L. Wisotzki
American Institute of Physics
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Astronomy and Astrophysics | 2003
Christian Wolf; L. Wisotzki; Andrea Borch; S. Dye; M. Kleinheinrich; Klaus Meisenheimer
We present a determination of the optical/UV AGN luminosity function and its evolution, based on a large sample of faint (R< 24) QSOs identified in the COMBO-17 survey. Using multi-band photometry in 17 filters within 350 nm < obs < 930 nm, we could simultaneously determine photometric redshifts with an accuracy of z < 0:03 and obtain spectral energy distributions. The redshift range covered by the sample is 1:2 < z < 4:8, which implies that even at z 3, the sample reaches below luminosities corresponding to MB= 23, conventionally employed to distinguish between Seyfert galaxies and quasars. We clearly detect a broad plateau-like maximum of quasar activity around z 2 and map out the smooth turnover between z 1a ndz 4. The shape of the LF is characterised by some mild curvature, but no sharp break is present within the range of luminosities covered. Using only the COMBO-17 data, the evolving LF can be adequately described by either a pure density evolution (PDE) or a pure luminosity evolution (PLE) model. However, the absence of a strong L-like feature in the shape of the LF inhibits a robust distinction between these modes. We present a robust estimate for the integrated UV luminosity generation by AGN as a function of redshift. We find that the LF continues to rise even at the lowest luminosities probed by our survey, but that the slope is suciently shallow that the contribution of low-luminosity AGN to the UV luminosity density is negligible. Although our sample reaches much fainter flux levels than previous data sets, our results on space densities and LF slopes are completely consistent with extrapolations from recent major surveys such as SDSS and 2QZ.
Astronomy and Astrophysics | 2013
S. F. Sánchez; F. F. Rosales-Ortega; Bruno Jungwiert; J. Iglesias-Páramo; J. M. Vílchez; R. A. Marino; C. J. Walcher; B. Husemann; D. Mast; A. Monreal-Ibero; R. Cid Fernandes; Emmanuelle Perez; R. M. González Delgado; R. García-Benito; L. Galbany; G. van de Ven; Knud Jahnke; H. Flores; Joss Bland-Hawthorn; A. R. Lopez-Sanchez; V. Stanishev; Daniel Miralles-Caballero; Angeles I. Díaz; P. Sánchez-Blázquez; M. Mollá; Anna Gallazzi; P. Papaderos; J. M. Gomes; N. Gruel; Isabel Pérez
We studied the global and local ℳ-Z relation based on the first data available from the CALIFA survey (150 galaxies). This survey provides integral field spectroscopy of the complete optical extent of each galaxy (up to 2−3 effective radii), with a resolution high enough to separate individual Hu2009II regions and/or aggregations. About 3000 individual Hu2009II regions have been detected. The spectra cover the wavelength range between [OII]3727 and [SII]6731, with a sufficient signal-to-noise ratio to derive the oxygen abundance and star-formation rate associated with each region. In addition, we computed the integrated and spatially resolved stellar masses (and surface densities) based on SDSS photometric data. We explore the relations between the stellar mass, oxygen abundance and star-formation rate using this dataset. We derive a tight relation between the integrated stellar mass and the gas-phase abundance, with a dispersion lower than the one already reported in the literature (σ_Δlogu2009(O/H) = 0.07 dex). Indeed, this dispersion is only slightly higher than the typical error derived for our oxygen abundances. However, we found no secondary relation with the star-formation rate other than the one induced by the primary relation of this quantity with the stellar mass. The analysis for our sample of ~3000 individual Hu2009II regions confirms (i) a local mass-metallicity relation and (ii) the lack of a secondary relation with the star-formation rate. The same analysis was performed with similar results for the specific star-formation rate. Our results agree with the scenario in which gas recycling in galaxies, both locally and globally, is much faster than other typical timescales, such like that of gas accretion by inflow and/or metal loss due to outflows. In essence, late-type/disk-dominated galaxies seem to be in a quasi-steady situation, with a behavior similar to the one expected from an instantaneous recycling/closed-box model.
