# Opening the Treasure Chest in Carina

**Authors:** B. Mookerjea (TIFR, Mumbai, India), G. Sandell (IofA, Univ of Hawaii),, R. Guesten (MPIfR, Bonn), D. Riquelme (MPIfR, Bonn), H. Wiesemeyer (MPIfR,, Bonn), E. Chambers (USRA/SOFIA)

arXiv: 1905.03161 · 2019-06-26

## TL;DR

This study maps and analyzes the physical conditions of the G287.84-0.82 globule in Carina, revealing how stellar radiation and winds shape its structure and gas properties, with detailed multi-line observations and modeling.

## Contribution

It provides a comprehensive multi-wavelength analysis of the globule, combining new observations with PDR and non-LTE models to characterize its morphology, kinematics, and physical conditions.

## Key findings

- Identification of two PDR gas components with different densities.
- Determination of optical depths and excitation temperatures of [CII].
- Estimation of the globule's total mass (~1000 solar masses).

## Abstract

We have mapped the G287.84-0.82 cometary globule (with the Treasure Chest cluster embedded in it) in the South Pillars region of Carina (i) in [CII], 63micron [OI], and CO(11-10) using upGREAT on SOFIA and (ii) in J=2-1 transitions of CO, 13CO, C18O and J=3-2 transitions of H2CO using the APEX telescope in Chile. We probe the morphology, kinematics, and physical conditions of the molecular gas and the photon dominated regions (PDRs) in G287.84-0.82. The [CII] and [OI] emission suggest that the overall structure of the pillar (with red-shifted photo evaporating tails) is consistent with the effect of FUV radiation and winds from eta-Car and O stars in Trumpler 16. The gas in the head of the pillar is strongly influenced by the embedded cluster, whose brightest member is an O9.5V star, CPD-59 2661. The emission of the [CII] and [OI] lines peak at a position close to the embedded star, while all other tracers peak at another position lying to the north-east consistent with gas being compressed by the expanding PDR created by the embedded cluster. The molecular gas inside the globule is probed with the J=2-1 transitions of CO and isotopologues as well as H2CO, and analyzed using a non-LTE model (escape-probability approach), while we use PDR models to derive the physical conditions of the PDR. We identify at least two PDR gas components; the diffuse part (~10^4 cm^-3) is traced by [CII], while the dense (n~ 2-8x10^5 cm^-3) part is traced by [CII], [OI], CO(11-10). Using the F=2-1 transition of [13CII] detected at 50 positions in the region, we derive optical depths (0.9-5), excitation temperatures of [CII] (80-255 K), and N(C+) of 0.3-1x10^19 cm^-2. The total mass of the globule is ~1000 Msun, about half of which is traced by [CII]. The dense PDR gas has a thermal pressure of 10^7-10^8 K cm^-3, which is similar to the values observed in other regions.

## Full text

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## Figures

23 figures with captions in the complete paper: https://tomesphere.com/paper/1905.03161/full.md

## References

50 references — full list in the complete paper: https://tomesphere.com/paper/1905.03161/full.md

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Source: https://tomesphere.com/paper/1905.03161