15 research outputs found

    A 1.4 deg^2 blind survey for CII], CIII] and CIV at z~0.7-1.5. I:Nature, morphologies and equivalent widths

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    While traditionally associated with active galactic nuclei (AGN), the properties of the CII], CIII] and CIV emission lines are still uncertain as large, unbiased samples of sources are scarce. We present the first blind, statistical study of CII], CIII] and CIV emitters at z∼0.68,1.05,1.53z\sim0.68,1.05,1.53, respectively, uniformly selected down to a flux limit of ∼4×10−17\sim4\times10^{-17} erg s−1^{-1} cm−1^{-1} through a narrow band survey covering an area of ∼1.4\sim1.4 deg2^2 over COSMOS and UDS. We detect 16 CII], 35 CIII] and 17 CIV emitters, whose nature we investigate using optical colours as well as HST, X-ray, radio and far infra-red data. We find that z∼0.7z\sim0.7 CII] emitters are consistent with a mixture of blue (UV slope β=−2.0±0.4\beta=-2.0\pm0.4) star forming galaxies with disky HST structure and AGN with Seyfert-like morphologies. Bright CII] emitters have individual X-ray detections as well as high average black hole accretion rates (BHAR) of ∼0.1\sim0.1 M⊙M_{\odot} yr−1^{-1}. CIII] emitters at z∼1.05z\sim1.05 trace a general population of SF galaxies, with β=−0.8±1.1\beta=-0.8\pm1.1, a variety of optical morphologies, including isolated and interacting galaxies and low BHAR (

    A 1.4 deg2 blind survey for C II], C III] and C IV at z ∼ 0.7–1.5:II. Luminosity functions and cosmic average line ratios

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    Recently, the CIII] and CIV emission lines have been observed in galaxies in the early Universe (z>5z>5), providing new ways to measure their redshift and study their stellar populations and AGN. We explore the first blind CII], CIII] and CIV survey (z∼0.68,1.05,1.53z\sim0.68, 1.05, 1.53, respectively) presented in Stroe et al. (2017). We derive luminosity functions (LF) and study properties of CII], CIII] and CIV line emitters through comparisons to the LFs of Hα\alpha and Lyα\alpha emitters, UV selected star forming (SF) galaxies and quasars at similar redshifts. The CII] LF at z∼0.68z\sim0.68 is equally well described by a Schechter or a power-law LF, characteristic of a mixture of SF and AGN activity. The CIII] LF (z∼1.05z\sim1.05) is consistent to a scaled down version of the Schechter Hα\alpha and Lyα\alpha LF at their redshift, indicating a SF origin. In stark contrast, the CIV LF at z∼1.53z\sim1.53 is well fit by a power-law, quasar-like LF. We find that the brightest UV sources ($M_{UV

    SOFIA/HAWC+ Detection of a Gravitationally Lensed Starburst Galaxy at z = 1.03

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    We present the detection at 89 μm (observed frame) of the Herschel-selected gravitationally lensed starburst galaxy HATLAS J1429-0028 (also known as G15v2.19) in 15 minutes with the High-resolution Airborne Wideband Camera-plus (HAWC+) onboard the Stratospheric Observatory for Infrared Astronomy (SOFIA). The spectacular lensing system consists of an edge-on foreground disk galaxy at z = 0.22 and a nearly complete Einstein ring of an intrinsic ultra-luminous infrared (IR) galaxy at z = 1.03. Is this high IR luminosity powered by pure star formation (SF) or also an active galactic nucleus (AGN)? Previous nebular line diagnostics indicate that it is star formation dominated. We perform a 27-band multiwavelength spectral energy distribution (SED) modeling including the new SOFIA/HAWC+ data to constrain the fractional AGN contribution to the total IR luminosity. The AGN fraction in the IR turns out to be negligible. In addition, J1429-0028 serves as a testbed for comparing SED results from different models/templates and SED codes (magphys, sed3fit, and cigale). We stress that star formation history is the dominant source of uncertainty in the derived stellar mass (as high as a factor of ~10) even in the case of extensive photometric coverage. Furthermore, the detection of a source at z ~ 1 with SOFIA/HAWC+ demonstrates the potential of utilizing this facility for distant galaxy studies including the decomposition of SF/AGN components, which cannot be accomplished with other current facilities

