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Table 3.

Calculated abundances for stable and unstable isotopes primarily affected by three groups of forward and reverse rates of the 42Ti(p,γ)43V with different sources (new, ths8, and rath).

Species New ths8 rath
42Ca 2.01×10−15(1.33–2.71) 3.55×10−15 3.92×10−15
42Sc 2.76×10−10(1.82–3.72) 4.86×10−10 5.38×10−10
43Sc 5.59×10−14(3.69–7.52) 1.00×10−13 1.11×10−13
42Ti 6.21×10−06(4.09–8.36) 1.09×10−05 1.21×10−05
43Ti 1.92×10−09(1.27–2.59) 3.38×10−09 3.74×10−09
45Ti 2.21×10−12(2.21–2.21) 9.93×10−13 9.88×10−13
46Ti 8.35×10−15(8.35–8.36) 4.19×10−15 4.16×10−15
43V 3.65×10−09(2.33–4.95) 7.24×10−10 7.39×10−13
45V 3.23×10−08(3.22–3.23) 1.45×10−08 1.44×10−08
46V 1.34×10−10(1.34–1.34) 6.71×10−11 6.68×10−11
47V 6.00×10−13(6.00–6.00) 4.82×10−13 4.80×10−13
44Cr 1.75×10−06(1.12–2.37) 3.48×10−07 3.56×10−10
45Cr 3.63×10−06(3.63–3.63) 1.59×10−06 1.59×10−06
46Cr 1.70×10−06(1.70–1.70) 8.51×10−07 8.49×10−07
47Cr 8.83×10−10(8.83–8.83) 5.10×10−10 5.08×10−10

Notes. The data in bold refer to the range of predicted isotopic abundances with the same order of magnitude as the front abundance values when the new forward and reverse rates are allowed to vary within their uncertainty bounds.

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