202 research outputs found

    The VIMOS Ultra Deep Survey. Luminosity and stellar mass dependence of galaxy clustering at z~3

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    We present the study of the dependence of galaxy clustering on luminosity and stellar mass in the redshift range 2<<z<<3.5 using 3236 galaxies with robust spectroscopic redshifts from the VIMOS Ultra Deep Survey (VUDS). We measure the two-point real-space correlation function wp(rp)w_p(r_p) for four volume-limited stellar mass and four luminosity, MUV_{UV} absolute magnitude selected, sub-samples. We find that the scale dependent clustering amplitude r0r_0 significantly increases with increasing luminosity and stellar mass indicating a strong galaxy clustering dependence on these properties. This corresponds to a strong relative bias between these two sub-samples of Δ\Deltab/b∗^*=0.43. Fitting a 5-parameter HOD model we find that the most luminous and massive galaxies occupy the most massive dark matter haloes with ⟹\langleMh_h⟩\rangle = 1012.30^{12.30} h−1^{-1} M⊙_{\odot}. Similar to the trends observed at lower redshift, the minimum halo mass Mmin_{min} depends on the luminosity and stellar mass of galaxies and grows from Mmin_{min} =109.73^{9.73} h−1^{-1}M⊙_{\odot} to Mmin_{min}=1011.58^{11.58} h−1^{-1}M⊙_{\odot} from the faintest to the brightest among our galaxy sample, respectively. We find the difference between these halo masses to be much more pronounced than is observed for local galaxies of similar properties. Moreover, at z~3, we observe that the masses at which a halo hosts, on average, one satellite and one central galaxy is M1_1≈\approx4Mmin_{min} over all luminosity ranges, significantly lower than observed at z~0 indicating that the halo satellite occupation increases with redshift. The luminosity and stellar mass dependence is also reflected in the measurements of the large scale galaxy bias, which we model as bg,HOD_{g,HOD}(>>L)=1.92+25.36(L/L∗^*)7.01^{7.01}. We conclude our study with measurements of the stellar-to-halo mass ratio (SHMR).Comment: 20 pages, 11 figures, A&A in press, v2. revised discussion in sec. 5.5, changed Fig. 4 and Fig. 11, added reference

    A subarcsecond near-infrared view of massive galaxies at z > 1 with Gemini Multiconjugate Adaptive Optics

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    We present images taken using the Gemini South Adaptive Optics Imager (GSAOI) with the Gemini Multiconjugate Adaptive Optics System (GeMS) in three 2 arcmin2^2 fields in the Spitzer Extragalactic Representative Volume Survey. These GeMS/GSAOI observations are among the first ≈0.1â€Čâ€Č\approx 0.1^{''} resolution data in the near-infrared spanning extragalactic fields exceeding 1.5â€Č1.5^{\prime} in size. We use these data to estimate galaxy sizes, obtaining results similar to those from studies with the Hubble Space Telescope, though we find a higher fraction of compact star forming galaxies at z>2z>2. To disentangle the star-forming galaxies from active galactic nuclei (AGN), we use multiwavelength data from surveys in the optical and infrared, including far-infrared data from Herschel, as well as new radio continuum data from the Australia Telescope Compact Array and Very Large Array. We identify ultraluminous infrared galaxies (ULIRGs) at z∌1−3z \sim 1-3, which consist of a combination of pure starburst galaxies and Active Galactic Nuclei (AGN)/starburst composites. The ULIRGs show signs of recent merger activity, such as highly disturbed morphologies and include a rare candidate triple AGN. We find that AGN tend to reside in hosts with smaller scale sizes than purely star-forming galaxies of similar infrared luminosity. Our observations demonstrate the potential for MCAO to complement the deeper galaxy surveys to be made with the James Webb Space Telescope.Comment: 20 pages, AJ, in pres

