Table 1.

|$M_{\rm ZAMS}$| ranges of PISN progenitors, for representative metallicities, obtained with the parsec-i, parsec-ii, and franec stellar evolution tracks. The ranges at metallicities in between the original ones from the stellar tracks are obtained via interpolation, as described in the text. All values are in solar units. Blanks indicate cases with no PISN, at |$Z\gt Z_{\rm max}$|⁠. Masses |$\gt 300\:\mathrm{ M}_{\rm \odot }$| are fixed to |$300\:\mathrm{ M}_{\rm \odot }$|⁠, that is, the highest |$M_{\rm up}$| considered in this work (see Appendix  B for an additional variation with |$M_{\rm up}=600\:\mathrm{ M}_{\rm \odot }$|⁠). The double intervals at |$Z=1\times 10^{-4}$| of parsec-ii are due to the non-monotonicity of the corresponding stellar track, which exits the PISN mass range and then re-enters again (see fig. 8 of Iorio et al. 2022).

graphic1 × 10−41 × 10−34 × 10−38 × 10−31 × 10−22 × 10−2
parsec-i
45–120108–257109–300158–300178–222
55–110126–237128–300195–300
60–105138–228139–300213–300
parsec-ii
45–120107–229112–23992–221111–294133–300
55–110117–150130–227109–202138–270166–300
153–211
60–105125–145140–221118–193151–258182–300-
158–203

franec
45–120111–262113–272136–300183–300220–300
55–110131–242134–251173–300233–300282–300
60–105141–232145–240192–300259–300
graphic1 × 10−41 × 10−34 × 10−38 × 10−31 × 10−22 × 10−2
parsec-i
45–120108–257109–300158–300178–222
55–110126–237128–300195–300
60–105138–228139–300213–300
parsec-ii
45–120107–229112–23992–221111–294133–300
55–110117–150130–227109–202138–270166–300
153–211
60–105125–145140–221118–193151–258182–300-
158–203

franec
45–120111–262113–272136–300183–300220–300
55–110131–242134–251173–300233–300282–300
60–105141–232145–240192–300259–300
Table 1.

|$M_{\rm ZAMS}$| ranges of PISN progenitors, for representative metallicities, obtained with the parsec-i, parsec-ii, and franec stellar evolution tracks. The ranges at metallicities in between the original ones from the stellar tracks are obtained via interpolation, as described in the text. All values are in solar units. Blanks indicate cases with no PISN, at |$Z\gt Z_{\rm max}$|⁠. Masses |$\gt 300\:\mathrm{ M}_{\rm \odot }$| are fixed to |$300\:\mathrm{ M}_{\rm \odot }$|⁠, that is, the highest |$M_{\rm up}$| considered in this work (see Appendix  B for an additional variation with |$M_{\rm up}=600\:\mathrm{ M}_{\rm \odot }$|⁠). The double intervals at |$Z=1\times 10^{-4}$| of parsec-ii are due to the non-monotonicity of the corresponding stellar track, which exits the PISN mass range and then re-enters again (see fig. 8 of Iorio et al. 2022).

graphic1 × 10−41 × 10−34 × 10−38 × 10−31 × 10−22 × 10−2
parsec-i
45–120108–257109–300158–300178–222
55–110126–237128–300195–300
60–105138–228139–300213–300
parsec-ii
45–120107–229112–23992–221111–294133–300
55–110117–150130–227109–202138–270166–300
153–211
60–105125–145140–221118–193151–258182–300-
158–203

franec
45–120111–262113–272136–300183–300220–300
55–110131–242134–251173–300233–300282–300
60–105141–232145–240192–300259–300
graphic1 × 10−41 × 10−34 × 10−38 × 10−31 × 10−22 × 10−2
parsec-i
45–120108–257109–300158–300178–222
55–110126–237128–300195–300
60–105138–228139–300213–300
parsec-ii
45–120107–229112–23992–221111–294133–300
55–110117–150130–227109–202138–270166–300
153–211
60–105125–145140–221118–193151–258182–300-
158–203

franec
45–120111–262113–272136–300183–300220–300
55–110131–242134–251173–300233–300282–300
60–105141–232145–240192–300259–300
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