Four-component LOC (see 3.3.1) results for He iλ5876, H β intensities (in |$\rm erg\, cm^{-2}\, s^{-1}$|), and line intensity ratio I(He i λ5876)/I(H β) for Zα = Z⊙, |$\rm He/H=0.1$| by number.
log nH . | log ϕ . | log I(He i λ5876) . | log I(H β) . | ratio . |
---|---|---|---|---|
10 | 19 | 5.984 | 6.973 | 0.102 |
10 | 20 | 6.982 | 7.876 | 0.128 |
11 | 19 | 6.184 | 7.094 | 0.123 |
11 | 20 | 7.205 | 8.009 | 0.157 |
log nH . | log ϕ . | log I(He i λ5876) . | log I(H β) . | ratio . |
---|---|---|---|---|
10 | 19 | 5.984 | 6.973 | 0.102 |
10 | 20 | 6.982 | 7.876 | 0.128 |
11 | 19 | 6.184 | 7.094 | 0.123 |
11 | 20 | 7.205 | 8.009 | 0.157 |
Four-component LOC (see 3.3.1) results for He iλ5876, H β intensities (in |$\rm erg\, cm^{-2}\, s^{-1}$|), and line intensity ratio I(He i λ5876)/I(H β) for Zα = Z⊙, |$\rm He/H=0.1$| by number.
log nH . | log ϕ . | log I(He i λ5876) . | log I(H β) . | ratio . |
---|---|---|---|---|
10 | 19 | 5.984 | 6.973 | 0.102 |
10 | 20 | 6.982 | 7.876 | 0.128 |
11 | 19 | 6.184 | 7.094 | 0.123 |
11 | 20 | 7.205 | 8.009 | 0.157 |
log nH . | log ϕ . | log I(He i λ5876) . | log I(H β) . | ratio . |
---|---|---|---|---|
10 | 19 | 5.984 | 6.973 | 0.102 |
10 | 20 | 6.982 | 7.876 | 0.128 |
11 | 19 | 6.184 | 7.094 | 0.123 |
11 | 20 | 7.205 | 8.009 | 0.157 |
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