    A WFC3 Grism Emission Line Redshift Catalog in the GOODS-South Field

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    We combine HST/WFC3 imaging and G141 grism observations from the CANDELS and 3D-HST surveys to produce a catalog of grism spectroscopic redshifts for galaxies in the CANDELS/GOODS-South field. The WFC3/G141 grism spectra cover a wavelength range of 1.1<lambda<1.7 microns with a resolving power of R~130 for point sources, thus providing rest-frame optical spectra for galaxies out to z~3.5. The catalog is selected in the H-band (F160W) and includes both galaxies with and without previously published spectroscopic redshifts. Grism spectra are extracted for all H-band detected galaxies with H<24 and a CANDELS photometric redshift z_phot > 0.6. The resulting spectra are visually inspected to identify emission lines and redshifts are determined using cross-correlation with empirical spectral templates. To establish the accuracy of our redshifts, we compare our results against high-quality spectroscopic redshifts from the literature. Using a sample of 411 control galaxies, this analysis yields a precision of sigma_NMAD=0.0028 for the grism-derived redshifts, which is consistent with the accuracy reported by the 3D-HST team. Our final catalog covers an area of 153 square arcmin and contains 1019 redshifts for galaxies in GOODS-S. Roughly 60% (608/1019) of these redshifts are for galaxies with no previously published spectroscopic redshift. These new redshifts span a range of 0.677 < z < 3.456 and have a median redshift of z=1.282. The catalog contains a total of 234 new redshifts for galaxies at z>1.5. In addition, we present 20 galaxy pair candidates identified for the first time using the grism redshifts in our catalog, including four new galaxy pairs at z~2, nearly doubling the number of such pairs previously identified.Comment: 25 Pages, 9 Figures, submitted to A

    The evolution of clustering length, large-scale bias and host halo mass at 2<z<5 in the VIMOS Ultra Deep Survey (VUDS)

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    We investigate the evolution of galaxy clustering for galaxies in the redshift range 2.0<zz<5.0 using the VIMOS Ultra Deep Survey (VUDS). We present the projected (real-space) two-point correlation function wp(rp)w_p(r_p) measured by using 3022 galaxies with robust spectroscopic redshifts in two independent fields (COSMOS and VVDS-02h) covering in total 0.8 deg2^2. We quantify how the scale dependent clustering amplitude r0r_0 changes with redshift making use of mock samples to evaluate and correct the survey selection function. Using a power-law model Ο(r)=(r/r0)−γ\xi(r) = (r/r_0)^{-\gamma} we find that the correlation function for the general population is best fit by a model with a clustering length r0r_0=3.95−0.54+0.48^{+0.48}_{-0.54} h−1^{-1}Mpc and slope Îł\gamma=1.8−0.06+0.02^{+0.02}_{-0.06} at zz~2.5, r0r_0=4.35±\pm0.60 h−1^{-1}Mpc and Îł\gamma=1.6−0.13+0.12^{+0.12}_{-0.13} at zz~3.5. We use these clustering parameters to derive the large-scale linear galaxy bias bLPLb_L^{PL}, between galaxies and dark matter. We find bLPLb_L^{PL} = 2.68±\pm0.22 at redshift zz~3 (assuming σ8\sigma_8 = 0.8), significantly higher than found at intermediate and low redshifts. We fit an HOD model to the data and we obtain that the average halo mass at redshift zz~3 is MhM_h=1011.75±0.23^{11.75\pm0.23} h−1^{-1}M⊙_{\odot}. From this fit we confirm that the large-scale linear galaxy bias is relatively high at bLHODb_L^{HOD} = 2.82±\pm0.27. Comparing these measurements with similar measurements at lower redshifts we infer that the star-forming population of galaxies at zz~3 should evolve into the massive and bright (MrM_r<-21.5) galaxy population which typically occupy haloes of mass ⟹Mh⟩\langle M_h\rangle = 1013.9^{13.9} h−1^{-1} M⊙M_{\odot} at redshift zz=0.Comment: 19 pages, 10 figures, submitted to A&

    The VIMOS Ultra Deep Survey: Lyα\alpha Emission and Stellar Populations of Star-Forming Galaxies at 2<z<2.5

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    The aim of this paper is to investigate spectral and photometric properties of 854 faint (iABi_{AB}<~25 mag) star-forming galaxies (SFGs) at 2<z<2.5 using the VIMOS Ultra-Deep Survey (VUDS) spectroscopic data and deep multi-wavelength photometric data in three extensively studied extragalactic fields (ECDFS, VVDS, COSMOS). These SFGs were targeted for spectroscopy based on their photometric redshifts. The VUDS spectra are used to measure the UV spectral slopes (ÎČ\beta) as well as Lyα\alpha equivalent widths (EW). On average, the spectroscopically measured ÎČ\beta (-1.36±\pm0.02), is comparable to the photometrically measured ÎČ\beta (-1.32±\pm0.02), and has smaller measurement uncertainties. The positive correlation of ÎČ\beta with the Spectral Energy Distribution (SED)-based measurement of dust extinction, Es_{\rm s}(B-V), emphasizes the importance of ÎČ\beta as an alternative dust indicator at high redshifts. To make a proper comparison, we divide these SFGs into three subgroups based on their rest-frame Lyα\alpha EW: SFGs with no Lyα\alpha emission (SFGN_{\rm N}; EW≀\le0\AA), SFGs with Lyα\alpha emission (SFGL_{\rm L}; EW>>0\AA), and Lyα\alpha emitters (LAEs; EW≄\ge20\AA). The fraction of LAEs at these redshifts is ∌\sim10%, which is consistent with previous observations. We compared best-fit SED-estimated stellar parameters of the SFGN_{\rm N}, SFGL_{\rm L} and LAE samples. For the luminosities probed here (∌\simL∗^*), we find that galaxies with and without Lyα\alpha in emission have small but significant differences in their SED-based properties. We find that LAEs have less dust, and lower star-formation rates (SFR) compared to non-LAEs. We also find that LAEs are less massive compared to non-LAEs, though the difference is smaller and less significant compared to the SFR and Es_{\rm s}(B-V). [abridged]Comment: Accepted for publication in A&A, 19 pages, 10 figures, 1 tabl

