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Table 1.

Summary of properties for the progenitor, the ejecta, the magnetar, as well as results at bolometric maximum obtained with the CMFGEN simulations.

Model 56Ni Mej Ekin Epm Ppm Bpm V0 dV tpm tpeak Lpeak
(M) (M) (erg) (erg) (ms) (G) (km s−1) (km s−1) (d) (d) (erg s−1)
5p11Bx2th 0.19 3.63 2.49(51) 0.4(51) 7.0 3.5(14) 6000 3000 19.1 26.0 4.83(43)
5p11Bx2 0.19 3.63 2.49(51) 0.4(51) 7.0 3.5(14) 6000 3000 19.1 26.7 4.86(43)

r0e2 0.13 9.69 4.12(51) 0.4(51) 7.0 3.5(14) 5700 2850 19.1 31.7 3.75(43)
r0e2n 0.13 9.69 4.12(51) ... ... ... ... ... ... 44.4 2.25(42)

r0e2 0.13 9.69 4.12(51) 0.4(51) 7.0 3.5(14) 5700 2850 19.1 31.7 3.75(43)
r0e2s 0.13 9.69 4.12(51) 0.4(51) 7.0 3.5(14) 1425 713 19.1 51.7 2.81(43)

r0e1 0.09 9.52 1.14(51) 0.4(51) 7.0 3.5(14) 2700 1350 19.1 43.0 2.53(43)
r0e2 0.13 9.69 4.12(51) 0.4(51) 7.0 3.5(14) 5700 2850 19.1 31.7 3.75(43)
r0e4 0.17 9.86 1.23(52) 0.4(51) 7.0 3.5(14) 10 000 5000 19.1 25.8 4.86(43)

r0e2 0.13 9.69 4.12(51) 0.4(51) 7.0 3.5(14) 5700 2850 19.1 31.7 3.75(43)
r0e2ba 0.13 9.69 4.12(51) 0.4(51) 7.0 1.0(14) 5700 2850 234.4 48.9 1.61(43)

r0e2 0.13 9.69 4.12(51) 0.4(51) 7.0 3.5(14) 5700 2850 19.1 31.7 3.75(43)
r0e2ea 0.13 9.69 4.12(51) 0.8(51) 5.0 3.5(14) 6800 3400 9.6 25.0 7.20(43)
r0e2eb 0.13 9.69 4.12(51) 1.2(51) 4.1 3.5(14) 8000 4000 6.4 21.6 1.03(44)
r0e2ec 0.13 9.69 4.12(51) 5.0(51) 2.0 2.0(14) 8000 4000 4.7 24.6 3.21(44)

Notes. Numbers in parenthesis correspond to powers of ten. Each group of models (separated by a horizontal line) has a specific purpose. Models 5p11Bx2 and 5p11Bx2th address the influence of non-thermal processes. The reference magnetar model r0e2 is confronted to model r0e2n (no magnetar), to model r0e2s (narrow magnetar-power deposition profile), to models r0e1 and r0e4 (different explosion energies), to model r0e2ba (different magnetar field strength), and to models r0e2ea, r0e2eb, and r0e2ec (different magnetar spins). Also discussed is the influence of ejecta clumping for model r0e2 (Sect. 9).

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