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Gas phase Elemental abundances in Molecular cloudS (GEMS): I. The prototypical dark cloud TMC 1.

Authors :
Fuente A
Navarro DG
Caselli P
Gerin M
Kramer C
Roueff E
Alonso-Albi T
Bachiller R
Cazaux S
Commercon B
Friesen R
García-Burillo S
Giuliano BM
Goicoechea JR
Gratier P
Hacar A
Jiménez-Serra I
Kirk J
Lattanzi V
Loison JC
Malinen J
Marcelino N
Martín-Doménech R
Muñoz-Caro G
Pineda J
Tafalla M
Tercero B
Ward-Thompson D
Treviño-Morales SP
Riviére-Marichalar P
Roncero O
Vidal T
Ballester MY
Source :
Astronomy and astrophysics [Astron Astrophys] 2019 May 17; Vol. 624. Date of Electronic Publication: 2019 Apr 19.
Publication Year :
2019

Abstract

GEMS is an IRAM 30m 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 TMC 1. Extensive millimeter observations have been carried out with the IRAM 30m telescope (3 mm and 2 mm) and the 40m Yebes telescope (1.3 cm and 7 mm) to determine the fractional abundances of CO, HCO <superscript>+</superscript> , HCN, CS, SO, HCS <superscript>+</superscript> , and N <subscript>2</subscript> H <superscript>+</superscript> 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 <subscript>V</subscript> ~ 3 to ~20 mag. Two phases with differentiated chemistry can be distinguished: i) the translucent envelope with molecular hydrogen densities of 1-5×10 <superscript>3</superscript> cm <superscript>-3</superscript> ; and ii) the dense phase, located at A <subscript>V</subscript> > 10 mag, with molecular hydrogen densities >10 <superscript>4</superscript> cm <superscript>-3</superscript> . Observations and modeling show that the gas phase abundances of C and O progressively decrease along the C <superscript>+</superscript> /C/CO transition zone (A <subscript>V</subscript> ~ 3 mag) where C/H ~ 8×10 <superscript>-5</superscript> and C/O~0.8-1, until the beginning of the dense phase at A <subscript>V</subscript> ~ 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 a S/H ~ (0.4 - 2.2) ×10 <superscript>-6</superscript> , 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 <superscript>-8</superscript> ). Based on our chemical modeling, we constrain the value of ζ <subscript>H <subscript>2</subscript> </subscript> to ~ (0.5 - 1.8) ×10 <superscript>-16</superscript> s <superscript>-1</superscript> in the translucent cloud.

Details

Language :
English
ISSN :
0004-6361
Volume :
624
Database :
MEDLINE
Journal :
Astronomy and astrophysics
Publication Type :
Academic Journal
Accession number :
31156252
Full Text :
https://doi.org/10.1051/0004-6361/201834654