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Table 4.

Ejected yields in M of trans-Fe elements from the T16 explosion model, adopting our final pre-explosive surface trans-Fe abundances as initial abundances.

Element Atomic Ejected Ejected mass [M]
number mass [M] No initial
trans-Fe
Ga 31 1.36e−06 7.89e−09
Ge 32 6.03e−06 1.93e−07
As 33 8.10e−07 2.79e−09
Se 34 5.00e−06 2.53e−07
Br 35 4.37e−07 1.16e−11
Kr 36 6.66e−06 1.61e−09
Rb 37 1.41e−06 4.29e−13
Sr 38 1.74e−06 2.21e−11
Y 39 3.70e−07 1.23e−14
Zr 40 7.64e−07 2.33e−13
Nb 41 1.63e−09 3.75e−17
Mo 42 5.10e−08 2.34e−16
Tc 43 5.22e−10 6.77e−19
Ru 44 7.29e−09 3.76e−17
Rh 45 5.20e−10 2.31e−19
Pd 46 1.94e−08 2.98e−18
Ag 47 1.48e−10 9.78e−24
Cd 48 1.95e−08 7.53e−24
In 49 1.03e−10 4.31e−30
Sn 50 5.56e−08 1.08e−31
Sb 51 1.41e−09 2.82e−39
Te 52 2.94e−09 1.30e−41
I 53 6.48e−10 9.31e−45
Xe 54 1.20e−08 2.01e−47
Cs 55 1.16e−09 1.68e−50
Ba 56 1.62e−08 2.57e−53

[Rb/Sr] 0.27
[Rb/Zr] 0.34

Notes. Surface trans-Fe abundances are from our Model D progenitor and are applied in the outermost ∼0.11 M. The adopted 22Ne(α,n)25Mg and 22Ne(α,γ)26Mg reaction rates are from Wiescher et al. (2023). The last column shows the final yields from the same explosive model but without the inclusion of trans-Fe element enrichment in the external layers of the primary WD, and with a 22Ne abundance equal to the accreted value for model D (as specified in Table 1). The elemental ratios [Rb/Sr] and [Rb/Zr] are also given in square bracket notation in the last two lines.

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