P. Persi1 - M. Tapia2
1 - Istituto Astrofisica Spaziale e Fisica Cosmica, CNR,
Via del Fosso del Cavaliere, 00133 Roma, Italy
2 - Instituto de Astronomía,
UNAM, Apartado Postal 877, Ensenada, Baja California, CP 22830,
Mexico
Received 4 March 2003 / Accepted 7 May 2003
Abstract
Mid-infrared images at 8.7, 9.7 and 12.5
are
presented of the star forming region GGD 14 associated with the
source IRAS 06084-0611. In an area of
30
around the
IRAS position, two mid-infrared sources were found. One was
identified with the cometary compact HII region VLA 1 and the
second with the faint and unresolved radio continuum source VLA 4.
The mid-infrared morphology of VLA 1 is very similar to that of the
radio continuum suggesting a direct interaction between the
ionized gas and the dust. The infrared source associated with VLA 4
shows a large infrared excess and its derived infrared luminosity is
,
indicating the presence of a young star
later than B3. In addition, its spectrum between 2.47 and 11.62
observed by ISOPHOT shows the presence of infrared
emission bands at 3.3, 6.2, 7.7, 8.6 and 11.2
with
relative intensity ratios typical of compact HII regions. Finally,
the radio continuum source VLA 2, undetected on our mid-infrared images,
shows an infrared luminosity of
confirming its
nature of an embedded T-Tauri star.
Key words: stars: formation - infrared: stars
The red nebulous object GGD 14 discovered by Gyulbudaghian et al.
(1978) is embedded in the Monoceros molecular cloud at a distance
of 1 kpc (Racine & van den Bergh 1970; Rodríguez
et al. 1980). This object is within an active star forming region
as shown by the presence of a well-known cometary HII region (VLA 1) ionized by a B0.5 zero-age main-sequence (ZAMS) star
(Tofani et al. 1995; Gómez et al. 1998; Gómez et al. 2000)
and associated with the IRAS source 06084-0611. No point-like
near-infrared source at a level of
has been detected at the
central position of the cometary HII region, although maps at 20,
50, 100 and 800
obtained by Harvey et al. (1985) and Little
et al. (1990) show strong emission centered on this source. This
implies a visual extinction larger than 55 mag in the direction of
the HII region.
A young cluster was found by means of radio and infrared observations
in a region of 30
around the compact cometary HII region
(Gómez et al. 2000; Harvey et al. 1985). Most of the members of
the cluster (at least 8 components) could be low-mass
pre-main-sequence stars as suggested by recent radio continuum
observations at 3.6 and 6 cm (Gómez et al. 2002).
Another active center of star formation in GGD 14 is located
approximately 30
NE of the compact HII region close to
the center of a CO bipolar outflow (Rodriguez et al. 1982), where
a water maser source (Rodriguez et al. 1980; Tofani et al. 1995) and
a radio continuum source (VLA 7) with an associated infrared
source (Gómez et al. 2002) are also located. VLA 7 is probably
the powering source of the molecular outflow.
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Figure 1:
Mid-infrared images of GGD 14 (IRAS 06084-0611). For comparison,
the 2.2 ![]() ![]() |
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Spectrophotometry between 2.47 and 11.62
has been obtained
with ISOPHOT (PHT-S, Lemke et al. 1996) around the IRAS position.
In this work we make use of ISOPHOT data of this source from the ISO Data
Archive (TDT No. 70901306).
In this paper we report the results of mid-infrared images centered on the IRAS position and we discuss the spectral energy distribution (SED) of the detected sources together with the ISOPHOT spectrophotometry.
The narrow-band images at 8.7, 9.7 and 12.5
centered at the
position of the IRAS source 06084-0611 in GGD 14 were taken the night
of November 9 2001 with the mid-infrared camera CID (Salas et al.
2003) on the 2.1m telescope of the Observatorio Astronómico
Nacional at San Pedro Mártir, Baja California, Mexico. This
camera is equipped with a Rockwell
pixel Si:As BIB
detector array and delivers an effective scale of
/pix. The images were taken in the standard
chop-nodding technique to remove the sky and telescope emission
background. The standard stars
Tau and
Aur were
observed before and after the source at similar air-mass for flux
calibration. The images of these stars were also used to estimate
the point-spread function at each wavelength. The mean PSF was
1.5
(FWHM), close to the diffraction limit. The
on-source integration times were 570 s at 8.7
,
and 720 s at 9.7 and 12.5
.
The derived detection limits are
0.2 Jy,
0.5 Jy and 0.3 Jy (1
)
respectively.
