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Fig. 13
Js and Ts as function of ξ for different densities and temperatures for the 44 GHz (solid line) and 95 GHz (dashed lines) transitions a), and for the 36 GHz (solid line) and 84 GHz (dashed lines) masers b). It is possible to convert ξ to methanol abundance using Eq. (3).
This figure is made of several images, please see below:
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