2024A&A...691A.157V


Query : 2024A&A...691A.157V

2024A&A...691A.157V - Astronomy and Astrophysics, volume 691A157 (2024/11-1)

Identifying the mechanisms of water maser variability during the accretion burst in NGC6334I.

VORSTER J.M., CHIBUEZE J.O., HIROTA T., MacLEOD G.C., VAN DER WALT D.J., VOROBYOV E.I., SOBOLEV A.M. and JUVELA M.

Abstract (from CDS):

Context. High-mass young stellar objects gain most of their mass in short intense bursts of accretion. Maser emission is an invaluable tool in discovering and probing these accretion bursts.
Aims. Our aim was to observe the 22 GHz water maser response induced by the accretion burst in NGC6334I-MM1B and to identify the underlying maser variability mechanisms.
Methods. We report seven epochs of very long baseline interferometry (VLBI) observations of 22 GHz water masers in NGC6334I with the VLBI Exploration of Radio Astrometry (VERA) array, from 2014 to 2016, spanning the onset of the accretion burst in 2015.1. We also report 2019 Atacama Large Millimeter/submillimeter Array (ALMA) observations of 321 GHz water masers and 22 GHz single-dish maser monitoring by the Hartebeesthoek Radio Astronomical Observatory (HartRAO). We analysed long-term variability patterns and used proper motions with the 22 GHz to 321 GHz line ratio to distinguish between masers in non-dissociative C-shocks and dissociative J-shocks. We also calculated the burst-to-quiescent variance ratio of the single-dish time series.
Results. We detected a water maser distribution resembling a bipolar outflow morphology. The constant mean proper motion before and after the burst indicates that maser variability is due to excitation effects from variable radiation rather than jet ejecta. For the whole region, we find that the flux density variance ratio in the single-dish time series can identify maser efficiency variations in 22 GHz masers. The northern region, CM2-W2, is excited in C-shocks and showed long-term flaring with velocity-dependent excitation of new maser features after the onset of the burst. We propose that radiative heating of H2 due to high-energy radiation from the accretion burst be the main mechanism for the flaring in CM2-W2. The southern regions are excited by J-shocks, which have shown short-term flaring and dampening of water masers. We attribute the diverse variability patterns in the southern regions to the radiative transfer of the burst energy in the complex source geometry.
Conclusions. Our results indicate that the effects of source geometry, shock type, and incident radiation spectrum are fundamental factors affecting 22 GHz maser variability. Investigating water masers in irradiated shocks will improve their use as a diagnostic in time-variable radiation environments, such as accretion bursting sources.

Abstract Copyright: © The Authors 2024

Journal keyword(s): masers - techniques: high angular resolution - stars: formation - ISM: jets and outflows - ISM: individual objects: NGC6334I

VizieR on-line data: <Available at CDS (J/A+A/691/A157): table2.dat>

Simbad objects: 21

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Number of rows : 21
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 NAME W 3 OH HII 02 27 04.1 +61 52 22           ~ 1064 2
2 MMB G192.600-00.048 Y*O 06 12 54.0100 +17 59 23.200           ~ 430 0
3 V* V723 Car Or* 10 43 23.26 -59 33 56.7           ~ 23 0
4 IRAS 15254-5621 Y*? 15 29 19.33 -56 31 22.8           ~ 108 0
5 [HBM2006b] I-SMA4 mm 17 20 53.099 -35 47 03.32           ~ 18 0
6 [BHC2016] MM2 mm 17 20 53.188 -35 46 59.32           ~ 47 0
7 NAME NGC 6334-I Cl* 17 20 53.35 -35 47 01.5           ~ 373 0
8 [BHC2016] MM1 cor 17 20 53.415 -35 46 57.88           ~ 121 0
9 [BHC2016] MM1B mm 17 20 53.419 -35 46 57.84           ~ 17 0
10 NAME NGC 6334F (C) HII 17 20 53.45 -35 47 02.6           ~ 244 1
11 QSO B1730-130 Bla 17 33 02.70578907 -13 04 49.5482119   18 19.50 18.78 17.39 ~ 1198 1
12 MMB G358.931-00.030 SFR 17 43 10.02 -29 51 45.8           ~ 70 0
13 [BHT2019] G358.93-00.03 MM1 mm 17 43 10.1014 -29 51 45.693           ~ 37 0
14 Cl* NGC 6618 GBL 2 Y*O 18 20 23.02 -16 11 47.9           ~ 15 0
15 RAFGL 7009S HII 18 34 20.911 -05 59 42.23           ~ 231 0
16 MSXDC G024.33+00.11 DNe 18 35 16.30 -07 36 09.3           ~ 25 0
17 GAL 024.78+00.08 HII 18 36.2 -07 13           ~ 89 0
18 W 49n HII 19 10 13.2 +09 06 12           ~ 497 3
19 [WBN74] W 51 IRS 2 SFR 19 23 39.93 +14 31 09.4           ~ 321 0
20 LDN 1204A HII 22 21 26.68 +63 51 38.2           ~ 120 0
21 NAME Cepheus A SFR 22 56 17.9 +62 01 49           ~ 760 2

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