Astronomy and Astrophysics | 2014
C. J. Walcher; L. Wisotzki; S. Bekeraite; B. Husemann; J. Iglesias-Páramo; N. Backsmann; J. Barrera Ballesteros; Cristina Catalán-Torrecilla; C. Cortijo; A. del Olmo; B. García Lorenzo; J. Falcón-Barroso; Lucie Jílková; V. Kalinova; D. Mast; R. A. Marino; J. Méndez-Abreu; Anna Pasquali; S. F. Sánchez; Scott Trager; S. Zibetti; J. A. L. Aguerri; J. Alves; Joss Bland-Hawthorn; A. Boselli; A. Castillo Morales; R. Cid Fernandes; H. Flores; L. Galbany; Anna Gallazzi
We describe and discuss the selection procedure and statistical properties of the galaxy sample used by the Calar Alto Legacy Integral Field Area (CALIFA) survey, a public legacy survey of 600 galaxies using integral field spectroscopy. The CALIFA mother sample was selected from the Sloan Digital Sky Survey (SDSS) DR7 photometric catalogue to include all galaxies with an r-band isophotal major axis between 45 and 79 : 2 and with a redshift 0 : 005 M-r > -23 : 1 and over a stellar mass range between 10(9.7) and 10(11.4) M-circle dot. In particular, within these ranges, the diameter selection does not lead to any significant bias against - or in favour of - intrinsically large or small galaxies. Only below luminosities of M-r = -19 (or stellar masses < 10(9.7) M-circle dot) is there a prevalence of galaxies with larger isophotal sizes, especially of nearly edge-on late-type galaxies, but such galaxies form < 10% of the full sample. We estimate volume-corrected distribution functions in luminosities and sizes and show that these are statistically fully compatible with estimates from the full SDSS when accounting for large-scale structure. For full characterization of the sample, we also present a number of value-added quantities determined for the galaxies in the CALIFA sample. These include consistent multi-band photometry based on growth curve analyses; stellar masses; distances and quantities derived from these; morphological classifications; and an overview of available multi-wavelength photometric measurements. We also explore different ways of characterizing the environments of CALIFA galaxies, finding that the sample covers environmental conditions from the field to genuine clusters. We finally consider the expected incidence of active galactic nuclei among CALIFA galaxies given the existing pre-CALIFA data, finding that the final observed CALIFA sample will contain approximately 30 Sey2 galaxies.
Astronomy and Astrophysics | 2014
P. Sánchez Blázquez; F. F. Rosales Ortega; J. Méndez Abreu; I. Pérez; S. F. Sánchez; S. Zibetti; J. A. L. Aguerri; Joss Bland-Hawthorn; Cristina Catalán Torrecilla; R. Cid Fernandes; A. L. de Amorim; A. de Lorenzo Cáceres; J. Falcón Barroso; A. Galazzi; R. García Benito; Armando Gil de Paz; R. M. González Delgado; B. Husemann; Jorge Iglesias Paramo; Bruno Jungwiert; R. A. Marino; I. Márquez; D. Mast; M. A. Mendoza; M. Mollá; P. Papaderos; T. Ruiz Lara; G. van de Ven; C. J. Walcher; L. Wisotzki
While studies of gasphase metallicity gradients in disc galaxies are common, very little has been done towards the acquisition of stellar abundance gradients in the same regions. We present here a comparative study of the stellar metallicity and age distributions in a sample of 62 nearly face-on, spiral galaxies with and without bars, using data from the CALIFA survey. We measure the slopes of the gradients and study their relation with other properties of the galaxies. We find that the mean stellar age and metallicity gradients in the disc are shallow and negative. Furthermore, when normalized to the effective radius of the disc, the slope of the stellar population gradients does not correlate with the mass or with the morphological type of the galaxies. In contrast to this, the values of both age and metallicity at similar to 2.5 scale lengths correlate with the central velocity dispersion in a similar manner to the central values of the bulges, although bulges show, on average, older ages and higher metallicities than the discs. One of the goals of the present paper is to test the theoretical prediction that non-linear coupling between the bar and the spiral arms is an efficient mechanism for producing radial migrations across significant distances within discs. The process of radial migration should flatten the stellar metallicity gradient with time and, therefore, we would expect flatter stellar metallicity gradients in barred galaxies. However, we do not find any difference in the metallicity or age gradients between galaxies with and without bars. We discuss possible scenarios that can lead to this lack of difference.
