396 research outputs found

    Merging galaxies produce outliers from the Fundamental Metallicity Relation

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    From a large sample of ≈170,000\approx 170,000 local SDSS galaxies, we find that the Fundamental Metallicity Relation (FMR) has an overabundance of outliers, compared to what would be expected from a Gaussian distribution of residuals, with significantly lower metallicities than predicted from their stellar mass and star formation rate (SFR). This low-metallicity population has lower stellar masses, bimodial specific SFRs with enhanced star formation within the aperture and smaller half-light radii than the general sample, and is hence a physically distinct population. We show that they are consistent with being galaxies that are merging or have recently merged with a satellite galaxy. In this scenario, low-metallicity gas flows in from large radii, diluting the metallicity of star-forming regions and enhancing the specific SFR until the inflowing gas is processed and the metallicity has recovered. We introduce a simple model in which mergers with a mass ratio larger than a minimum dilute the central galaxy's metallicity by an amount that is proportional to the stellar mass ratio for a constant time, and show that it provides an excellent fit to the distribution of FMR residuals. We find the dilution time-scale to be τ=1.568−0.027+0.029\tau=1.568_{-0.027}^{+0.029} Gyr, the average metallicity depression caused by a 1:1 merger to be α=0.2480−0.0020+0.0017\alpha=0.2480_{-0.0020}^{+0.0017} dex and the minimum mass ratio merger that can be discerned from the intrinsic Gaussian scatter in the FMR to be ξmin=0.2030−0.0095+0.0127\xi_\text{min}=0.2030_{-0.0095}^{+0.0127} (these are statistical errors only). From this we derive that the average metallicity depression caused by a merger with mass ratio between 1:5 and 1:1 is 0.114 dex.Comment: 14 pages, 10 figures, published in MNRAS, updated to be essentially identical to the published versio

    When Does the Intergalactic Medium Become Enriched?

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    We use cosmological hydrodynamic simulations including galactic feedback based on observations of local starbursts to find a self-consistent evolutionary model capable of fitting the observations of the intergalactic metallicity history as traced by C IV between z=6.0->1.5. Our main finding is that despite the relative invariance in the measurement of Omega(C IV) as well as the column density and linewidth distributions over this range, continual feedback from star formation-driven winds are able to reproduce the observations, while an early enrichment scenario where a majority of the metals are injected into the IGM at z>6 is disfavored. The constancy of the C IV observations results from a rising IGM metallicity content balanced by a declining C IV ionization fraction due to a 1) decreasing physical densities, 2) increasing ionization background strength, and 3) metals becoming more shock-heated at lower redshift. Our models predict that ~20x more metals are injected into the IGM between z=6->2 than at z>6. We show that the median C IV absorber at z=2 traces metals injected 1 Gyr earlier indicating that the typical metals traced by C IV are neither from very early times nor from very recent feedback.Comment: 6 pages, 3 figures, to appear in the proceedings of "Chemodynamics: from the First Stars to Local Galaxies", Lyon, France, July 10-14, 200

    Probing the Metal Enrichment of the Intergalactic Medium at z=5−6z=5-6 Using the Hubble Space Telescope

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    We test the galactic outflow model by probing associated galaxies of four strong intergalactic CIV absorbers at z=5z=5--6 using the Hubble Space Telescope (HST) ACS ramp narrowband filters. The four strong CIV absorbers reside at z=5.74z=5.74, 5.525.52, 4.954.95, and 4.874.87, with column densities ranging from NCIV=1013.8N_{\rm{CIV}}=10^{13.8} cm−2^{-2} to 1014.810^{14.8} cm−2^{-2}. At z=5.74z=5.74, we detect an i-dropout Lyα\alpha emitter (LAE) candidate with a projected impact parameter of 42 physical kpc from the CIV absorber. This LAE candidate has a Lyα\alpha-based star formation rate (SFRLyα_{\rm{Ly\alpha}}) of 2 M⊙M_\odot yr−1^{-1} and a UV-based SFR of 4 M⊙M_\odot yr−1^{-1}. Although we cannot completely rule out that this ii-dropout emitter may be an [OII] interloper, its measured properties are consistent with the CIV powering galaxy at z=5.74z=5.74. For CIV absorbers at z=4.95z=4.95 and z=4.87z=4.87, although we detect two LAE candidates with impact parameters of 160 kpc and 200 kpc, such distances are larger than that predicted from the simulations. Therefore we treat them as non-detections. For the system at z=5.52z=5.52, we do not detect LAE candidates, placing a 3-σ\sigma upper limit of SFRLyα≈1.5 M⊙_{\rm{Ly\alpha}}\approx 1.5\ M_\odot yr−1^{-1}. In summary, in these four cases, we only detect one plausible CIV source at z=5.74z=5.74. Combining the modest SFR of the one detection and the three non-detections, our HST observations strongly support that smaller galaxies (SFRLyα≲2 M⊙_{\rm{Ly\alpha}} \lesssim 2\ M_\odot yr−1^{-1}) are main sources of intergalactic CIV absorbers, and such small galaxies play a major role in the metal enrichment of the intergalactic medium at z≳5z\gtrsim5.Comment: Accepted for Publications in ApJ

