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The Different Structures of the Two Classes of Starless Cores

  • Authors: Eric Keto and Paola Caselli

Keto & Caselli 2008 The Astrophysical Journal 683 238.

  • Provider: AAS Journals

Caption: Fig. 10.

Line intensity of C18O(1–0) and C18O(2–1) (radiation temperature) and their ratio (2–1)/(1–0) in unstable, prestellar thermally supercritical cores. The temperature structure for this model is shown in Fig. 7. The density structure is shown in Fig. 9. The ratio of the CO lines is a function of the excitation temperature of the CO. In this model because of the low densities at the edge of the core, the CO excitation temperature is much lower than the gas temperature. Parameters are listed in Table 1.

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