The Astrophysical Journal | 2009
Anna Gallazzi; Eric F. Bell; Christian Wolf; Meghan E. Gray; Casey Papovich; Marco Barden; Chien Y. Peng; Klaus Meisenheimer; Catherine Heymans; Eelco van Kampen; Rachel Gilmour; M. Balogh; Daniel H. McIntosh; David Bacon; Fabio D. Barazza; Asmus Boehm; John A. R. Caldwell; Boris Haeussler; Knud Jahnke; Shardha Jogee; Kyle Lane; Aday R. Robaina; Sebastian F. Sanchez; Andy Taylor; L. Wisotzki; Xianzhong Zheng
We explore the amount of obscured star formation as a function of environment in the Abell 901/902 (A901/902) supercluster at z = 0.165 in conjunction with a field sample drawn from the A901 and CDFS fields, imaged with the Hubble Space Telescope as part of the Space Telescope A901/902 Galaxy Evolution Survey and Galaxy Evolution from Morphology and Spectral Energy Distributions (SEDs) Survey. We combine the combo-17 near-UV/optical SED with Spitzer 24 mu m photometry to estimate both the unobscured and obscured star formation in galaxies with M(*) > 10(10) M(circle dot). We find that the star formation activity in massive galaxies is suppressed in dense environments, in agreement with previous studies. Yet, nearly 40% of the star-forming (SF) galaxies have red optical colors at intermediate and high densities. These red systems are not starbursting; they have star formation rates (SFRs) per unit stellar mass similar to or lower than blue SF galaxies. More than half of the red SF galaxies have low infrared-to-ultraviolet (IR-to-UV) luminosity ratios, relatively high Sersicindices, and they are equally abundant at all densities. They might be gradually quenching their star formation, possibly but not necessarily under the influence of gas-removing environmental processes. The other greater than or similar to 40% of the red SF galaxies have high IR-to-UV luminosity ratios, indicative of high dust obscuration. They have relatively high specific SFRs and are more abundant at intermediate densities. Our results indicate that while there is an overall suppression in the SF galaxy fraction with density, the small amount of star formation surviving the cluster environment is to a large extent obscured, suggesting that environmental interactions trigger a phase of obscured star formation, before complete quenching.
The Astrophysical Journal | 2004
Knud Jahnke; Sebastian F. Sanchez; L. Wisotzki; Marco Barden; Steven V. W. Beckwith; Eric F. Bell; Andrea Borch; J. A. R. Caldwell; Boris Häussler; Catherine Heymans; S. Jogee; Daniel H. McIntosh; Klaus Meisenheimer; C. Y. Peng; H.-W. Rix; Rachel S. Somerville; Christian Wolf
We have performed Hubble Space Telescope imaging of a sample of 23 high-redshift (1.8 < z < 2.75) active galactic nuclei (AGNs), drawn from the COMBO-17 survey. The sample contains moderately luminous quasars (MB ~ -23). The data are part of the Galaxy Evolution from Morphologies and SEDs imaging survey that provides high-resolution optical images obtained with the Advanced Camera for Surveys in two bands (F606W and F850LP), sampling the rest-frame UV flux of the targets. To deblend the AGN images into nuclear and resolved (host galaxy) components, we use a point-spread function subtraction technique that is strictly conservative with respect to the flux of the host galaxy. We resolve the host galaxies in both filter bands in nine of the 23 AGNs, whereas the remaining 14 objects are considered nondetections, with upper limits of less than 5% of the nuclear flux. However, when we co-add the unresolved AGN images into a single high signal-to-noise ratio composite image, we find again an unambiguously resolved host galaxy. The recovered host galaxies have apparent magnitudes of 23.0 < F606W < 26.0 and 22.5 < F850LP < 24.5, with rest-frame UV colors in the range -0.2 < (F606W - F850LP)obs < 2.3. The rest-frame absolute magnitudes at 200 nm are -20.0 < M200 nm < -22.2. The photometric properties of the composite host are consistent with the individual resolved host galaxies. We find that the UV colors of all host galaxies are substantially bluer than expected from an old population of stars with formation redshift z ≤ 5, independent of the assumed metallicities. These UV colors and luminosities range up to the values found for Lyman break galaxies (LBGs) at z = 3. Our results suggest either a recent starburst of, e.g., a few percent of the total stellar mass at 100 Myr before observation, with mass fraction and age strongly degenerate, or the possibility that the detected UV emission may be due to young stars forming continuously. For the latter case we estimate star formation rates of typically ~6 M☉ yr-1 (uncorrected for internal dust attenuation), which again lies in the range of rates implied from the UV flux of LBGs. Our results agree with the recent discovery of enhanced blue stellar light in AGN hosts at lower redshifts.
