Properties in the u band of local star-forming galaxies Cristina Dı́az1 , Jaime Zamorano1, Jesús Gallego1 , P.G. Pérez-González1, and A. Gil de Paz1 Departamento de Astrofı́sica, Universidad Complutense de Madrid, Avda. Complutense s/n 28040 Madrid, Spain cdl@astrax.fis.ucm.es Summary. We present u0 Sloan photometry for a representative sample of local star-forming UCM galaxies. We perform a comparison with previous photometry, showing that galaxy colors are those typical for late type galaxies; the study of structural parameters (effective radii and light concentration indexes) points to a mainly central location for the star-forming bursts. 1 Introduction The Universidad Complutense de Madrid Survey (list I, Zamorano et al. 1994; list II, Zamorano et al. 1996; list III, Alonso et al. 1999) constitutes a representative and fairly complete sample of current star-forming galaxies in the local Universe. The survey was carried out with the 80/120 cm f/3 Schmidt telescope at the German-Spanish Observatory of Calar Alto (Almerı́a, Spain). The objects were selected by the presence of Hα λ6563 + [NII] λ6584 emission in their spectra. A total number of 191 objects were cataloged as UCM galaxies in List I and List II. The galaxies included in UCM lists I and II (hereafter the UCM Survey) have been deeply analyzed in optical and infrared bandpass: Johnson B (Pérez-González et al., 2000, 2001), Gunn r (Vitores et al., 1996a,b), J and K nIR (Alonso-Herrero et al., 1996; Gil de Paz et al., 1998), narrow band Hα (Pérez-González et al., 2003c). The spectroscopic analysis was performed by Gallego et al. (1996, 1997) and it has also been used to determine the Hα luminosity function and star formation rate density in the Local Universe (Gallego et al., 1995; Pérez-González et al., 2003c). Spectroscopically, all types of star-forming galaxies are represented, mainly low-excitation, high-metallicity starburst-like galaxies (57%), but also high-excitation, low-metallicity HIIlike galaxies (32%), and a small fraction (8%) of AGN. Morphologically, the sample is dominated by late-type spirals, with less than 10% showing typical parameters of earlier types (Vitores et al., 1996a; Pérez-González et al., 2001). 2 Dı́az, C., et al. 70 60 50 25 40 20 30 15 20 10 10 5 0 -23 -22 -21 -20 -19 -18 -17 -16 -15 0 -14 MB 60 30 25 -0.2 0.2 0.6 1 1.4 1.8 2.2 UCM Survey This subsample u + ha obs 20 Ngal Ngal 40 30 15 20 10 10 5 0 -0.6 B-r UCM Survey This subsample u + ha obs 50 UCM Survey This subsample u + ha obs 30 Ngal Ngal 35 UCM Survey This subsample u + ha obs 50 100 150 200 250 300 350 400 450 500 EW (Hα) 0 -26 -25 -24 -23 -22 -21 -20 -19 -18 -17 MK Fig. 1. Histograms for the UCM Survey galaxies and the galaxies involved in this study. Most of the galaxies observed at the u band have Hα images. The analysis of the properties of the stellar populations in the UCM galaxies has been tackled in Pérez-González et al. (2003a,b). An average UCM galaxy has subsolar metallicity, total stellar ∼ 1010 M , and harbored an instantaneous burst about 5 Myr ago, involving ∼ 5% of the total stellar mass. Here we present u0 Sloan band photometry for a representative subsample of galaxies of the UCM Survey. This band has been chosen because it yields in the optical range for high-z populations and, while LU V (λ . 2500 Å) is commonly used as an SFR tracer (e.g. Sullivan et al., 2000; Schiminovich et al., 2005), the luminosity at the u-band (λ ≈ 3600 Å) is similarly dominated in starburst galaxies by young stellar populations, and so it may be used as and SFR indicator (Hopkins et al., 2003) for high-z objects. 