The A33 field was observed with the Narrow Field Instruments (NFI)
of the Beppo-SAX satellite from November 23
to
25
,
1996.
The total effective exposure time is
s
for the LECS instrument and
s
for the MECS instrument (see e.g. Boella et al. 1997a and 1997b for a technical
description of the Beppo-SAX mission and instrumentation).
Data preparation and linearization was performed using the SAXDAS v.1.3 package under the FTOOLS environment. The imaging analysis was performed using the XIMAGE package (Giommi et al. 1991). The extraction of the source and background spectra was done within the XSELECT package. The spectral analysis was performed using XSPEC v.9.0.
The only previous claimed X-ray detection of A33 was done with
the HEAO1 satellite (Johnson et al. 1983; Kowalski et al. 1984).
Due to the large error box of the HEAO1 detectors,
the coordinates of the X-ray source were associated with the optical
coordinates of the A33 cluster. Thus the
Beppo-SAX observation was centered on the optical coordinates
and
.
The MECS 2-10 keV X-ray image of the field is shown in
Fig. 1, where three different subsystems are
evident: a bright and apparently extended source,
1SAXJ0027.1-1926, an extended but smaller source, 1SAXJ0027.2-1930,
located to the south of the brightest source and an apparently
point-like source, 1SAXJ0027.0-1928, located to the west.
Positions, count rates and extraction region radii,
,
are listed in Table 1.
The sources have sufficient count rates to be detected
individually at more than 4 sigma level by the MECS instruments.
The poorer spatial resolution of the LECS instead allows only to determine the
count rate of the brightest source 1SAXJ0027.1-1926.
In the following we describe the spatial structure of each
source detected in the A33 field as derived from the MECS data.
The MECS PSF is
arcmin Half Energy Width, and this spatial resolution
allows us to detect the sources 1SAXJ0027.1-1926 and 1SAXJ0027.2-1930 as extended in the
MECS image of Fig. 1.
The source 1SAXJ0027.1-1926 has an extension of
arcmin (radius).
As discussed in Sects. 3 and 4, this source is most probably the result
of the blending of two point-like sources not resolved by the MECS PSF.
The X-ray MECS image contours superposed onto the POSS II image of
the field plotted in Fig. 2
show that there is no clear galaxy excess
associated to the X-ray source 1SAXJ0027.1-1926.
The source 1SAXJ0027.2-1930, located
arcmin
south of the brightest source (see Fig. 1), has an extension of
arcmin radius. Using a
-model with values
and
kpc (
)
chosen as representative of such
low luminosity objects, and convolved with the MECS PSF
we find a central density of
cm-3.
Moreover, an extended, low surface brightness X-ray emission
is visible in the southern part of the image (see Figs. 1 and 2).
Such a low surface brightness source extends for a few arcminutes
at levels of
cts s-1 cm-2 arcmin-2.
The extended source 1SAXJ0027.2-1930 is associated with A33 as shown
in the POSS II image of the field (see Fig. 2 and
Sect. 3).
The third source 1SAXJ0027.0-1928, located
arcmin south-west
of the brightest source, has a point-like appearance.
Two faint objects in the POSS II are positionally consistent with
1SAXJ0027.0-1928.
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