Table 3.
Sensitivity to a bulk change in the rates of a given source.
Model | Source(a) | Scaling factor(a) | ![]() |
![]() |
Relevant yield ratios(c) |
---|---|---|---|---|---|
S | MPLD00 | ×10 | 0.002 | −0.021 | 58Ni(×2.2); 62Ni(×2.0); 60Ni(×0.86); 47Ti(×0.41) |
S | MPLD00 | ×0.1 | 0.000 | 0.002 | 47Ti(×1.2); 64Zn(×1.1); 62Ni(×0.89); 58Ni(×0.88) |
S+ | MPLD00 - p(d) | ×10 | 0.002 | −0.025 | 58Ni(×1.9); 62Ni(×1.6); 60Ni(×0.89); 47Ti(×0.36) |
C2 | MPLD00 - p | ×10 | −0.003 | −0.055 | 50Ti(×27.); 64Ni(×23.); 54Cr(×14.); 58Ni(×1.2) |
C3 | MPLD00 | ×10 | −0.030 | −0.130 | 48Ca(×4.9E5); 64Ni(×164.); 54Cr(×8.9); 54Fe(×0.86) |
C3 | MPLD00 | ×0.1 | 0.000 | 0.104 | 64Zn(×1.2); 58Ni(×0.69); 48Ca(×2.0E−2); 54Cr(×1.7E−5) |
C3 | MPLD00 - p | ×10 | −0.004 | −0.066 | 48Ca(×2.6E3); 64Ni(×34.); 54Cr(×3.8); 54Fe(×1.01) |
C3 | MPLD00 - p | ×0.1 | 0.001 | 0.011 | 58Ni(×1.00); 64Zn(×0.99); 54Cr(×0.71); 48Ca(×0.13) |
C3 | Oda94 | ×10 | 0.000 | 0.000 | 48Ca(×1.3); 64Ni(×1.1); 54Cr(×1.05); 29Si(×0.98) |
C3 | Oda94 | ×0.1 | −0.001 | −0.003 | 17O(×1.01); 50Ti(×0.99); 64Ni(×0.99); 48Ca(×0.97) |
C3 | FFN82 | ×10 | 0.000 | 0.000 | 48Ca(×1.01); 64Ni(×1.01); 47Ti(×0.998); 33S(×0.994) |
C3 | FFN82 | ×0.1 | 0.000 | 0.000 | 22Ne(×1.01); 48Ca(×0.998); 33S(×0.996); 21Ne(×0.987) |
C4 | MPLD00 - p | ×10 | −0.006 | −0.056 | 80Se(×55.); 48Ca(×42.); 64Ni(×3.8); 54Cr(×2.1) |
C5 | MPLD00 - p | ×10 | −0.009 | −0.062 | 80Se(×7.3E3); 48Ca(×14.); 64Ni(×2.1); 54Cr(×1.6) |
C3_100 | MPLD00 - p | ×10 | −0.004 | −0.037 | 48Ca(×5.1); 64Ni(×2.5); 54Cr(×1.9); 54Fe(×1.05) |
C3_500 | MPLD00 - p | ×10 | −0.004 | −0.074 | 48Ca(×9.3E3); 64Ni(×90.); 54Cr(×7.2); 54Fe(×4.4) |
C3_1p2 | MPLD00 - p | ×10 | −0.007 | −0.139 | 48Ca(×2.4E3); 64Ni(×33.); 54Cr(×3.8); 54Fe(×1.01) |
C3_4p0 | MPLD00 - p | ×10 | −0.002 | −0.047 | 48Ca(×2.7E3); 64Ni(×34.); 54Cr(×3.8); 54Fe(×1.03) |
Notes.
Relative change in the final kinetic energy and the mass of 56Ni, with respect to the values reported for the same model in Table 1.
Ratio of the final yield of a few selected isotopes with respect to those in the same model with no weak rates scaled. The isotopes reported in this work are a selection among those with non-negligible ejected mass and whose yield is most affected by the scaling. Ratios larger than 999. are given in exponential format, for example ( × 5E5) means an increment of the yield by a factor 5 × 105.
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