Issue |
A&A
Volume 407, Number 2, August IV 2003
|
|
---|---|---|
Page(s) | 573 - 587 | |
Section | Interstellar and circumstellar matter | |
DOI | https://doi.org/10.1051/0004-6361:20030875 | |
Published online | 17 November 2003 |
Long-term study of water masers associated with Young Stellar Objects
II. Analysis
1
Istituto di Radioastronomia C.N.R., Via Gobetti 101, 40129 Bologna, Italy
2
INAF - Osservatorio Astrofisico di Arcetri, Largo E. Fermi 5, 50125 Firenze, Italy
3
Istituto di Radioastronomia C.N.R., Sezione Firenze, Largo E. Fermi 5, 50125 Firenze, Italy
Corresponding author: J. Brand, brand@ira.cnr.it
Received:
17
March
2003
Accepted:
9
June
2003
We present the analysis of the properties of water maser emission
in 14 star forming regions (SFRs), which have been monitored for up to 13
years with a sampling rate of about once every 2–3 months. The 14 regions were
chosen to span a range in luminosity Lfir of the associated Young
Stellar Object (YSO) between 20 and
.
The general scope of the analysis is to investigate the dependence of the
overall spectral morphology of the maser emission and its variability on the
luminosity of the YSO. We find that higher-luminosity sources tend to
be associated with stronger and more stable masers. Higher-luminosity YSOs
can excite more emission components over a larger range in velocity, yet
the emission that dominates the spectra is at a velocity very near that of the
molecular cloud in which the objects are embedded.
For Lfir
the maser emission
becomes increasingly structured and more extended in velocity with increasing
Lfir. Below this limit the maser emission shows the same variety of
morphologies, but without a clear dependence on Lfir and with a smaller
velocity extent. Also, for sources with Lfir above
this limit, the water maser is always present above the 5σ-level; below
it, the typical 5σ detection rate is 75–80%.
Although the present sample contains few objects
with low YSO luminosity, we can conclude that there must be a lower limit to
Lfir (
), below which the associated maser is below the
detection level most of the time.
These results can be understood in terms of scaled versions of similar SFRs
with different YSO luminosities, each with
many potential sites of maser amplification, which can be excited provided
there is sufficient energy to pump them, i.e. the basic pumping process is
identical regardless of the YSO luminosity. In SFRs with lower input
energies, the conditions of maser amplification are much closer to the
threshold conditions, and consequently more unstable.
We find indications that the properties of the maser emission may be determined
also by the geometry of the SFR, specifically by the beaming and collimation
properties of the outflow driven by the YSO.
For individual emission components the presence of
velocity gradients seems to be quite common; we find both
acceleration and deceleration, with values between 0.02 and 1.8 km s-1 yr-1.
From the 14 “bursts” that we looked at in some detail we derive
durations of between 60 and 900 days and flux density increases of between
40% and
1840% (with an absolute maximum of ∼820 Jy over 63
days).
The ranges found in burst- intensity and -duration are biased by our minimum
sampling interval, while the lifetime of the burst is furthermore affected by
the fact that bursts of very long duration may not be recognized as such.
In addition to the flux density variations in individual emission components,
the H2O maser output
as a whole is found to exhibit a periodic long-term variation in several
sources. This may be a consequence of periodic variations in the wind/jets
from the exciting YSO.
Key words: masers / stars: formation / radio lines: ISM
© ESO, 2003
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