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Table 1.

Stellar masses of our set of low-mass He-core WD models (Col. 1) and the H content associated with different thicknesses of the envelope adopted for each stellar mass (Teff ∼ 8000 K).

M/M log(MH/M) log(MH/M) log(MH/M) log(MH/M) log(MH/M) log(MH/M) log(MH/M)
0.1554 −1.69 −2.50 −3.00 −3.72 −4.37 −5.02 −5.20
0.1612 −1.76 −2.49 −3.00 −3.70 −4.35 −5.04 −5.23
0.1650 −1.82 −2.50 −3.01 −3.69 −4.35 −5.06 −5.28
0.1706 −1.89 −2.50 −3.01 −3.69 −4.39 −5.13 −5.32
0.1762 −1.95 −2.50 −3.00 −3.66 −4.34 −5.14 −5.43
0.1805 −2.44 −3.00 −3.65 −4.33 −5.17 −5.51
0.1869 −2.37 −2.99 −3.64 −4.32 −5.19 −5.61
0.1921 −2.35 −3.02 −3.62 −4.30 −5.17 −5.58
0.2025 −2.43 −3.00 −3.61 −4.30 −5.20 −5.62
0.2390 −2.45 −3.04 −3.67 −4.28 −5.15 −5.58
0.2707 −2.96 −3.67 −4.32 −5.19 −5.54
0.3205 −2.81 −3.60 −4.30 −5.08 −5.54
0.3624 −3.10 −3.62 −4.32 −5.15 −5.64
0.4352 −3.21 −3.71 −4.32 −5.14 −5.79

Notes. Column 2 indicates the upper limit of the H-envelope thickness (“canonical envelope”) for each stellar mass as given by our fully evolutionary computations that assume that mass loss proceeds via stable Roche lobe overflow.

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