Abstract
We report a reanalysis of a near-pristine absorption system, located at a redshift
toward the quasar Q1243+307, based on the combination of archival and new data obtained with the HIRES ...echelle spectrograph on the Keck telescope. This absorption system, which has an oxygen abundance O/H = −2.769 ± 0.028 (≃1/600 of the solar abundance), is among the lowest metallicity systems currently known where a precise measurement of the deuterium abundance is afforded. Our detailed analysis of this system concludes, on the basis of eight D
i
absorption lines, that the deuterium abundance of this gas cloud is
, which is in very good agreement with the results previously reported by Kirkman et al., but with an improvement on the precision of this single measurement by a factor of ∼3.5. Combining this new estimate with our previous sample of six high precision and homogeneously analyzed D/H measurements, we deduce that the primordial deuterium abundance is
or, expressed as a linear quantity,
this value corresponds to a one percent determination of the primordial deuterium abundance. Combining our result with a big bang nucleosynthesis (BBN) calculation that uses the latest nuclear physics input, we find that the baryon density derived from BBN agrees to within 2
σ
of the latest results from the
Planck
cosmic microwave background data.
We use photoionization models that are designed to reconcile the joint rest-UV-optical spectra of high-z star-forming galaxies to self-consistently infer the gas chemistry and nebular ionization and ...excitation conditions for ∼150 galaxies from the Keck Baryonic Structure Survey (KBSS), using only observations of their rest-optical nebular spectra. We find that the majority of z ∼ 2-3 KBSS galaxies are moderately O-rich, with an interquartile range in 12 + log(O/H) = 8.29-8.56, and have significantly sub-solar Fe enrichment, with an interquartile range of Fe/H = −0.79, −0.53, which contributes additional evidence in favor of super-solar O/Fe in high-z galaxies. The model-inferred ionization parameters and N/O are strongly correlated with common strong-line indices (such as O32 and N2O2), with the latter exhibiting similar behavior to local extragalactic H ii regions. In contrast, diagnostics commonly used for measuring gas-phase O/H (such as N2 and O3N2) show relatively large scatter with the overall amount of oxygen present in the gas and behave differently than observed at z ∼ 0. We provide a new calibration for using R23 to measure O/H in typical high-z galaxies, although it is most useful for relatively O-rich galaxies; combining O32 and R23 does not yield a more effective calibration. Finally, we consider the implications for the intrinsic correlations between physical conditions across the galaxy sample and find that N/O varies with O/H in high-z galaxies in a manner that is almost identical to local H ii regions. However, we do not find a strong anti-correlation between ionization parameter and metallicity (O/H or Fe/H) in high-z galaxies, which is one of the principal bases for using strong-line ratios to infer oxygen abundance.
Abstract
We present results of a deep spectroscopic survey quantifying the statistics of the escape of ionizing radiation from star-forming galaxies at
z
∼ 3. We measure the ratio of ionizing to ...non-ionizing UV flux density
, where
f
900
is the mean flux density evaluated over the range 880, 910 Å. We quantify the emergent ratio of ionizing to non-ionizing UV flux density by analyzing high signal-to-noise ratio composite spectra formed from subsamples with common observed properties and numbers sufficient to reduce the statistical uncertainty in the modeled IGM+CGM correction to obtain precise values of
, including a full-sample average
= 0.057 ± 0.006. We show that
increases monotonically with
, inducing an inverse correlation with UV luminosity as a by-product. We fit the composite spectra using stellar spectral synthesis together with models of the ISM in which a fraction
f
c
of the stellar continuum is covered by gas with column density
. We show that the composite spectra simultaneously constrain the intrinsic properties of the stars (
L
900
/
L
1500
)
int
along with
f
c
,
,
, and
f
esc,abs
, the absolute escape fraction of ionizing photons. We find a sample-averaged
f
esc,abs
= 0.09 ± 0.01, with subsamples falling along a linear relation
. Using the far-UV luminosity function, the distribution function
n
(
W
(Ly
α
)), and the relationship between
and
, we estimate the total ionizing emissivity of
z
∼ 3 star-forming galaxies with
M
uv
≤ −19.5, which exceeds the contribution of quasi-stellar objects by a factor of ∼3, and accounts for ∼50% of the total
ϵ
LyC
at
z
∼ 3 estimated using indirect methods.