    Reionization in Technicolor

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    We present the Technicolor Dawn simulations, a suite of cosmological radiation-hydrodynamic simulations of the first 1.2 billion years. By modeling a spatially-inhomogeneous UVB on-the-fly with 24 frequencies and resolving dark matter halos down to 108M⊙10^8 M_\odot within 12 h−1h^{-1} Mpc volumes, our simulations unify observations of the intergalactic and circumgalactic media, galaxies, and reionization into a common framework. The only empirically-tuned parameter, the fraction fesc,gal(z)f_{\mathrm{esc,gal}}(z) of ionizing photons that escape the interstellar medium, is adjusted to match observations of the Lyman-α\alpha forest and the cosmic microwave background. With this single calibration, our simulations reproduce the history of reionization; the stellar mass-star formation rate relation of galaxies; the number density and metallicity of damped Lyman-α\alpha absorbers (DLAs) at z∼5z\sim5; the abundance of weak metal absorbers; the ultraviolet background (UVB) amplitude; and the Lyman-α\alpha flux power spectrum at z=5.4z=5.4. The galaxy stellar mass and UV luminosity functions are underproduced by ≤2×\leq2\times, suggesting an overly vigorous feedback model. The mean transmission in the Lyman-α\alpha forest is underproduced at z<6z<6, indicating tension between measurements of the UVB amplitude and Lyman-α\alpha transmission. The observed SiIV column density distribution is reasonably well-reproduced (∼1σ\sim 1\sigma low). By contrast, CIV remains significantly underproduced despite being boosted by an intense >4>4 Ryd UVB. Solving this problem by increasing metal yields would overproduce both weak absorbers and DLA metallicities. Instead, the observed strength of high-ionization emission from high-redshift galaxies and absorption from their environments suggest that the ionizing flux from conventional stellar population models is too soft.Comment: 24 pages, 17 figures, accepted to MNRA

    The importance of nebular emission for SED modeling of distant star-forming galaxies

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    We highlight and discuss the importance of accounting for nebular emission in the SEDs of high redshift galaxies, as lines and continuum emission can contribute significantly or subtly to broad-band photometry. Physical parameters such as the galaxy age, mass, star-formation rate, dust attenuation and others inferred from SED fits can be affected to different extent by the treatment of nebular emission. We analyse a large sample of Lyman break galaxies from z~3-6, and show some main results illustrating e.g. the importance of nebular emission for determinations of the mass-SFR relation, attenuation and age. We suggest that a fairly large scatter in such relations could be intrinsic. We find that the majority of objects (~60-70%) is better fit with SEDs accounting for nebular emission; the remaining galaxies are found to show relatively weak or no emission lines. Our modeling, and supporting empirical evidence, suggests the existence of two categories of galaxies, "starbursts" and "post-starbursts" (lower SFR and older galaxies) among the LBG population, and relatively short star-formation timescales.Comment: To appear in IAU Symp. 284, The Spectral Energy Distribution of Galaxies, Preston (UK), September 2011, eds. R. J. Tuffs and C. C. Popesc

    The Reionization of Carbon

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    Observations suggest that CII was more abundant than CIV in the intergalactic medium towards the end of the hydrogen reionization epoch. This transition provides a unique opportunity to study the enrichment history of intergalactic gas and the growth of the ionizing background (UVB) at early times. We study how carbon absorption evolves from z=10-5 using a cosmological hydrodynamic simulation that includes a self-consistent multifrequency UVB as well as a well-constrained model for galactic outflows to disperse metals. Our predicted UVB is within 2-4 times that of Haardt & Madau (2012), which is fair agreement given the uncertainties. Nonetheless, we use a calibration in post-processing to account for Lyman-alpha forest measurements while preserving the predicted spectral slope and inhomogeneity. The UVB fluctuates spatially in such a way that it always exceeds the volume average in regions where metals are found. This implies both that a spatially-uniform UVB is a poor approximation and that metal absorption is not sensitive to the epoch when HII regions overlap globally even at column densites of 10^{12} cm^{-2}. We find, consistent with observations, that the CII mass fraction drops to low redshift while CIV rises owing the combined effects of a growing UVB and continued addition of carbon in low-density regions. This is mimicked in absorption statistics, which broadly agree with observations at z=6-3 while predicting that the absorber column density distributions rise steeply to the lowest observable columns. Our model reproduces the large observed scatter in the number of low-ionization absorbers per sightline, implying that the scatter does not indicate a partially-neutral Universe at z=6.Comment: 16 pages, 14 figures, accepted to MNRA
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