A&A 379, 407-411 (2001)
DOI: 10.1051/0004-6361:20011344
I. D. Karachentsev 1 - M. E. Sharina 1,10 - A. E. Dolphin 2 - D. Geisler 3 - E. K. Grebel 4 - P. Guhathakurta 5,
- P. W. Hodge 6 -
V. E. Karachentseva 7 - A. Sarajedini 8 - P. Seitzer 9
1 - Special Astrophysical Observatory, Russian Academy
of Sciences, N.Arkhyz, KChR, 369167, Russia
2 - Kitt Peak National Observatory, National Optical Astronomy Observatories,
PO Box 26732, Tucson, AZ 85726, USA
3 - Departamento de Fisica, Grupo de Astronomia, Universidad de Concepcion,
Casilla 160-C, Concepcion, Chile
4 - Max-Planck-Institut für Astronomie, Königstuhl 17, 69117
Heidelberg, Germany
5 - UCO/Lick Observatory, University of California at Santa Cruz, Santa Cruz,
CA 95064, USA
6 - Department of Astronomy, University of Washington, Box 351580, Seattle, WA, USA
7 - Astronomical observatory of Kiev University, 04053, Observatorna 3, Kiev,
Ukraine
8 - Department of Astronomy, University of Florida, Gainesville, FL 32611, USA
9 - Department of Astronomy, University of Michigan, 830 Dennison Building,
Ann Arbor, MI 48109, USA
10 - Isaac Newton Institute, Chile, SAO Branch, Russia
Received 31 July 2001 / Accepted 12 September 2001
Abstract
We present HST WFPC2 and ground-based images of the low surface brightness
dwarf Irr/Sph galaxy KKR 25 in Draco. Its colour-magnitude diagram shows
red giant branch stars with the tip at
,
and the presence of
some blue stars. The derived true distance modulus,
,
corresponds to linear distances of KKR 25 from the Milky Way and from the
Local Group centroid of 1.86 and 1.79 Mpc, respectively. The absolute magnitude
of the galaxy,
MV = -10.48, its linear diameter (0.54 Kpc) and central
surface brightness (
)
are
typical of other dIrr/dSphs in the Local Group. Being situated just
beyond the radius of the zero-velocity surface of the Local Group, KKR 25
moves away from the LG centroid at a velocity of
VLG = + 72 km s-1.
Key words: galaxies: dwarf - galaxies: distances
Among the faintest dwarf irregular (dIrr) galaxies in the Local Group, there are galaxies that may be in transition from dIrrs to dwarf spheroidals (dSphs): Phoenix (MV=-9.8) and LGS 3 (MV=-10.5). These galaxies contain prominent old populations reminiscent of dSphs, but also some recent star formation as indicated by young blue stars and have HI associated with them, which is characteristic for dIrrs. They are therefore classified as dIrr/dSphs (Grebel 2000). The discovery of Antlia dwarf (Whiting et al. 1997) with MV= -10.7 at a distance of D = 1.32 Mpc, shows that such extremely faint bluish galaxies of regular shape may also occur outside the Local Group. A detailed studying of these tiny transient objects is very important to understand their origin and evolution.
The detection of low surface brightness galaxies with an
absolute magnitude of about
,
situated between galaxy groups, is a
complicated observational task. Recent all-sky searches for nearby dwarf
galaxies made on the POSS-II and ESO/SERC plates by Karachentseva
& Karachentsev (1998), Karachentseva et al. (1999, 2000), and
Karachentsev et al. (2000) has led to the discovery of
600 objects
mainly of low surface brightness. One object from these lists, KKR 25
(Karachentseva et al. 1999), is considered in the present Note.
KKR 25 has an apparent size of 1
65 and is located next
to a luminous red foreground star. In its direction Huchtmeier et al. (2000)
detected HI emission with a heliocentric radial velocity
kms-1 and a linewidth
W50 = 14 kms-1, which was
attributed to local Galactic hydrogen.
