2016A&A...587A..91B


Query : 2016A&A...587A..91B

2016A&A...587A..91B - Astronomy and Astrophysics, volume 587A, 91-91 (2016/3-1)

Exploring molecular complexity with ALMA (EMoCA): Deuterated complex organic molecules in Sagittarius B2(N2).

BELLOCHE A., MUELLER H.S.P., GARROD R.T. and MENTEN K.M.

Abstract (from CDS):

Deuteration is a powerful tracer of the history of the cold prestellar phase in star-forming regions. Apart from methanol, little is known about deuterium fractionation of complex organic molecules in the interstellar medium, especially in regions forming high-mass stars. Our goal is to detect deuterated complex organic molecules toward the high mass star-forming region Sagittarius B2 (Sgr B2) and derive the level of deuteration for these molecules. We use a complete 3-mm spectral line survey performed with the Atacama Large Millimeter/submillimeter Array (ALMA) to search for deuterated complex organic molecules toward the hot molecular core Sgr B2(N2). We constructed population diagrams and integrated intensity maps to fit rotational temperatures and emission sizes for each molecule. Column densities are derived by modeling the full spectrum under the assumption of local thermodynamic equilibrium. We compare the results to predictions of two astrochemical models that treat the deuteration process. We report the detection of CH2DCN toward Sgr B2(N2) with a deuteration level of 0.4%, and tentative detections of CH2DOH, CH2DCH2CN, the chiral molecule CH3CHDCN, and DC3N with levels in the range 0.05%-0.12%. A stringent deuteration upper limit is obtained for CH3OD (<0.07%). Upper limits in the range 0.5-1.8% are derived for the three deuterated isotopologues of vinyl cyanide, the four deuterated species of ethanol, and CH2DOCHO. Ethyl cyanide is less deuterated than methyl cyanide by at least a factor five. The [CH2DOH]/[CH3OD] abundance ratio is higher than 1.8. It may still be consistent with the value obtained in Orion KL. Except for methyl cyanide, the measured deuteration levels lie at least a factor four below the predictions of current astrochemical models. The deuteration levels in Sgr B2(N2) are also lower than in Orion KL by a factor of a few up to a factor ten. The discrepancy between the deuteration levels of Sgr B2(N2) and the predictions of chemical models, and the difference between Sgr B2(N2) and Orion KL may both be due to the higher kinetic temperatures that characterize the Galactic center region compared to nearby clouds. Alternatively, they may result from a lower overall abundance of deuterium itself in the Galactic center region by up to a factor ten.

Abstract Copyright:

Journal keyword(s): astrochemistry - line: identification - stars: formation - ISM: individual objects: Sagittarius B2 - ISM: molecules

Nomenclature: [BMG2016] Sgr B2(NN) (Nos N1-N2).

Simbad objects: 17

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Number of rows : 17
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 W 3(H2O) Mas 02 27 04.6 +61 52 25           ~ 145 0
2 TMC-1 MoC 04 41 45.9 +25 41 27           ~ 1676 0
3 NAME Orion-KL SFR 05 35 14.16 -05 22 21.5           ~ 2294 1
4 NGC 2264 OpC 06 40 52.1 +09 52 37           ~ 1793 0
5 [WZM2000] MMS 3 mm 06 41 12.3 +09 29 12           ~ 32 0
6 IRAS 16293-2422 cor 16 32 22.56 -24 28 31.8           ~ 1252 1
7 QSO J1700-2610 QSO 17 00 53.15406418 -26 10 51.7253944   16.50       ~ 109 1
8 QSO B1730-130 QSO 17 33 02.70578907 -13 04 49.5482119   18 19.50 18.78 17.39 ~ 1138 1
9 QSO J1744-3116 Bla 17 44 23.57824 -31 16 36.2943           ~ 158 1
10 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 14415 0
11 [QSR2011] Sgr B2(N)-SMA2 cor 17 47 19.885 -28 22 13.29           ~ 93 0
12 [BMG2016] Sgr B2(N1) cor 17 47 19.889 -28 22 18.22           ~ 57 0
13 NAME Sgr B2 (North) Rad 17 47 20.2 -28 22 21           ~ 673 1
14 NAME Sgr B2 MoC 17 47 20.4 -28 23 07           ~ 2266 1
15 NAME Sgr B2 Main Rad 17 47 20.5 -28 23 06           ~ 407 1
16 RAFGL 2271 SFR 18 53 18.54 +01 14 57.9           ~ 505 0
17 NAME NGC 7129 FIR 2 IR 21 44 01.5 +66 03 40           ~ 98 0

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