2 The data The UCM Survey includes 191 galaxies in regions of 12h−16h and 22h−2h on RA, respectively, covering a 10◦ width strip centered at DEC 20◦ . This work presents the u0 observations for a subsample of 71 galaxies (40% of the total). According to the Kolmogorov-Smirnov test, the subset is representative of the whole sample with over 85% of confidence in properties such as equivalent width of the Hα line, K and B band magnitude and B − r color (figure 1). Properties in the u band of local star-forming galaxies 3 The galaxies were observed during three runs and two service nights at the CAHA 2.2m Telescope1 , and another run at the NOT Telescope2 . At the 2.2m telescope in Calar Alto, the instrument BUSCA was used to get simultaneous images of the UCM galaxies in u, g, r Gunn-Thuan and I Johnson with a scale of 0.34 00 /pix, ensuring a good sampling of the objects, with seeing values from 000. 9 to 200. 5. The effective wavelength and the FWHM in the u channel are 3633 and 400 Å. At the NOT telescope, the ALFOSC instrument provide images at the u’ Sloan band with 0.19 00 /pix. 3 Galaxy photometry 3.1 Data reduction and flux calibration Standard reduction procedures for CCD photometry were applied. Raw images were bias subtracted by using a master bias for each run (an average of the nightly 15-20 bias images). Flat field correction was applied after combining at least seven sky-flats images. Cosmic rays were removed using the laplacian cosmic ray removal algorithm of van Dokkum (2001) and near foreground stars masked using the cr utils IRAF3 package. For the purposes of photometric calibration, standard stars were observed during each night under different airmasses. The standards were chosen between those standard stars that define the SDSS u0 , g 0 , r0 , i0 , z 0 photometric system (Smith et al., 2002). Standard stars fluxes were measured using the IRAF apphot package, and the differences between the u0 filter and the one used at CAHA runs were taken into account in the color term of the Bouguer equation to transform instrumental to u0 magnitudes: mu0 + 2.5 · log(Fu ) = Cu − Ku · X + K(u0 −g0 ) · (u0 − g 0 ) 0 (1) −1 where mu0 is SDSS u magnitude, Fu is the flux in counts s , C is the instrumental constant, Ku0 the extinction, X the airmass, and K(u0 −g0 ) the color constant referred to the SDSS u0 − g 0 color. 3.2 Integrated photometry The measurement of galaxy fluxes has made use of the IRAF task polyphot: we built polygons around the galaxies including the whole object but also 1 2 3 Centro Astronómico Hispano Alemán (CAHA) at Calar Alto, operated jointly by the Max-Planck Institut für Astronomie and the Instituto de Astrofı́sica de Andalucı́a (CSIC) Nordic Optical Telescope, operated on the island of La Palma jointly by Denmark, Finland, Iceland, Norway, and Sweden, in the Spanish Observatorio del Roque de los Muchachos of the Instituto de Astrofı́sica de Canarias IRAF is distributed by the National Optical Astronomy Observatories, which are operated by the Association of Universities for Research in Astronomy, Inc., under cooperative agreement with the National Science Foundation Sab S0 Scd Sbc 0.2 Irr 0.2 E Irr 0.25 Sab S0 Dı́az, C., et al. Scd Sbc 4 N/Ntot N/Ntot 0.15 0.15 0.1 0.05 0.05 0 0.1 0 0 0.5 1 1.5 2 0 u-b 0.5 1 u-r 1.5 2 Fig. 2. Normalized histograms for the u − B and u − r colors. Median, first and third quartiles are shown at the top of each panel. Mean values for morphological types according to Fukugita et al. (1995). minimizing the area of sky also included. Object fluxes were determined as an average of several measurements with at least two different polygons, taking also into account the Poisson noise, the uncertainty in the sky determination, the readout noise of the CCD and the errors associated to the Bouguer fit to compute the final error for each galaxy magnitude determination. At the end of the process, we compute apparent total galaxy magnitudes within an error interval of 0.15 mag, with a mean error of 0.05 mag. The apparent magnitudes were converted into absolute magnitudes. Galactic extinction correction was applied (Schlegel et al., 1998); K-correction are small at the redshifts of the galaxies and a linear dependency with z is enough for our purposes. Internal extinction correction is not applied. We also compute u − B and u − r colors. 