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Table 2

Physical parameters in our binary population models and the derived CEMP/VMP ratio.

Model set Ang. mom. loss βacc Third dredge up CEMP/VMP (%)

A as Hurley et al. (2002) BHL standard 2.30 ± 0.04
A′ ssw – Eq. (4) BHL standard 2.31 ± 0.04

B ssw – Eq. (4) BHL standard 2.22 ± 0.04
C ssw – Eq. (4) WRLOF standard 2.90 ± 0.04
Cq ssw – Eq. (4) WRLOF q-dep standard 2.63 ± 0.04
D γ2 – Eq. (10) BHL standard 3.12 ± 0.04
E γ2 – Eq. (10) WRLOF standard 4.06 ± 0.03
Eq γ2 – Eq. (10) WRLOF q-dep standard 3.85 ± 0.04

G ssw – Eq. (4) BHL enhanced 9.00 ± 0.12
J ssw – Eq. (4) WRLOF enhanced 11.15 ± 0.13
Jq ssw – Eq. (4) WRLOF q-dep enhanced 11.91 ± 0.14
I γ2 – Eq. (10) BHL enhanced 10.27 ± 0.13
K γ2 – Eq. (10) WRLOF enhanced 12.96 ± 0.14
Kq γ2 – Eq. (10) WRLOF q-dep enhanced 13.66 ± 0.14

Notes.Model set A is the same as in the article by I09. All models use the wind velocity prescription of Vassiliadis & Wood (1993) except model sets A and A′ where vw ∝ vesc. The errors convey only Poisson statistics and could be reduced by increasing the resolution N of our grid of models. A finer grid is not necessary because the observed CEMP/VMP ratio varies between 9% and 25%, a much wider range than the errors in our models.

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