Gas phase Elemental abundances in Molecular cloudS (GEMS)

I. the prototypical dark cloud TMC 1

Journal Article (2019)
Author(s)

A. Fuente (Observatorio Astronómico Nacional (OAN))

D. G. Navarro (Observatorio Astronómico Nacional (OAN))

P. Caselli (Max Planck Institute for Extraterrestrial Physics Garching)

M. Gerin (Observatoire de Paris)

C. Kramer (Instituto Radioastronomía Milimétrica (IRAM))

E. Roueff (Observatoire de Paris)

T. Alonso-Albi (Observatorio Astronómico Nacional (OAN))

R. Bachiller (Observatorio Astronómico Nacional (OAN))

S. Cazaux (Astrodynamics & Space Missions, Universiteit Leiden)

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Astrodynamics & Space Missions
DOI related publication
https://doi.org/10.1051/0004-6361/201834654
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Publication Year
2019
Language
English
Astrodynamics & Space Missions
Volume number
624
Article number
A105
Downloads counter
235

Abstract

GEMS is an IRAM 30 m Large Program whose aim is determining the elemental depletions and the ionization fraction in a set of prototypical star-forming regions. This paper presents the first results from the prototypical dark cloud Taurus molecular cloud (TMC) 1. Extensive millimeter observations have been carried out with the IRAM 30 m telescope (3 and 2 mm) and the 40 m Yebes telescope (1.3 cm and 7 mm) to determine the fractional abundances of CO, HCO + , HCN, CS, SO, HCS + , and N 2 H + in three cuts which intersect the dense filament at the well-known positions TMC 1-CP, TMC 1-NH3, and TMC 1-C, covering a visual extinction range from A V ~ 3 to ~20 mag. Two phases with differentiated chemistry can be distinguished: (i) the translucent envelope with molecular hydrogen densities of 1-5 × 10 3 cm -3 ; and (ii) the dense phase, located at A V > 10 mag, with molecular hydrogen densities >10 4 cm -3 . Observations and modeling show that the gas phase abundances of C and O progressively decrease along the C + /C/CO transition zone (A V ~ 3 mag) where C/H ~ 8 × 10 -5 and C/O ~ 0.8-1, until the beginning of the dense phase at A V ~ 10 mag. This is consistent with the grain temperatures being below the CO evaporation temperature in this region. In the case of sulfur, a strong depletion should occur before the translucent phase where we estimate an S/ H ~ (0.4-2.2) × 10 -6 , an abundance ~7-40 times lower than the solar value. A second strong depletion must be present during the formation of the thick icy mantles to achieve the values of S/H measured in the dense cold cores (S H ~ 8 × 10 -8 ). Based on our chemical modeling, we constrain the value of ζ H 2 to ~(0.5-1.8) × 10 -16 s -1 in the translucent cloud.

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