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Table 1
Central density, enclosed mass, central lepton fraction at bounce, for different strengths of the electron capture on nuclei, and for m∗ = m∗(0) or m∗ = m∗(T).
| Capture rates | ρc,b [1014 g cm-3] | Mb [M⊙] | Yl,b |
|
|
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| Bruenn (1985), m∗(0) | 2.83 | 0.82 | 0.372 |
| Bruenn (1985), m∗(T) | 2.61 | 0.90 (0.08) | 0.377 (0.005) |
|
|
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| NpNh = 1, m∗(0) | 2.79 | 0.79 | 0.345 |
| NpNh = 1, m∗(T) | 2.57 | 0.87 (0.08) | 0.348 (0.003) |
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|||
| NpNh = 10, m∗(0) | 2.67 | 0.67 | 0.308 |
| NpNh = 10, m∗(T) | 2.49 | 0.77 (0.1) | 0.311 (0.003) |
Notes. The values in parentheses are the differences due to the thermal effect under study in the enclosed mass and lepton fraction at bounce.
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