Two distinct bright mid-infrared sources separated by 0.2
in RA and 7.3
in Dec are present in all mid-infrared images. We
identify these two sources with the cometary HII region VLA 1,
and with the faint compact radio continuum source VLA 4 (see
Fig. 1). These are also sources Irs 4 and Irs 2 observed by
Harvey et al. (1985) and their 20
map of Fig. 4 is very
similar to our 12.5
image. The mid-infrared emission from the
other three radio continuum sources VLA 2, VLA 6, and VLA 10
(Gómez et al. 2002) are below our detection limits, although
included in the observed field. With the exception of VLA 1, all
the radio continuum sources have associated a near-infrared source as
seen in Hodapp's (1994)
image also displayed in Fig. 1. The mid-infrared
source associated with the cometary HII region is slightly
elongated in the NE-SW direction, while the mid-infrared emission from
VLA 4 appears point-like.
The photometry of the two mid-infrared sources was performed with the
DAOPHOT package within IRAF (Stetson 1987). The flux densities, the 1
statistical errors, and the aperture used for the
photometry of the two sources, are given in Table 1. The IRAS
flux observed at 12
of 27.1 Jy probably include both
sources, VLA 1 and VLA 4.
Spectrophotometry between 2.47 and 11.62
towards
IRAS 06084-0611 was obtained with PHT-S (PHT40) on 25 October
1997. The coordinates of the center of the
aperture of PHT-S on ISO are recorded in the observing log, namely
;
with a probable error of
2-3
(ISO Handbook, Vol. I). This nominal position is
2
west and 4
south of the VLA position of source
VLA 4 (Irs 2) and 6
west and 11
south of source
VLA 1 (Irs 4).
We obtained the PHOT-S calibrated scientific data from the ESO Data Archive
(TDT No. 70901306). Figure 2 illustrates the spectrum
with a total integration time of 620 s. In the figure, our flux
densities for source VLA 4 (open circles) are also reported.
The main uncertainty in this observation is the extent to which the flux from
the northernmost infrared source (VLA 1) is also included in
the aperture, as this is nominally located close or at the edge of the square
aperture of the instrument. Another serious caveat that has to be taken into
account is that the PHT-S spectrophotometry calibrations are accurate only
for sources within 3
of the center of the aperture
(ISO Handbook, Vol. IV).
Table 1: Mid infrared photometry of VLA 1 and VLA 4.
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Figure 2: The PHT-S spectrum towards the IRAS source 06084-0611. The open circles represents our observed flux densities of the source VLA 4 (Irs2). The bars show the widths of the mid-infrared filters. |
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Table 2: Measured line fluxes of the IEB.
The spectrum is dominated by the infrared emission bands (IEB) at 3.3, 6.2, "7.7'', 8.6 and 11.2 m attributed to polycyclic aromatic hydrocarbons (PAHs). In
particular, the so-called "7.7''
m band appears to be composed of two emission
bands at 7.6 and 7.8
m. This double peak is also seen in other compact HII
regions (Roelfsema et al. 1996) and other types of sources. The measured line fluxes
of these bands are reported in Table 2.
Considering the arguments given at the begining of this section,
we estimate that the fluxes reported in Fig. 2 and Table 2
are accurate only to around 25% (see also Mattila et al. 1996).
As mentioned before, we find enough evidence to believe that the ISO spectrum is dominated by source VLA 4 (Irs 2): it is close to the center of the PHT-S aperture in contrast to VLA 1 which lies close to the edge of the PHT-S aperture. Apart from the fact that VLA 1 is extended and may be partially out of the aperture, this ISO instrument exhibits a steep beam profile (ISO Handbook, Vol. IV) which affects very strongly the measured flux away from the center of the field. We cannot exclude, though, that VLA 1 may contribute to a small fraction of the measured flux. It should be mentioned that the fluxes of VLA 4 from our images are consistent with those implied by the satellite spectrum.
Figure 3 illustrates the comparison between our 12.5 contour map and the 3.6 cm contour map from Gómez et al.
(2002). Two of the five radio sources present in our observed
field (VLA 1 and VLA 4), were detected in the mid-infrared. VLA 2, 4 and 10 are coincident with the near-infrared sources found in the Two
Micron All Sky Survey (2MASS) (see Gómez et al. 2002) and in
the K-band image of Hodapp (1994) (Fig. 1). Using the 2MASS
photometry, we derived their positions in the J-H vs. H-Kdiagram, which is presented in Fig. 4. The analysis of this
diagram indicates that VLA 2 is a very highly reddened star with a
small near-infrared excess, while the location of VLA 10 suggests this
source is a late-type star (AV=5-6) with no near-infrared excess. In
contrast, a significant near-infrared excess is observed towards VLA 4.
Gómez et al. (2002) proposed a possible T-Tauri nature for
these sources to explain their observed negative radio spectral
index and radio variability.
In the following sections we discuss individually the nature of
the three radio sources VLA 1, VLA 4 and VLA 2.