Astronomy and Astrophysics | 2014
R. M. González Delgado; Emmanuelle Perez; R. Cid Fernandes; R. García-Benito; A. L. de Amorim; S. F. Sánchez; B. Husemann; C. Cortijo-Ferrero; R. López Fernández; P. Sánchez-Blázquez; S. Bekeraite; C. J. Walcher; J. Falcón-Barroso; Anna Gallazzi; G. van de Ven; J. Alves; Joss Bland-Hawthorn; Robert C. Kennicutt; D. Kupko; Mariya Lyubenova; D. Mast; M. Mollá; R. A. Marino; A. Quirrenbach; J. M. Vílchez; L. Wisotzki
We have studied the radial structure of the stellar mass surface density (μ∗) and stellar population age as a function of the total stellar mass and morphology for a sample of 107 galaxies from the CALIFA survey. We applied the fossil record method based on spectral synthesis techniques to recover the star formation history (SFH), resolved in space and time, in spheroidal and disk dominated galaxies with masses from 10^9 to 10^12 M_⊙. We derived the half-mass radius, and we found that galaxies are on average 15% more compact in mass than in light. The ratio of half-mass radius to half-light radius (HLR) shows a dual dependence with galaxy stellar mass; it decreases with increasing mass for disk galaxies, but is almost constant in spheroidal galaxies. In terms of integrated versus spatially resolved properties, we find that the galaxy-averaged stellar population age, stellar extinction, and μ_∗ are well represented by their values at 1 HLR. Negative radial gradients of the stellar population ages are present in most of the galaxies, supporting an inside-out formation. The larger inner (≤1 HLR) age gradients occur in the most massive (10^11 M_⊙) disk galaxies that have the most prominent bulges; shallower age gradients are obtained in spheroids of similar mass. Disk and spheroidal galaxies show negative μ∗ gradients that steepen with stellar mass. In spheroidal galaxies, μ∗ saturates at a critical value (~7 × 10^2 M_⊙/pc^2 at 1 HLR) that is independent of the galaxy mass. Thus, all the massive spheroidal galaxies have similar local μ_∗ at the same distance (in HLR units) from the nucleus. The SFH of the regions beyond 1 HLR are well correlated with their local μ_∗, and follow the same relation as the galaxy-averaged age and μ_∗; this suggests that local stellar mass surface density preserves the SFH of disks. The SFH of bulges are, however, more fundamentally related to the total stellar mass, since the radial structure of the stellar age changes with galaxy mass even though all the spheroid dominated galaxies have similar radial structure in μ_∗. Thus, galaxy mass is a more fundamental property in spheroidal systems, while the local stellar mass surface density is more important in disks.