We present a combined analysis of rest-frame far-UV (FUV; 1000-2000 A) and rest-frame optical (3600-7000 A) composite spectra formed from very deep Keck/LRIS and Keck/MOSFIRE observations of a sample ...of 30 star-forming galaxies with z= 2.40 + or - 0.11, selected to be broadly representative of the full KBSS-MOSFIRE spectroscopic survey. Since the same massive stars are responsible for the observed FUV continuum and for the excitation of the observed nebular emission, a self-consistent stellar population synthesis model should simultaneously match the details of the FUV stellar+nebular continuum and-when inserted as the excitation source in photoionization models-predict all observed nebular emission line ratios. We find that only models including massive star binaries, having low stellar metallicity ( Zlow */Z sub(middot in circle)Asymptotically = to 0.1) but relatively high nebular (ionized gas-phase) abundances ( Z sub(nch)/Zmid dot in circle sub(middot in circle)Asymptotically = to 0.5), can successfully match all of the observational constraints. We show that this apparent discrepancy is naturally explained by highly super-solar O/Fe (Asymptotically = to4-5 (O/Fe)Asymptotically = to), expected for a gas whose enrichment is dominated by the products of core-collapse supernovae. While O dominates the physics of the ionized gas (and thus the nebular emission lines), Fe dominates the extreme-UV (EUV) and FUV opacity and controls the mass-loss rate from massive stars, resulting in particularly dramatic effects for massive stars in binary systems. This high nebular excitation-caused by the hard EUV spectra of Fe-poor massive stars-is much more common at high redshift (z> ~ 2) than low redshift due to systematic differences in the star formation history of typical galaxies.
We report new observations of SL2S J021737-051329, a lens system consisting of a bright arc at z = 1.84435, magnified ∼17× by a massive galaxy at z = 0.65. SL2S0217 is a low-mass (M < 109 M ), ...low-metallicity (Z ∼ 1/20 Z ) galaxy, with extreme star-forming conditions that produce strong nebular UV emission lines in the absence of any apparent outflows. Here we present several notable features from rest-frame UV Keck/LRIS spectroscopy: (1) Very strong narrow emission lines are measured for C iv λλ1548, 1550, He ii λ1640, O iii λλ1661, 1666, Si iii λλ1883, 1892, and C iii λλ1907, 1909. (2) Double-peaked Ly emission is observed with a dominant blue peak and centered near the systemic velocity. (3) The low- and high-ionization absorption features indicate very little or no outflowing gas along the sight line to the lensed galaxy. The relative emission-line strengths can be reproduced with a very high ionization, low-metallicity starburst with binaries, with the exception of He ii, which indicates that an additional ionization source is needed. We rule out large contributions from active galactic nuclei and shocks to the photoionization budget, suggesting that the emission features requiring the hardest radiation field likely result from extreme stellar populations that are beyond the capabilities of current models. Therefore, SL2S0217 serves as a template for the extreme conditions that are important for reionization and thought to be more common in the early universe.
We present the first spectroscopic measurements of the shape of the far-ultraviolet (far-UV; lambda = 950-1500 A) dust attenuation curve at high redshift (z~ 3). Our analysis employs rest-frame UV ...spectra of 933 galaxies at z~ 3, 121 of which have very deep spectroscopic observations (> ~7 hr) at lambda = 850-1300 A, with the Low Resolution Imaging Spectrograph on the Keck Telescope. By using an iterative approach in which we calculate the ratios of composite spectra in different bins of continuum color excess, E(B- V), we derive a dust curve that implies a lower attenuation in the far-UV for a given E(B- V) than those obtained with standard attenuation curves. We demonstrate that the UV composite spectra of z~ 3 galaxies can be modeled well by assuming our new attenuation curve, a high covering fraction of H I, and absorption from the Lyman-Werner bands of H sub(2) with a small (< ~20%) covering fraction. The low covering fraction of H sub(2) relative to that of the H sub(1) and dust suggests that most of the dust in the ISM of typical galaxies at z~ 3 is unrelated to the catalysis of H sub(2), and is associated with other phases of the ISM (i.e., the ionized and neutral gas). The far-UV dust curve implies a factor of thickapproximate2 lower dust attenuation of Lyman continuum (ionizing) photons relative to those inferred from the most commonly assumed attenuation curves for L* galaxies at z~ 3. Our results may be utilized to assess the degree to which ionizing photons are attenuated in H II regions or, more generally, in the ionized or low column density (N(H I) < ~ 10 super(17,2) cm super(-2)) neutral ISM of high-redshift galaxies.
