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Astron. Astrophys. 349, 475-484 (1999) 1. IntroductionIt is well established that young stars are often strong X-ray sources. The X-ray activity of weak-lined T Tauri stars is now regarded as a defining property of the class, and far more WTTs have been found in X-ray surveys than were known previously from other methods (Neuhäuser et al. 1995a). The Classical T Tauris (CTTS), thought to be younger than the WTTS, are also known to have associated X-ray emission, albeit less extreme. Recently, a number of younger, embedded objects have been detected in X-rays (Casanova et al. 1995, Grosso et al. 1997, Koyama et al. 1996, Carkner et al. 1998). The heating mechanism for the X-ray emitting plasma in WTTS is believed to be magnetic activity, similar to that seen on the Sun but many times stronger. This belief gains varying degrees of support from several directions. Young low-mass stars are rapidly rotating and convective, and so might be expected to have strong magnetic fields. This is borne out by direct measurements of the surface fields of several TTS (Guenther et al. 1999). Strong flaring activity is also often observed (Montmerle et al. 1983, Feigelson & Montmerle 1985, Guenther & Emerson 1997). Preibisch (1998) (hereafter P98) reported the detection of a strong
X-ray source in the Serpens star forming region. This X-ray source
(hereafter Ser-X3) was identified with a group of optically invisible,
IR stars collectively known as SVS4 (Strom et al. 1976). The SVS4
stars have been extensively studied in the NIR by, among others, Eiroa
& Casali (1989), Eiroa & Casali (1992), Giovanetti et al.
(1998) and Horrobin, Casali & Eiroa (1997). These sources are
identified as pre-main sequence objects by Eiroa & Casali (1992)
due to their being embedded in nebulous emission. P98 specifically
associated the ROSAT source with the SVS4 member EC95, but could not
exclude the possibility that nearby EC92 was the true counterpart.
[Note: here, and henceforth, we use the numbering scheme of Eiroa
& Casali (1992) (in their Table 1) to identify the IR
sources.]. By deriving extinctions from the NIR colours, P98
calculated the hydrogen column density in the line of sight, and hence
derived X-ray luminosities from the observed count rates of
(2-7) Table 1. The observed radio flux associated with the point-like source S68-2 (EC95) at two wavelengths on 3 separate dates. The derived radio luminosity at the distance of the Serpens cloud (310 pc) is also given, as derived from the integrated flux. Both IR sources are embedded in nebulosity linking them to
neighbouring IR sources. This suggests they are an integral part of
the SVS4 group and not background objects. Followup observations by
Preibisch (1999, hereafter P99) indicate that EC95 has a total
luminosity of 60 IR photometry has been presented by Eiroa & Casali (1992) and
Giovannetti et al. (1998), amongst others. 3mm observations by Testi
& Sargent (1998) show no sign of a source at the position of EC95
(an upper limit of 2.7mJy beam-1 for a beam of
approximately 5" Preibisch (1997) (hereafter P97) used the ROSAT HRI detector to
search for point sources in the NGC 1333 star-forming region. A number
of X-ray sources associated with YSO's were detected. One of these
X-ray sources, P97's source number 11 which we will refer to hereafter
as NGC1333-X11, or just X11, was associated with the
optically-invisible object SVS16. This object had a very large derived
optical extinction ( Preibisch et al. (1998) (hereafter PNS98) obtained further NIR
photometry and spectoscopy of this object. SVS16 consists of two
widely separated components, SVS16-e and SVS16-w. As with EC95, IR
spectra were used with an iterative fitting technique to obtain
stellar parameters. For 16-w and 16-e, the spectral types are found to
be M2 and M3, the luminosities 3.8 and
2.7 The X-ray luminosity was measured to be
2 The detection of these extreme sources poses interesting questions
concerning the nature of X-ray emission from pre-main sequence
objects. In particular, there is the question of whether any coronal
model can explain such activity. A particular problem lies with the
ratio There is no shortage of alternative candidates for modelling X-ray emission from a Young Stellar Object (YSO). The environments of YSO's are complex and poorly understood. Remnants of the parent cloud continue to accrete onto the star, either falling inwards in a spherically symmetric flow, or being channelled through an accretion disk. The disk may possess a magnetic field of its own, and in the case of Classical T Tauri stars (CTTS) stellar magnetic fields may play a role in channelling the material onto the stellar surface in the very inner regions (Königl 1991). At the centre of the system, the young star itself is often rapidly rotating, not yet having shed the angular momentum of its parent cloud (Bouvier et al. 1993). The interaction of various magnetic fields with the accreting material produces jets and outflows (e.g. Shu et al. 1994). Any or all of these types of processes could be invoked to produce significant X-ray flux. The purpose of this paper is to investigate one of the empirical properties of coronae in general, that thermal X-ray emission from coronal plasma is correlated with synchrotron radio emission from accelerated electrons (Güdel & Benz 1993, Benz & Güdel 1994). We therefore search for radio counterparts to the two extreme sources. If radio luminosity of approximately the correct magnitude is found, this is evidence (although not conclusive evidence) that the source is coronal. Stronger evidence for magnetic activity (implying a corona) would include the detection of rapid flaring activity, circular polarization, or a synchrotron-type falling spectrum.
© European Southern Observatory (ESO) 1999 Online publication: September 2, 1999 ![]() |