    The OTELO survey: A case study of [O III] lambda 4959,5007 emitters at z=0.83

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    Context. The OSIRIS Tunable Filter Emission Line Object (OTELO) survey is a very deep, blind exploration of a selected region of the Extended Groth Strip and is designed for finding emission-line sources (ELSs). The survey design, observations, data reduction, astrometry, and photometry, as well as the correlation with ancillary data used to obtain a final catalogue, including photo-z estimates and a preliminary selection of ELS, were described in a previous contribution. Aims. Here, we aim to determine the main properties and luminosity function (LF) of the [O III] ELS sample of OTELO as a scientific demonstration of its capabilities, advantages, and complementarity with respect to other surveys. Methods. The selection and analysis procedures of ELS candidates obtained using tunable filter pseudo-spectra are described. We performed simulations in the parameter space of the survey to obtain emission-line detection probabilities. Relevant characteristics of [O III] emitters and the LF ([O III]), including the main selection biases and uncertainties, are presented. Results. From 541 preliminary emission-line source candidates selected around z = 0.8, a total of 184 sources were confirmed as [O III] emitters. Consistent with simulations, the minimum detectable line flux and equivalent width in this ELS sample are ∼5 × 10−19 erg s−1 cm2 and ∼6 Å, respectively. We are able to constrain the faint-end slope (α = −1.03 ± 0.08) of the observed LF ([O III]) at a mean redshift of z = 0.83. This LF reaches values that are approximately ten times lower than those from other surveys. The vast majority (84%) of the morphologically classified [O III] ELSs are disc-like sources, and 87% of this sample is comprised of galaxies with stellar masses of M⋆ <  1010 M⊙

    Spitzer catalog of Herschel-selected ultrared dusty, star-forming galaxies

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    The largest Herschel extragalactic surveys, H-ATLAS and HerMES, have selected a sample of "ultrared" dusty, star-forming galaxies (DSFGs) with rising SPIRE flux densities (S500>S350>S250S_{500} > S_{350} > S_{250}; so-called "500 μ\mum-risers") as an efficient way for identifying DSFGs at higher redshift (z>4z > 4). In this paper, we present a large Spitzer follow-up program of 300 Herschel ultrared DSFGs. We have obtained high-resolution ALMA, NOEMA, and SMA data for 63 of them, which allow us to securely identify the Spitzer/IRAC counterparts and classify them as gravitationally lensed or unlensed. Within the 63 ultrared sources with high-resolution data, ∼\sim65% appear to be unlensed, and ∼\sim27% are resolved into multiple components. We focus on analyzing the unlensed sample by directly performing multi-wavelength spectral energy distribution (SED) modeling to derive their physical properties and compare with the more numerous z∼2z \sim 2 DSFG population. The ultrared sample has a median redshift of 3.3, stellar mass of 3.7 ×\times 1011^{11} M⊙M_{\odot}, star formation rate (SFR) of 730 M⊙M_{\odot}yr−1^{-1}, total dust luminosity of 9.0 ×\times 1012^{12} L⊙L_{\odot}, dust mass of 2.8 ×\times 109^9 M⊙M_{\odot}, and V-band extinction of 4.0, which are all higher than those of the ALESS DSFGs. Based on the space density, SFR density, and stellar mass density estimates, we conclude that our ultrared sample cannot account for the majority of the star-forming progenitors of the massive, quiescent galaxies found in infrared surveys. Our sample contains the rarer, intrinsically most dusty, luminous and massive galaxies in the early universe that will help us understand the physical drivers of extreme star formation
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