    The VIMOS Ultra Deep Survey First Data Release: spectra and spectroscopic redshifts of 698 objects up to z~6 in CANDELS

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    This paper describes the first data release (DR1) of the VIMOS Ultra Deep Survey (VUDS). The DR1 includes all low-resolution spectroscopic data obtained in 276.9 arcmin2 of the CANDELS-COSMOS and CANDELS-ECFDS survey areas, including accurate spectroscopic redshifts z_spec and individual spectra obtained with VIMOS on the ESO-VLT. A total of 698 objects have a measured redshift, with 677 galaxies, two type-I AGN and a small number of 19 contaminating stars. The targets of the spectroscopic survey are selected primarily on the basis of their photometric redshifts to ensure a broad population coverage. About 500 galaxies have z_spec>2, 48 with z_spec>4, and the highest reliable redshifts reach beyond z_spec=6. This dataset approximately doubles the number of galaxies with spectroscopic redshifts at z>3 in these fields. We discuss the general properties of the sample in terms of the spectroscopic redshift distribution, the distribution of Lyman-alpha equivalent widths, and physical properties including stellar masses M_star and star formation rates (SFR) derived from spectral energy distribution fitting with the knowledge of z_spec. We highlight the properties of the most massive star-forming galaxies, noting the large range in spectral properties, with Lyman-alpha in emission or in absorption, and in imaging properties with compact, multi-component or pair morphologies. We present the catalogue database and data products. All data are publicly available and can be retrieved from a dedicated query-based database available at http://cesam.lam.fr/vuds.Comment: 11 pages, 6 figures, submitted to A&

    The impact of the Star Formation Histories on the SFR-M∗_{*} relation at z≄\ge2

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    In this paper we investigate the impact of different star formation histories (SFHs) on the relation between stellar mass M∗_{*} and star formation rate (SFR) using a sample of galaxies with reliable spectroscopic redshift zspec>2 drawn from the VIMOS Ultra-Deep Survey (VUDS). We produce an extensive database of dusty model galaxies, calculated starting from the new library of single stellar population (SSPs) models presented in Cassara' et al. 2013 and weighted by a set of 28 different SFHs based on the Schmidt function, and characterized by different ratios of the gas infall time scale τinfall\tau_{infall} to the star formation efficiency Îœ\nu. The treatment of dust extinction and re-emission has been carried out by means of the radiative transfer calculation. The spectral energy distribution (SED) fitting technique is performed by using GOSSIP+, a tool able to combine both photometric and spectroscopic information to extract the best value of the physical quantities of interest, and to consider the Intergalactic Medium (IGM) attenuation as a free parameter. We find that the main contribution to the scatter observed in the SFR−M∗SFR-M_{*} plane is the possibility of choosing between different families of SFHs in the SED fitting procedure, while the redshift range plays a minor role. The majority of the galaxies, at all cosmic times, are best-fit by models with SFHs characterized by a high τinfall/Îœ\tau_{\rm infall}/\nu ratio. We discuss the reliability of the presence of a small percentage of dusty and highly star forming galaxies, in the light of their detection in the FIR.Comment: 14 pages, 13 figures, accepted for pubblication in A&

    The Lyman Continuum escape fraction of galaxies at z=3.3 in the VUDS-LBC/COSMOS field

