Figure 8.
Illustration of the effect of beaming on the optical depth of the $1_{10}{\!-\!}1_{11}$ and $2_{11}{\!-\!}2_{12}$ transitions. The parameters for the calculation are shown in the upper panel. The red dashed vertical line indicates the specific column density where the $4_{13}{\!-\!}4_{14}$ transition (48 GHz) switches from being inverted to non-inverted. The black dashed vertical line indicates the specific column density where the maser path-length equals $7 \times 10^{16}$ cm.

Illustration of the effect of beaming on the optical depth of the |$1_{10}{\!-\!}1_{11}$| and |$2_{11}{\!-\!}2_{12}$| transitions. The parameters for the calculation are shown in the upper panel. The red dashed vertical line indicates the specific column density where the |$4_{13}{\!-\!}4_{14}$| transition (48 GHz) switches from being inverted to non-inverted. The black dashed vertical line indicates the specific column density where the maser path-length equals |$7 \times 10^{16}$| cm.

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