The first large-scale image of KKR 25 was obtained
with the 6-m telescope (SAO, Russia) in the R and I bands with a
1
seeing (FWHM) on June 18, 1999. The R image,
presented in Fig. 1,
![]() |
Figure 1:
R-band image of KKR 25 in Draco obtained with the 6 m SAO telescope. The horizontal
line corresponds to 10
![]() |
Open with DEXTER |
Observations of KKR 25 with the Hubble Space Telescope WFPC2 were obtained
on May 25, 2001 as part of the HST snapshot survey of probable nearby
galaxies (GO program 8601, PI: P. Seitzer). The galaxy was imaged in
F606W and F814W with exposure times of 600
each, with the galaxy center
located in the WF3 chip. Figure 2 shows the galaxy image on this chip
resulting from the combination of both filters to remove cosmic rays.
![]() |
Figure 2: WF3 image of KKR 25 produced by combining the two 600 s exposures taken through the F606W and F814W filters. A globular cluster candidate is indicated by the arrow. |
Open with DEXTER |
The photometric pipeline used for the snapshot survey has been described
in detail in Dolphin et al. (2001), and what follows is only a summary.
After obtaining the calibrated images from STScI, cosmic ray cleaning
was performed with the HSTphot (Dolphin 2000a) cleansep routine
which cleans images taken with different filters by allowing for a
colour variation. Stellar photometry was then obtained with the HSTphot
multiphot routine which measures magnitudes simultaneously in
the two images, accounting for image alignment, WFPC2's wavelength-dependent
plate scale, and geometric distortion.
The final photometry was then done using aperture corrections to a
radius, and the Dolphin (2000b) charge-transfer inefficiency (CTE)
correction and zero-point calibration applied. We estimate the aperture corrections
in the three wide field chips to be accurate to 0.05 mag. The CTE
correction depends on the X- and Y-positions, the background counts,
the brightness of the stars, and the time of the observations. For our
data the mean CTE correction makes a star brighter by
.
Because of the small areal coverage of the Planetary Camera (PC) and
consequent lack of stars suitable for an
accurate aperture correction, the PC photometry is excluded from our
analysis. Aditionally, stars with a signal-to-noise ratio
chi
,
or
sharpness
in each
exposure were eliminated from the final photometry list,
in order to minimize the number of false detections.
Finally, the F606W and F814W instrumental magnitudes
of 1875 stars were converted to
the standard
system following the "synthetic" transformations of
Holtzman et al. (1995). We used the parameters of transformation from their
Table 10, taking into account different relations for blue and red stars
separately. Because we used the non-standard V filter F606W instead of
F555W, the resulting I and especially V magnitudes may contain systematic
errors. However, when comparing our F606W, F814W photometry of other
snapshot targets with ground-based V,I photometry, we find that the
transformation uncertainties,
and
,
are
within 0
05 for stars with colours of
0 < (V-I) < 2. Note that
the zero-point for the F606W observations is taken from WFPC2 observations of
Omega Centauri as measured by Dolphin (2000b).
Figure 3 shows the colour-magnitude diagrams (CMDs) derived for the
central WF3 field,
![]() |
Figure 3: WFPC2 colour-magnitude diagram for KKR 25 in Draco. The left panel shows stars in the WF3 chip, the middle and the right CMDs correspond to the WF2 and WF4 chips. The solid line in the left panel shows the red giant branch of the globular cluster M 15 with metallicity of -2.17 dex. |
Open with DEXTER |
The magnitude of the TRGB has been obtained applying a Sobel filter.
Following Sakai et al. (1996), we use an edge-detection filter, which is a
modified version of a Sobel kernel ([-1,0,+1]), to the Gaussian-smoothed
I-band luminosity function. Only red stars with colours
0.6 < (V-I) < 1.6were considered. The resulting luminosity function and the Sobel
filtered luminosity function are shown in Fig. 4.
![]() |
Figure 4:
The Gaussian-smoothed I-band luminosity function restricted to red
stars with colors between
![]() |
Open with DEXTER |
According to Da Costa & Armandroff (1990), the TRGB can be assumed to
be at
MI = -4.05 for metal-poor systems. With a Galactic extinction
along the line of sight toward KKR 25 of
(Schlegel et al.
1998) this yields a distance modulus of
or
Mpc. The quoted errors include the error in the TRGB detection
(0
10), as well as uncertainties of the HST photometry zero point
(
), the aperture corrections (
), and crowding effects
(
)
added in quadrature.