Using a large sample of spectroscopically confirmed z~ 3 galaxies, we establish an empirical relationship between reddening (E(B- V)), neutral gas covering fraction (f sub(cov)(H I)), and the escape ...of ionizing (Lyman continuum, LyC) photons. Our sample includes 933 galaxies at z~ 3, 121 of which have deep spectroscopic observations (> ~7 hr) at 850 < ~ lambda sub(rest)< ~ 1300 A with the Low Resolution Imaging Spectrograph on Keck. The high covering fraction of outflowing optically thick H i indicated by the composite spectra of these galaxies implies that photoelectric absorption, rather than dust attenuation, dominates the depletion of LyC photons. By modeling the composite spectra as the combination of an unattenuated stellar spectrum including nebular continuum emission with one that is absorbed by H 1 and reddened by a line-of-sight extinction, we derive an empirical relationship between E(B- V) and f sub(cov)(H 1). Galaxies with redder UV continua have larger covering fractions of H 1 characterized by higher line-of-sight extinctions. We develop a model which connects the ionizing escape fraction with E(B- V), and which may be used to estimate the ionizing escape fraction for an ensemble of galaxies. Alternatively, direct measurements of the escape fraction for our sample allow us to constrain the intrinsic LyC-to-UV flux density ratio to be left angle bracket S(900 A)/S(1500 A)right angle bracket sub(int)> ~ 0.20, a value that favors stellar population models that include weaker stellar winds, a flatter initial mass function, and/or binary evolution. Last, we demonstrate how the framework discussed here may be used to assess the pathways by which ionizing radiation escapes from high-redshift galaxies.
ABSTRACT
We present near-infrared observations of 42 gravitationally lensed galaxies obtained in the framework of the KMOS Lensed Emission Lines and VElocity Review (KLEVER) Survey, a programme aimed ...at investigating the spatially resolved properties of the ionized gas in 1.2 < z < 2.5 galaxies by means of a full coverage of the YJ, H, and K near-infrared bands. Detailed metallicity maps and gradients are derived for a subsample of 28 galaxies from reconstructed source-plane emission-line maps, exploiting the variety of different emission-line diagnostics provided by the broad wavelength coverage of the survey. About $85 {{\, per\ cent}}$ of these galaxies are characterized by metallicity gradients shallower than $0.05\ \rm dex\, kpc^{-1}$ and $89{{\ \rm per\ cent}}$ are consistent with a flat slope within 3σ ($67{{\ \rm per\ cent}}$ within 1σ), suggesting a mild evolution with cosmic time. In the context of cosmological simulations and chemical evolution models, the presence of efficient feedback mechanisms and/or extended star formation profiles on top of the classical ‘inside-out’ scenario of mass assembly is generally required to reproduce the observed flatness of the metallicity gradients beyond z ∼ 1. Three galaxies with significantly (>3σ) ‘inverted’ gradients are also found, showing an anticorrelation between metallicity and star formation rate density on local scales, possibly suggesting recent episodes of pristine gas accretion or strong radial flows in place. Nevertheless, the individual metallicity maps are characterized by a variety of different morphologies, with flat radial gradients sometimes hiding non-axisymmetric variations on kpc scales, which are washed out by azimuthal averages, especially in interacting systems or in those undergoing local episodes of recent star formation.
We present a survey for metal absorption systems traced by neutral oxygen over 3.2 < z < 6.5. Our survey uses Keck/ESI and VLT/X-Shooter spectra of 199 QSOs with redshifts up to 6.6. In total, we ...detect 74 O i absorbers, of which 57 are separated from the background QSO by more than 5000 km s−1. We use a maximum likelihood approach to fit the distribution of O i λ1302 equivalent widths in bins of redshift and from this determine the evolution in number density of absorbers with W1302 > 0.05 , of which there are 49 nonproximate systems in our sample. We find that the number density does not monotonically increase with decreasing redshift, as would naively be expected from the buildup of metal-enriched circumgalactic gas with time. The number density over 4.9 < z < 5.7 is a factor of 1.7-4.1 lower (68% confidence) than that over 5.7 < z < 6.5, with a lower value at z < 5.7 favored with 99% confidence. This decrease suggests that the fraction of metals in a low-ionization phase is larger at z ∼ 6 than at lower redshifts. Absorption from highly ionized metals traced by C iv is also weaker in higher-redshift O i systems, supporting this picture. The evolution of O i absorbers implies that metal-enriched circumgalactic gas at z ∼ 6 is undergoing an ionization transition driven by a strengthening ultraviolet background. This in turn suggests that the reionization of the diffuse intergalactic medium may still be ongoing at or only recently ended by this epoch.
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