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

Authors :
Fuente, A.
Navarro, D. G.
Caselli, P.
Gerin, M.
Kramer, C.
Roueff, E.
Alonso-Albi, T.
Bachiller, R.
Cazaux, S.
Commercon, B.
Friesen, R.
García-Burillo, S.
Giuliano, B. M.
Goicoechea, J. R.
Gratier, P.
Hacar, A.
Jiménez-Serra, I.
Kirk, J.
Lattanzi, V.
Loison, J. C.
Source :
Astronomy & Astrophysics / Astronomie et Astrophysique; Apr2019, Vol. 624, pN.PAG-N.PAG, 25p
Publication Year :
2019

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<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 an 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> $\zeta_{\textrm{H}_2}$ ζ H 2 to ~(0.5–1.8) × 10<superscript>−16</superscript> s<superscript>−1</superscript> in the translucent cloud. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
00046361
Volume :
624
Database :
Complementary Index
Journal :
Astronomy & Astrophysics / Astronomie et Astrophysique
Publication Type :
Academic Journal
Accession number :
136717789
Full Text :
https://doi.org/10.1051/0004-6361/201834654