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Figure 3:
Contour maps at 12.5 ![]() ![]() |
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Figure 4: J-Hvs. H-K diagram of the VLA sources in the GGD 14 region. The continuous line marks the locus of the main sequence stars from Koornneef (1983). The two parallel lines represent the standard reddening vectors for late and early-type stars. |
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Figure 5:
Spectral energy distribution of VLA 1. The symbols are:
open circles from Harvey et al. (1985), open squares from Little
et al. (1990) with a 15
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Combining our mid-infrared flux densities of Table 1, the narrow-band
photometry around 10 and 20
of Harvey et al. (1985), the
-band upper limit taken from 2MASS, and the sub-millimeter and
millimeter observations at 450, 800 and 1100
with a 15
beam from Little et al. (1990), we obtain the spectral
energy distribution (SED) of VLA 1 shown in Fig. 5. The IRAS flux
densities reported in the SED include the emission of both
sources, VLA 1 and VLA 4, as discussed in Sect. 2.1. Therefore, the
derived luminosity of
,
obtained including
the far-infrared observations (Gómez et al. 2002) is for the two
sources.
Finally, the SED of VLA 1 appears very steep with the infrared spectral index
The mid-infrared emission of VLA 4 appears point-like on our images. The
SED of this source obtained from the near and mid-infrared photometry of
Harvey et al. (1985) and our flux densities of Table 1 taken with a
similar aperture is flatter than that of VLA 1, having a spectral
index
(left panel of Fig. 6). Integrating the infrared
energy distribution and assuming a distance of 1 kpc, we obtain a
luminosity between 1 and 20
.
This
value is consistent with the presence of a very young star
somewhat later than B3. In addition, the measured intensity ratios
I (3.3)/ I(11.2)=0.20, and
I(6.2)/I(7.6)=0.29 of the PAH bands
present in the ISOPHOT spectrum (Fig. 2), are very similar to a
number of Herbig Ae/Be stars and compact HII regions. This young
object is probably a Herbig Ae/Be star.
VLA 2 is a very faint and unresolved radio source
(0.3
)
detected by Gómez et al. (2000) and
associated with source Irs 6 of Harvey et al. (1985). Its
spectral energy distribution (right panel of Fig. 6) is obtained
from the near-infrared photometry of 2MASS and from the photometry up to
20
of Harvey et al. (1985). Our upper limit at 12.5
is also reported in the SED.
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Figure 6: Left panel: SED of VLA 4. The symbols are: open circles from Harvey et al. (1985) and filled circles from this work. Right panel: SED of VLA 2. The symbols are: open circles from Harvey et al. (1985) and filled squared from 2MASS. |
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The two sets of near infrared observations (2MASS and Harvey et al.
1985) suggest that this source is variable as shown in the right
panel of Fig. 6. This fact, together with the estimated
luminosity of
,
indicate that VLA 2 is an embedded
T-Tauri star, in agreement with the conclusion given for this
object by Gómez et al. (2002).
From the analysis of the images at 8.7, 9.7 and 12.5
of a
region of size
30
around GGD 14 around
IRAS 06084-0611) we reached the following conclusions:
1) Two mid-infrared sources associated with the cometary compact HII region VLA 1 and with the faint radio continuum source VLA 4 have
been found. The two sources contribute to the observed IRAS
fluxes. VLA 1 shows a diffuse mid-infrared emission very similar to that
of radio continuum at 3.6 cm (Fig. 3). Its energy distribution is
very steep with the infrared spectral index
.
The bolometric luminosity of this source is <
.
2) The mid-infrared source associated with VLA 4 shows an infrared
excess and its derived infrared luminosity of
is consistent with the presence of a young embedded star
of spectral type somewhat later than B3. Infrared emission bands
at 3.3, 6.2, "7.7'', 8.6 and 11.2
have been observed by ISOPHOT towards this source (Fig. 2). The double peak of the "7.7''
band and the relative intensity ratios are typical of
compact HII regions.
3) The three other radio continuum sources present in our region,
VLA 2, 6 and 10, and classified as possible T-Tauri stars by
Gómez et al. (2002), were not detected in the mid-infrared with
our sensitivity. Particularly interesting is VLA 2 that is
associated with the infrared source Irs 6 of Harvey et al. (1985). This
very red source has a luminosity between 1-20
of
and shows variability in the near-infrared. This confirms
the presence of an embedded T Tauri star.
With our available data, it is impossible to classify for sources VLA 6 and VLA 10.
In summary, we can confirm that the star forming region GGD 14 is a very young complex where stars of different masses ranging from high mass (VLA 1) to intermediate (VLA 4) to low-mass star (VLA 2) are detected in the radio and infrared.
Acknowledgements
Part of this work was supported by a CNR(Italy)-Conacyt(Mexico) bilateral agreement. MT also acknowledges grants from Conacyt and DGAPA-UNAM (IN-105400). We would like to thank Yolanda Gómez for the 3.6 cm image. This publication makes use of data products from the Two Micron All Sky Survey, which is a joint project of the University of Massachusetts and the Infrared Processing and Analysis Center/California institute of Technology, funded by the National Aeronautics and Space Administration and the National Science Foundation.