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    The Lyman continuum (LyC) flux escaping from high-z galaxies into the IGM is a fundamental quantity to understand the physical processes involved in the reionization epoch. We have investigated a sample of star-forming galaxies at z~3.3 in order to search for possible detections of LyC photons escaping from galaxy halos. UV deep imaging in the COSMOS field obtained with the prime focus camera LBC at the LBT telescope was used together with a catalog of spectroscopic redshifts obtained by the VIMOS Ultra Deep Survey (VUDS) to build a sample of 45 galaxies at z~3.3 with L>0.5L*. We obtained deep LBC images of galaxies with spectroscopic redshifts in the interval 3.27<z<3.40 both in the R and deep U bands. A sub-sample of 10 galaxies apparently shows escape fractions>28% but a detailed analysis of their properties reveals that, with the exception of two marginal detections (S/N~2) in the U band, all the other 8 galaxies are most likely contaminated by the UV flux of low-z interlopers located close to the high-z targets. The average escape fraction derived from the stacking of the cleaned sample was constrained to fesc_rel<2%. The implied HI photo-ionization rate is a factor two lower than that needed to keep the IGM ionized at z~3, as observed in the Lyman forest of high-z QSO spectra or by the proximity effect. These results support a scenario where high redshift, relatively bright (L>0.5L*) star-forming galaxies alone are unable to sustain the level of ionization observed in the cosmic IGM at z~3. Star-forming galaxies at higher redshift and at fainter luminosities (L<<L*) can be the major contributors to the reionization of the Universe only if their physical properties are subject to rapid changes from z~3 to z~6-10. Alternatively, ionizing sources could be discovered looking for fainter sources among the AGN population at high-z.Comment: 21 pages, 9 figures. Accepted for publication in A&

    Combined analysis of Hubble and VLT photometry of the intermediate mass black hole ESO 243-49 HLX-1

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    In this paper, we present a combined analysis of data obtained with the Hubble Space Telescope (HST), Very Large Telescope (VLT) and Swift X-ray telescope of the intermediate-mass black hole ESO 243-49 HLX-1 that were taken two months apart between 2010 September and November. Previous separate analyses of these data found that they were consistent with an irradiated accretion disc with contribution from either a very young or very old stellar population, and also indicated that the optical flux of the HLX-1 counterpart could be variable. Such variability could only be attributed to a varying accretion disc, so simultaneous analysis of all data sets should break the degeneracies in the model fits. We thus simultaneously fit the broad-band spectral energy distribution (SED) from near-infrared through to X-ray wavelengths of the two epochs of data with a model consisting of an irradiated accretion disc and a stellar population. We show that this combined analysis rules out an old stellar population, finding that the SED is dominated by emission from an accretion disc with moderate reprocessing in the outer disc around an intermediate-mass black hole imbedded in a young (&tilde;20 Myr) stellar cluster with a mass of &tilde;105 M&amp;sun;. We also place an upper limit on the mass of an additional hidden old stellar population of &tilde;106 M&amp;sun;. However, optical r&#39;-band observations of HLX-1 obtained with the Gemini-South telescope covering part of the decay from a later X-ray outburst are consistent with constant optical flux, indicating that the observed variability between the HST and VLT observations could be spurious caused by differences in the background subtraction applied to the two optical data sets. In this scenario, the contribution of the stellar population, and thus the stellar mass of the cluster, may be higher. Nonetheless, variability of &lt;50 per cent cannot be ruled out by the Gemini data and thus they are still consistent within the errors with an exponential decay similar to that observed in X-rays.</p

    NEOWISE Observations of Near-Earth Objects: Preliminary Results

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    With the NEOWISE portion of the \emph{Wide-field Infrared Survey Explorer} (WISE) project, we have carried out a highly uniform survey of the near-Earth object (NEO) population at thermal infrared wavelengths ranging from 3 to 22 ÎŒ\mum, allowing us to refine estimates of their numbers, sizes, and albedos. The NEOWISE survey detected NEOs the same way whether they were previously known or not, subject to the availability of ground-based follow-up observations, resulting in the discovery of more than 130 new NEOs. The survey's uniformity in sensitivity, observing cadence, and image quality have permitted extrapolation of the 428 near-Earth asteroids (NEAs) detected by NEOWISE during the fully cryogenic portion of the WISE mission to the larger population. We find that there are 981±\pm19 NEAs larger than 1 km and 20,500±\pm3000 NEAs larger than 100 m. We show that the Spaceguard goal of detecting 90% of all 1 km NEAs has been met, and that the cumulative size distribution is best represented by a broken power law with a slope of 1.32±\pm0.14 below 1.5 km. This power law slope produces ∌13,200±\sim13,200\pm1,900 NEAs with D>D>140 m. Although previous studies predict another break in the cumulative size distribution below D∌D\sim50-100 m, resulting in an increase in the number of NEOs in this size range and smaller, we did not detect enough objects to comment on this increase. The overall number for the NEA population between 100-1000 m are lower than previous estimates. The numbers of near-Earth comets will be the subject of future work.Comment: Accepted to Ap
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