2013ApJ...769...19V


Query : 2013ApJ...769...19V

2013ApJ...769...19V - Astrophys. J., 769, 19 (2013/May-3)

Hot water in the inner 100 AU of the class 0 protostar NGC 1333 IRAS2A.

VISSER R., JORGENSEN J.K., KRISTENSEN L.E., VAN DISHOECK E.F. and BERGIN E.A.

Abstract (from CDS):

Evaporation of water ice above 100 K in the inner few 100 AU of low-mass embedded protostars (the so-called hot core) should produce quiescent water vapor abundances of ∼10–4 relative to H2. Observational evidence so far points at abundances of only a few 10–6. However, these values are based on spherical models, which are known from interferometric studies to be inaccurate on the relevant spatial scales. Are hot cores really that much drier than expected, or are the low abundances an artifact of the inaccurate physical models? We present deep velocity-resolved Herschel-HIFI spectra of the 312-303 lines of H162O and H182O (1097 GHz, Eu/k = 249 K) in the low-mass Class 0 protostar NGC 1333 IRAS2A. A spherical radiative transfer model with a power-law density profile is unable to reproduce both the HIFI data and existing interferometric data on the H182O 313-220 line (203 GHz, Eu/k = 204 K). Instead, the HIFI spectra likely show optically thick emission from a hot core with a radius of about 100 AU. The mass of the hot core is estimated from the C18O J = 9-8 and 10-9 lines. We derive a lower limit to the hot water abundance of 2x10–5, consistent with the theoretical predictions of ∼10–4. The revised HDO/H2 O abundance ratio is 1x10–3, an order of magnitude lower than previously estimated.

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Journal keyword(s): astrochemistry - circumstellar matter - stars: formation - stars: protostars - techniques: spectroscopic

Simbad objects: 5

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Number of rows : 5
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 [JCC87] IRAS 2A Y*O 03 28 55.55 +31 14 36.7           ~ 513 3
2 [JCC87] IRAS 4A Y*O 03 29 10.49 +31 13 30.8           ~ 770 1
3 [JCC87] IRAS 4 FIR 03 29 10.9 +31 13 26           ~ 489 0
4 [JCC87] IRAS 4B Y*O 03 29 12.058 +31 13 02.05           ~ 625 0
5 IRAS 16293-2422 cor 16 32 22.56 -24 28 31.8           ~ 1357 1

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