The Astrophysical Journal | 2005
Christian Wolf; Eric F. Bell; Daniel H. McIntosh; H.-W. Rix; Marco Barden; Steven V. W. Beckwith; Andrea Borch; J. A. R. Caldwell; Boris Häussler; Catherine Heymans; Knud Jahnke; S. Jogee; Klaus Meisenheimer; C. Y. Peng; Sebastian F. Sanchez; Rachel S. Somerville; L. Wisotzki
We combine high-resolution images from GEMS with redshifts and spectral energy distributions from COMBO-17 to explore the morphological types of galaxies that dominate the z ~ 0.7 UV luminosity density. We analyzed rest-frame 280 nm and V-band luminosities of 1483 galaxies with 0.65 < z < 0.75, combining these with visual morphological classifications from F850LP images (approximately rest-frame V band) taken with HST ACS on the Extended Chandra Deep Field-South. We derive UV luminosity functions and j280 luminosity densities for spheroid-dominated galaxies, spiral galaxies, Magellanic irregular galaxies, and clearly interacting galaxies with morphologies suggestive of ongoing major mergers. We check the reliability of GEMS morphologies against the deeper GOODS images and quantify an incompleteness of the GEMS merger identification at the faint end. We derive the fractions of the global UV luminosity density j280 originating from the galaxy types and find that spiral and Magellanic irregular galaxies dominate with about 40% each. Interacting and merging galaxies account for roughly 20% of j280, while the contribution of early types is negligible. These results imply that the strong decline in the UV luminosity density of the universe observed from z ~ 1 until today is dominated by the decreasing UV luminosities of normal spiral galaxies, accompanied by the migration of UV-luminous star formation in irregular galaxies to systems of progressively lower mass and luminosity. These conclusions suggest that major-merger-driven star formation cannot dominate the declining cosmic star formation rate, unless major mergers are substantially more obscured than intensely star-forming spiral galaxies and the decline in observed cosmic star formation rate is substantially stronger than the already precipitous decline in uncorrected UV luminosity density.
Astronomy and Astrophysics | 2006
L. Christensen; Knud Jahnke; L. Wisotzki; S. F. Sánchez
Context. Quasars trace the most massive structures at high redshifts and their presence may influence the evolution of the massive host galaxies. Aims. We study the extended Lyα emission line regions (EELRs) around seven bright, mostly radio-quiet quasars (QSOs) at 2.7 < z < 4.5, and compare luminosities with EELRs around radio-loud QSOs reported in the literature. Methods. Using integral field spectroscopy, we analyse the morphology and kinematics of the quiescent Lya EELRs around the QSOs. Results. We find evidence for the presence of EELRs around four radio-quiet and one radio-loud QSO. All EELRs appear asymmetric and the optically brightest QSOs also have the brightest Lya nebulae. For the two brightest nebulae we find velocities between ∼600 km s -1 at the QSO position to ∼200 km s -1 at a distance of 3-4 from the QSO and surface flux densities up to 2-3 x 10 -16 erg cm -2 s -1 arcsec -2 . The five EELRs have total Lyα luminosities which correspond to ∼0.5% of the luminosities from the QSOs broad Lyα emission lines. This fraction is an order of magnitude smaller than found for EELRs around radio-loud, steep spectrum QSOs reported in the literature. While the nebulae luminosities are correlated with the QSO Lyα luminosities, we find that nebulae luminosities are not correlated with the central QSO ionising fluxes. Conclusions. The presence of gas in the EELRs can be interpreted based on two competing scenarios: either from quasar feedback mechanisms, or from infalling matter. Apart from these two effects, the Lyα flux around radio-loud objects can be enhanced due to interactions with the radio jets. The relatively fainter nebulae around radio-quiet QSOs compared to lobe-dominated radio-loud QSOs can be ascribed to this effect, or to significant differences in the environments between the two classes.
Nature | 2005
Pierre Magain; Géraldine Letawe; F. Courbin; Pascale Jablonka; Knud Jahnke; G. Meylan; L. Wisotzki
A quasar is thought to be powered by the infall of matter onto a supermassive black hole at the centre of a massive galaxy. Because the optical luminosity of quasars exceeds that of their host galaxy, disentangling the two components can be difficult. This led in the 1990s to the controversial claim of the discovery of ‘naked’ quasars. Since then, the connection between quasars and galaxies has been well established. Here we report the discovery of a quasar lying at the edge of a gas cloud, whose size is comparable to that of a small galaxy, but whose spectrum shows no evidence for stars. The gas in the cloud is excited by the quasar itself. If a host galaxy is present, it is at least six times fainter than would normally be expected for such a bright quasar. The quasar is interacting dynamically with a neighbouring galaxy, whose gas might be feeding the black hole.