For optically thin CO rotational thermometry of the same emitting population, the upper-level abundance ratio isThe difference can be obtained directly from the two successive transition frequencies, , or approximately from . Using the supplied rounded molecular data gives K. ThereforeThe observed ratio is , henceAt 20 K the predicted ratio would be only about 61, so the two detections reject that single-temperature optically thin 20-K model. The inferred value is an excitation temperature under the stated assumptions, not a model-independent measurement of the gas's kinetic temperature.
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