Table 3.
Molecular gas properties of the Planck’s dusty GEMS inferred from the MCMC sampling of the LVG model parameter space using RADEX.
Source | log(nH2) (cm−3) | log(Tk) (K) | log(NCO/dv) (cm−2 km−1 s) |
---|---|---|---|
Single component | |||
PLCK_G045.1+61.1 |
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PLCK_G080.2+49.8 |
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PLCK_G092.5+42.9 |
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PLCK_G102.1+53.6 |
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PLCK_G113.7+61.0 |
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PLCK_G138.6+62.0 |
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PLCK_G145.2+50.9 |
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PLCK_G165.7+67.0 |
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PLCK_G200.6+46.1 |
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PLCK_G231.3+72.2 |
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PLCK_G244.8+54.9 |
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Two components | |||
PLCK_G092.5+42.9 L |
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PLCK_G092.5+42.9 H |
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PLCK_G113.7+61.0 L |
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PLCK_G113.7+61.0 H |
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PLCK_G138.6+62.0 L |
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PLCK_G138.6+62.0 H |
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PLCK_G165.7+67.0 L |
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PLCK_G165.7+67.0 H |
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PLCK_G244.8+54.9 L |
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PLCK_G244.8+54.9 H |
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Notes. Values quoted for each parameter are the median and ±1σ uncertainties of the marginal probability distribution functions. All sources are modeled with a single excitation component and those for which there is a significant mismatch between the best-fit model and observed fluxes of low and/or high-J CO lines are also modeled with two excitation components. In these cases, “L” and “H” indicate the low and high-excitation components, respectively.
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