign flip during its evolution from 15 to 300 days. The evolution of the quantity −Qcont, defined as −100FQ/FI, is shown in Fig. B.4. We show the average of this quantity in the spectral region from 6900 to 7200 Å. The full description of these quantities is given in the Appendix A. All 2D simulations adopt mirror symmetry with respect to the equatorial plane.

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