2013A&A...558A.126M


Query : 2013A&A...558A.126M

2013A&A...558A.126M - Astronomy and Astrophysics, volume 558A, 126-126 (2013/10-1)

Waterfalls around protostars. Infall motions towards class 0/I envelopes as probed by water.

MOTTRAM J.C., VAN DISHOECK E.F., SCHMALZL M., KRISTENSEN L.E., VISSER R., HOGERHEIJDE M.R. and BRUDERER S.

Abstract (from CDS):

For stars to form, material must fall inwards from core scales through the envelope towards the central protostar. While theories of how this takes place have been around for some time, the velocity profile around protostars is poorly constrained. The combination of observations in multiple transitions of a tracer which is sensitive to kinematics and radiative transfer modelling of those lines has the potential to break this deadlock. Seven protostars observed with the Heterodyne Instrument for the Far-Infrared (HIFI) on board the Herschel Space Observatory as part of the ``Water in star-forming regions with Herschel'' (WISH) survey show infall signatures in water line observations. We aim to constrain the infall velocity and the radii over which infall is taking place within the protostellar envelopes of these sources. We will also use these data to constrain the chemistry of cold water. We use 1-D non-LTE ratran radiative transfer models of the observed water lines to constrain the infall velocity and chemistry in the protostellar envelopes of six Class 0 protostars and one Class I source. We assume a free-fall velocity profile and, having found the best fit, vary the radii over which infall takes place. In the well-studied Class 0 protostar NGC1333-IRAS4A we find that our observations probe infall over the whole envelope to which our observations are sensitive (r>1000AU). For L1527, L1157, BHR71 and IRAS 15398 infall takes place on core to envelope scales (i.e. ∼10000-3000AU). In Serpens-SMM4 and GSS30 the inverse P-Cygni profiles seen in the ground-state lines are more likely due to larger-scale motions or foreground clouds. Models including a simple consideration of the chemistry are consistent with the observations, while using step abundance profiles are not. The non-detection of excited water in the inner envelope in six out of seven protostars is further evidence that water must be heavily depleted from the gas-phase at these radii. Infall in four of the sources is supersonic and in all sources must take place at the outer edge of the envelope, which may be evidence that collapse is global or outside-in rather than inside-out. The mass infall rate in NGC1333-IRAS4A is large (>10–4M/yr), higher than the mass outflow rate and expected mass accretion rates onto the star. This suggests that any flattened disk-like structure on small scales will be gravitationally unstable, potentially leading to rotational fragmentation and/or episodic accretion.

Abstract Copyright:

Journal keyword(s): astrochemistry - line: profiles - stars: formation - stars: protostars - ISM: abundances - ISM: kinematics and dynamics

Simbad objects: 23

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Number of rows : 23
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 [JCC87] IRAS 4A Y*O 03 29 10.49 +31 13 30.8           ~ 715 1
2 [JCC87] IRAS 4 FIR 03 29 10.9 +31 13 26           ~ 478 0
3 [JCC87] IRAS 4B Y*O 03 29 12.058 +31 13 02.05           ~ 600 0
4 [JCC87] IRAS 4C Y*O 03 29 13.54 +31 13 58.2           ~ 107 1
5 NAME Perseus Cloud SFR 03 35.0 +31 13           ~ 1364 0
6 NAME [BM89] B5 DNe 03 47 38.3 +32 52 43           ~ 223 0
7 LDN 1527 DNe 04 39 53 +25 45.0           ~ 634 0
8 LDN 1544 DNe 05 04 16.6 +25 10 48           ~ 863 0
9 [B2001b] IRS 1 Y*O 12 01 36.53040 -65 08 51.9180           ~ 153 0
10 BHR 71 MoC 12 01 37 -65 08.8           ~ 154 0
11 V* DK Cha TT* 12 53 17.2111480272 -77 07 10.736046012           F0e 142 0
12 IRAS 15398-3359 Y*? 15 43 02.21016 -34 09 07.7112       18.38 21.72 ~ 174 0
13 HD 147889 Y*O 16 25 24.3163637976 -24 27 56.569805208 8.56 8.73 7.90     B2V 476 1
14 GSS 30 Y*O 16 26 21.38160 -24 23 04.0524           ~ 210 1
15 NAME VLA 1623-243 Y*O 16 26 26.42 -24 24 30.0           ~ 404 0
16 NAME Ophiuchus Molecular Cloud SFR 16 28 06 -24 32.5           ~ 3630 1
17 NAME Serpens Cloud SFR 18 29 49 +01 14.8           ~ 1100 2
18 GCNM 23 Y*O 18 29 49.63 +01 15 21.9           ~ 273 2
19 NAME Serpens SMM 4 cor 18 29 57.1 +01 13 15           ~ 137 0
20 NAME SERPENS SMM 3 Y*O 18 29 59.28 +01 14 01.7           ~ 101 1
21 SNR G030.8-00.0 SNR 18 47 32 -01 56.5           ~ 531 0
22 AGAL G030.818-00.056 cor 18 47 47.0 -01 54 28           ~ 164 0
23 LDN 1157 DNe 20 39 06.4 +68 02 13           ~ 572 0

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