2014A&A...563A..74P


C.D.S. - SIMBAD4 rel 1.7 - 2019.11.18CET03:29:55

2014A&A...563A..74P - Astronomy and Astrophysics, volume 563A, 74-74 (2014/3-1)

The deuterium fractionation of water on solar-system scales in deeply-embedded low-mass protostars.

PERSSON M.V., JORGENSEN J.K., VAN DISHOECK E.F. and HARSONO D.

Abstract (from CDS):

The chemical evolution of water through the star formation process directly affects the initial conditions of planet formation. The water deuterium fractionation (HDO/H2O abundance ratio) has traditionally been used to infer the amount of water brought to Earth by comets. Measuring this ratio in deeply-embedded low-mass protostars makes it possible to probe the critical stage when water is transported from clouds to disks in which icy bodies are formed. We aim to determine the HDO/H2O abundance ratio in the warm gas in the inner 150AU for three deeply-embedded low-mass protostars NGC 1333-IRAS 2A, IRAS 4A-NW, and IRAS 4B through high-resolution interferometric observations of isotopologues of water. We present sub-arcsecond resolution observations of the 31,2-22,1 transition of HDO at 225.89672GHz in combination with previous observations of the 31,3-22,0 transition of H218O at 203.40752GHz from the Plateau de Bure Interferometer toward three low-mass protostars. The observations have similar angular resolution (0.7"-1.3"), probing scales R≲150AU. In addition, observations of the 21,1-21,2 transition of HDO at 241.561GHz toward IRAS 2A are presented to constrain the excitation temperature. A direct and model independent HDO/H2O abundance ratio is determined for each source and compared with HDO/H2O ratios derived from spherically symmetric full radiative transfer models for two sources. From the two HDO lines observed toward IRAS 2A, the excitation temperature is found to be Tex=124±60K. Assuming a similar excitation temperature for H218O and all sources, the HDO/H2O ratio is 7.4±2.1x10–4 for IRAS 2A, 19.1±5.4x10–4 for IRAS 4A-NW, and 5.9±1.7x10–4 for IRAS 4B. The abundance ratios show only a weak dependence on the adopted excitation temperature. The abundances derived from the radiative transfer models agree with the direct determination of the HDO/H2O abundance ratio for IRAS 16293-2422 within a factor of 2-3, and for IRAS 2A within a factor of 4; the difference is mainly due to optical depth effects in the HDO line. Our HDO/H2O ratios for the inner regions (where T>100 K) of four young protostars are only a factor of 2 higher than those found for pristine, solar system comets. These small differences suggest that little processing of water occurs between the deeply embedded stage and the formation of planetesimals and comets.

Abstract Copyright:

Journal keyword(s): astrochemistry - stars: formation - ISM: abundances - protoplanetary disks - stars: general

Simbad objects: 13

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Number of rows : 13

N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2020
#notes
1 3C 84 Sy2 03 19 48.1597607660 +41 30 42.114155434   13.10 12.48 11.09   ~ 3464 3
2 NGC 1333 SFR 03 28 55 +31 22.2   10.9       ~ 1182 1
3 [JCC87] IRAS 2A Y*O 03 28 55.55 +31 14 36.7           ~ 372 3
4 [JCC87] IRAS 4A Y*O 03 29 10.49 +31 13 30.8           ~ 567 1
5 [JCC87] IRAS 4 FIR 03 29 10.9 +31 13 26           ~ 462 0
6 [JCC87] IRAS 4B Y*O 03 29 12.058 +31 13 02.05           ~ 544 0
7 NAME Perseus Cloud SFR 03 35.0 +31 13           ~ 1010 0
8 4C 32.14 QSO 03 36 30.10760600 +32 18 29.3422210     17.50 16.6   ~ 568 1
9 NAME Ophiuchus Molecular Cloud SFR 16 28 06 -24 32.5           ~ 2938 0
10 IRAS 16293-2422 cor 16 32 22.56 -24 28 31.8           ~ 1000 1
11 4C 09.57 BLL 17 51 32.81857318 +09 39 00.7284829   17.46 16.78 15.57   ~ 785 1
12 EM* MWC 349 Em* 20 32 45.6328 +40 39 36.143   15.88 13.15 12.13   Bep 691 1
13 NAME BL Lac BLL 22 02 43.2913773726 +42 16 39.978417860   15.66 14.72     ~ 1975 1

    Equat.    Gal    SGal    Ecl

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2019.11.18-03:29:55

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