3.3 Effective radii and concentration indexes The effective radius is the one containing half of the total light of a galaxy. We have calculated an equivalent half light radius in arcsec by measuring the flux of the galaxy inside circular apertures and selecting the one containing half of the light. The value in kpc is computed considering the concordance cosmology values (H0 = 70 km s−1 Mpc−1 , ΩM = 0.3, ΩΛ = 0.7). A similar process allows to measure radius containing several percentages of total flux and to compute the light concentration indexes c31 and c42 : r75 r80 c31 = ; c42 = 5 log (2) r25 r20 4 Data analysis and results In figure 2 we plot the histograms for u − B, u − r colors. By comparing with mean colors in Fukugita et al. (1995), we can see that the colors for the UCM Properties in the u band of local star-forming galaxies 1.5 0.25 S0 Sa Sb Sc+ INT BCD 0.2 E S0 Sab 0.15 Sbc Sc+ Scd Sa B-r N/Ntot 1 0.1 0.5 INT Sb BCD 0.05 0 5 Irr 0 -24-23-22-21-20-19-18-17-16-15-14-13 Mu 0 0.5 1 1.5 2 u-B Fig. 3. u absolute magnitude histogram and B −r vs. u−B color-color plot. Dashed line is the separation early - late types found by Strateva et al. (2001). Ellipses show mean and std deviation values for Hubble types. Mean values of Fukugita et al. (1995) (red). The arrow marks mean dust correction following Calzetti et al. (2000). galaxies are those typical for intermediate and late spiral. Figure 3 shows the u absolute magnitudes and the u − B vs. u − r color-color plot; UCM galaxies are located were expected for late type galaxies, according to studies involving thousand of galaxies of the SDSS survey (Strateva et al., 2001). The values of effective radii and concentration indexes at the u0 band are directly comparable to previous measurements of these parameters at larger wavelenghts (B, Pérez-González et al. 2001; r, Vitores et al. 1996b). Figure 4 shows the histograms for effective radii and concentration index c31 in the three bands, and table 1 includes the mean values, for the spectroscopic disklike and HII-like galaxy types and the whole subsample. The young stars, responsible for the most of the luminosity at the u band, are mainly located at the central regions of the galaxies, as pointed by the low values for ref f ; concentration indexes c31 and c42 have however lower values than in bluer bands. This two facts point to a different correlation between these structural parameters and morphological types (usually performed with the values at B band) and has to be taken into account in studies involving high-z galaxies. Table 1. Statistic on surface photometry of UCM galaxies. r1/2 (kpc) c31 c42 u B r u B r u B r Disk-like 1.48 ± 0.10 5.86 ± 0.38 5.09 ± 0.33 2.97 ± 0.13 3.36 ± 0.09 3.18 ± 0.08 2.85 ± 0.10 3.21 ± 0.06 3.07 ± 0.05 HII-like 1.19 ± 0.15 4.03 ± 0.27 3.55 ± 0.17 2.49 ± 0.18 3.48 ± 0.12 3.07 ± 0.11 2.41 ± 0.19 3.31 ± 0.08 2.98 ± 0.08 Total 1.39 ± 0.09 5.16 ± 0.27 4.49 ± 0.23 3.22 ± 0.39 3.40 ± 0.07 3.12 ± 0.06 2.80 ± 0.11 3.25 ± 0.05 3.02 ± 0.04 6 Dı́az, C., et al. 0.20 u 0.30 u 0.15 0.20 0.10 0.10 0.05 0.00 0.00 0.15 B 0.15 N/Ntot N/Ntot 0.20 0.10 0.05 0.05 0.00 0.30 0.00 0.25 r 0.25 r 0.20 0.20 0.15 0.15 0.10 0.10 0.05 0.05 0.00 B 0.10 0 1 2 3 4 5 Reff (kpc) 6 7 8 0.00 1 2 3 4 5 c31 6 7 8 Fig. 4. Normalized histograms for the effective radii and concentration indexes. References Alonso, O., Garcı́a-Dabó, C. 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