The solid line in Fig. 3 (left panel) is the M 15 globular cluster
fiducial with [Fe/H] = -2.2 dex from Da Costa & Armandroff (1990), which
was reddened and shifted to the derived galaxy's distance. This
low-metallicity fiducial provides a good fit to the RGB of KKR 25. With
knowledge of the distance modulus of KKR 25 we can estimate its mean
metallicity from the mean colour of the RGB measured at an absolute
magnitude
MI = -3.5, as recommended by Lee et al. (1993). Based on
a Gaussian fit to the colour distribution of the giant stars in the
range
we derive a mean dereddened colour of the RGB
stars of
.
Following Lee et al. (1993)
this yields a mean metallicity [Fe/H
dex.
Integrated photometry of the HST data of the galaxy was
carried out with increasing
circular apertures. The sky level was approximated by a two-dimensional
polynomial, using regions with only a few stars near the edges of the images.
Then the galaxy magnitude in each band was measured as the asymptotic
value of the derived curve of growth. Figure 5 shows the results.
![]() |
Figure 5: Radial distribution of surface brightness in KKR 25 in the V(dashed) and the I (solid line) bands. |
Open with DEXTER |
A summary of the basic properties of KKR 25 is given in Table 1.
Parameter | KKR 25 |
RA (B1950.0) | 16![]() ![]() |
Dec (B1950.0) | +54
![]() |
RA (J2000.0) | 16![]() ![]() |
Dec (J2000.0) | +54
![]() |
Morphological type | dIrr/dSph |
Angular diameter, a26.5 | 1
![]() |
Axial ratio | 0.59 |
Extinction, AV/AI |
![]() |
Total magnitude, ![]() |
![]() |
![]() |
0.88![]() |
Central surface brightness,
![]() |
![]() |
![]() |
![]() |
(m-M)0 |
![]() |
Distance,
![]() |
1.86 Mpc |
Distance,
![]() |
1.79 Mpc |
Linear diameter, A26.5 | 0.54 Kpc |
Absolute magnitude, MV | -10.48 |
(V - I)0,-3.5 | 1.26![]() |
![]() |
-2.1![]() |
Heliocentric velocity, ![]() |
-135![]() |
Corrected velocity,
![]() |
+72 kms-1 |
HI flux | 2.20 Jy![]() |
HI line width, W50 | 14 kms-1 |
M(HI)/LV | 0.80
![]() |
M(dyn)/LV | 1.50
![]() |
As mentioned above, KKR 25 contains a population of faint bluish stars
with
(V-I) < 0.5. These stars are distributed more or less homogeneously
over the galaxy body. On August 2000 KKR 25 was imaged with the 6-m telescope
with an H
filter. After the subtraction of the continuum the
H
image shows no compact HII regions. These properties indicate
that KKR 25 can be classified as a dIrr/dSph just as Phoenix and LGS 3.
We searched for globular clusters in KKR 25 and found one candidate
situated half-way from the center to the left edge of WF3 (see Fig. 2).
This bright diffuse object has an integrated apparent magnitude
and an angular half-light radius
that
corresponds to
and
R(0.5L) = 5.2 pc, which are within
the values typical of Galactic globular clusters. However, the integrated
color of the object,
,
seems to be too red for a globular
cluster.
According to its distance with respect to the Local Group centroid,
Mpc, KKR 25 is situated beyond the radius of the zero-velocity
surface for the Local Group (Karachentsev & Makarov 2001). The distance
of KKR 25 is in good agreement with
its positive radial velocity
kms-1with respect to the Local Group centroid. Note that the distance and the
velocity of KKR 25 are almost the same as for another dIrr/dSph galaxy,
Antlia, which has
Mpc and
kms-1 (Aparicio
et al. 1997). Compared to Antlia, KKR 25 has a somewhat smaller luminosity
and size. But unlike Antlia (assosiated with NGC 3109, Sex A, and
Sex B), KKR 25 is a totally isolated object, with no other known galaxies
within a radius of 0.5 Mpc.
Acknowledgements
Support for this work was provided by NASA through grant GO-08601.01-A from the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., under NASA contract NAS5-26555. I.D.K., V.E.K., and E.K.G. acknowledge partial support through the Henri Chrétien International Research Grant administered by the American Astronomical Society. D.G. acknowledges financial support for this project received from CONICYT through Fondecyt grant 8000002. This work has also been partially supported by the DFG-RFBR grant 01-02-04006 and RFBR grant 01-02-16001