Astron. Astrophys. 327, 755-757 (1997)
1. Introduction
Since their discovery by Magnani et al. (1985, hereafter MBM),
molecular clouds at high latitudes ( ) have
received considerable attention. The majority of high-latitude clouds
are characterized by low average volume densities
( 100 cm-3), masses (in the range 10
to 100 ), and have visual extinctions between 1
and 5 magnitudes (van Dishoeck et al. 1991). A catalog of all the
presently known clouds has been compiled by Magnani et al. (1996).
From their analysis, Magnani et al. (1996) conclude that the majority
of the high-latitude clouds are local objects (the mean distance of
the sample is 150 pc), possibly located at the near edge of the Local
Bubble. Their ensemble should contribute to 10% to 20% of the total
molecular gas budget of the local ISM.
Multitransition observations of several molecular species indicate
the existence of small cores with densities in excess of
cm-3 (Turner et al. 1992; Reach et
al. 1995). These conditions are very similar to those observed in dark
clouds at low galactic latitudes which are well known sites of
low-mass star formation. The question has naturally raised whether the
translucent molecular clouds share this property with standard dark
clouds.
There have been two recent attempts to answer this question. In the
first one, Magnani et al. (1995, hereafter MCBB) have compiled a list
of all possible star forming sites based on data from the IRAS Faint
Source Survey (Moshir et al. 1989). By using far-infrared colours
typical of pre-main-sequence stars and young stellar objects (YSOs),
they identified 127 candidate sources not associated with regions of
known molecular clouds (hereafter referred to as sample A), plus
another 65 sources with less reliability (sample B). MCBB estimate
that the star formation efficiency in high-latitude clouds would be at
most of order of 1%, assuming that all the faint
IRAS sources were genuine young stars of solar mass. In a second
paper, Caillault et al. (1995) have used X-ray emission as a
diagnostic of the nature of the sources embedded in some high-latitude
clouds. A search through the Einstein IPC X-ray database
yielded negative results, with the exception of one star located
however in a Lynds dark cloud (L1457, MBM12-1). The result was
considered not too surprising, and Caillault et al. (1995) concluded
that the translucent clouds have yet to reveal any evidence of star
formation.
Guided by the MCBB paper, we have set out an experiment aimed at
detecting 22.2 GHz water maser emission in a sample of their sources.
The presence of O maser emission reveals dense
gas (with densities in excess of
cm-3) in star forming regions. It is well known that
O masers are associated with objects in the
earliest evolutionary phases independent of their luminosity/mass.
Several surveys towards HII regions (Codella et al.
1994; Codella & Palla 1995), IRAS sources in the inner and outer
Galaxy (Wouterloot et al. 1993, 1995), CO outflow sources (Tofani et
al. 1995) and low-mass stars (Wilking et al. 1994) have greatly
expanded our knowledge of the occurrence of the maser phenomenon. The
detection of water masers can therefore be considered a secure
identifying criterion even in the case of the infrared sources
embedded within high-latitude clouds.
Previous searches for water masers at high-latitudes have yielded
only upper limits to the O flux. In a survey of
1409 IRAS sources selected using the Emerson (1987) colour criteria
for YSOs, Palumbo et al. (1994) and Codella et al.(1995) have observed
80 sources with with an average rms of 2 Jy.
Maser emission was found only in two sources within known star forming
regions (Orion and HH 7-11).
It is well known that the luminosity of the maser source
( ) scales with the far-infrared (FIR) luminosity
of the associated IRAS source, and the typical ratio of the
luminosities is of order -
(e.g. Palagi et al. 1993). Since the average
luminosity of the IRAS sources in the MCBB sample is
0.1 , assuming a distance
of 150 pc, the expected O luminosity is about
, or a peak flux of
0.3 Jy for isotropic emission and a linewidth of
1 km s-1. However, the flux could be quite smaller than the
isotropic value and this calls for high sensitivity observations. In
this paper, we report on the results of such a survey performed with
the MPIfR Effelsberg (Bonn, Germany) 100-m radiotelescope.
© European Southern Observatory (ESO) 1997
Online publication: April 6, 1998
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