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The geometry of the neutral gas in and around galaxies is a key regulator of the escape of ionizing photons. We present the first statistical study aimed at linking the neutral and ionized gas distributions to the Lyman continuum (LyC) escape fraction ( in a sample of 22 confirmed LyC leakers and non-leakers at $z using the Keck Cosmic Web Imager (Keck/KCWI) and the Low Resolution Spectrograph 2 (HET/LRS2). Our integral field unit data enable the detection of neutral and low-ionization gas, as traced by Mg ii and ionized gas, as traced by O ii extending beyond the stellar continuum for seven and ten objects, respectively. All but one object with extended Mg ii emission also show extended O ii emission; in this case Mg ii emission is always more extended than O ii by a factor 1.2 on average. Most of the galaxies with extended emission are non or weak LyC leakers ( < 5<!PCT!>), but we find a large diversity of neutral and low-ionization gas configurations around these weakly LyC-emitting galaxies. Conversely, the strongest leakers ( > 5<!PCT!>) appear uniformly compact in both Mg ii and O ii with exponential scale lengths lesssim 1 kpc. Most are unresolved at the resolution of our data. We also find a trend between and the spatial offsets of the nebular gas and the stellar continuum emission. Moreover, we find significant anticorrelations between the spatial extent of the neutral and/or low-ionization gas and the O iii O ii ratio, and Hbeta equivalent width, as well as positive correlations with metallicity and UV size, suggesting that galaxies with more compact neutral and/or low-ionization gas sizes are more highly ionized. The observations suggest that strong LyC emitters do not have extended neutral and/or low-ionization gas halos and ionizing photons may be emitted in many directions. Combined with high ionization diagnostics, we propose that the Mg ii and potentially O ii spatial compactness are indirect indicators of LyC emitting galaxies at high redshift.
The geometry of the neutral gas in and around galaxies is a key regulator of the escape of ionizing photons. We present the first statistical study aimed at linking the neutral and ionized gas distributions to the Lyman continuum (LyC) escape fraction ( in a sample of 22 confirmed LyC leakers and non-leakers at $z using the Keck Cosmic Web Imager (Keck/KCWI) and the Low Resolution Spectrograph 2 (HET/LRS2). Our integral field unit data enable the detection of neutral and low-ionization gas, as traced by Mg ii and ionized gas, as traced by O ii extending beyond the stellar continuum for seven and ten objects, respectively. All but one object with extended Mg ii emission also show extended O ii emission; in this case Mg ii emission is always more extended than O ii by a factor 1.2 on average. Most of the galaxies with extended emission are non or weak LyC leakers ( < 5<!PCT!>), but we find a large diversity of neutral and low-ionization gas configurations around these weakly LyC-emitting galaxies. Conversely, the strongest leakers ( > 5<!PCT!>) appear uniformly compact in both Mg ii and O ii with exponential scale lengths lesssim 1 kpc. Most are unresolved at the resolution of our data. We also find a trend between and the spatial offsets of the nebular gas and the stellar continuum emission. Moreover, we find significant anticorrelations between the spatial extent of the neutral and/or low-ionization gas and the O iii O ii ratio, and Hbeta equivalent width, as well as positive correlations with metallicity and UV size, suggesting that galaxies with more compact neutral and/or low-ionization gas sizes are more highly ionized. The observations suggest that strong LyC emitters do not have extended neutral and/or low-ionization gas halos and ionizing photons may be emitted in many directions. Combined with high ionization diagnostics, we propose that the Mg ii and potentially O ii spatial compactness are indirect indicators of LyC emitting galaxies at high redshift.
Dusty star-forming galaxies (DSFGs) at z > 2 have been commonly observed in overdense regions, where the merging processes and large halo masses induce rapid gas accretion, triggering star formation rates (SFRs) up to ∼1000 M⊙ yr−1. Despite the importance of these DSFGs for understanding star formation in the early Universe, their stellar distributions, traced by the near-infrared (near-IR) emission, had remained spatially unresolved until the arrival of the JWST. In this work, we present, for the first time, a spatially resolved morphological analysis of the rest-frame near-IR (∼1.1–3.5 μm) emission in DSFGs traced with the JWST/MIRI F560W, F770W, F1280W, and F1800W filters. In particular, we studied the mature stellar component for the three DSFGs and a Lyman-break galaxy (LBG) present in an overdensity at z = 4.05. Moreover, we used these rest-frame near-IR images along with ultraviolet (UV) and (sub)-mm ancillary photometric data to model their spectral energy distributions (SEDs) and extract their main physical properties (e.g. M*, SFR, AV). The sub-arcsec resolution images from the JWST have revealed that the light distributions in these galaxies present a wide range of morphologies, from disc-like to compact and clump-dominated structures. Two DSFGs and the LBG are classified as late-type galaxies (LTGs) according to non-parametric morphological indices, while the remaining DSFG is an early-type galaxy (ETG). These near-IR structures contrast with their ultraviolet emission, which is diffuse and, in GN20 and GN20.2b, off-centred by ∼4 kpc. This result suggests that star formation takes place across the entire galaxy, while the UV light traces only those regions where the otherwise high internal extinction decreases significantly. The SED fitting analysis yields large SFRs (∼300–2500 M⊙ yr−1), large stellar masses (M* = (0.24–1.79) × 1011 M⊙), and high integrated extinction values (AV = 0.8–1.5 mag) for our galaxies. In particular, we observe that GN20 dominates the total SFR with a value 2550 ± 150 M⊙ yr−1, while GN20.2b has the highest stellar mass (M* = (2.2 ± 1.4) × 1011 M⊙). The two DSFGs classified as LTGs (GN20 and GN20.2a) have a high specific SFR (sSFR > 30 Gyr−1), placing them above the star-forming main sequence (SFMS) at z ∼ 4 by ∼0.5 dex; whereas the ETG (i.e. GN20.2b) is compatible with the high-mass end of the main sequence. In comparison with other DSFGs in overdensities at z ∼ 2–7, we observe that our objects present similar SFRs, depletion times, and projected separations. Nevertheless, the sizes computed for GN20 and GN20.2a are up to two times larger than those of isolated galaxies observed in CEERS and ALMA-HUDF at similar redshifts. We interpret this difference in size as an effect of rapid growth induced by the dense environment.
The study of gas-phase metallicity and its spatial distribution at high redshift is crucial to understand the processes that shaped the growth and evolution of galaxies in the early Universe. Here we study the spatially resolved metallicity in three systems at $z$ sim 6--8, namely and with JWST NIRSpec IFU low-resolution ($R$ sim 100) spectroscopic observations. These are among the highest-$z$ sources in which metallicity gradients have been probed so far. Each of these systems hosts several spatial components in the process of merging within a few kiloparsecs, identified from the rest-frame UV and optical stellar continuum and ionised gas emission line maps. The sources have heterogeneous properties, with stellar masses log($M_*/M_ sim 7.6--9.3, star formation rates (SFRs) sim 1--15 $M_ $, and gas-phase metallicities 12+log(O/H) sim 7.7--8.3, which exhibit a large scatter within each system. Their properties are generally consistent with those of the highest-redshift samples to date ($z$ sim 3--10), though the sources in and are at the high end of the mass-metallicity relation (MZR) defined by the $z$ sim 3--10 sources. Moreover, the targets in this work follow the predicted slope of the MZR at $z$ sim 6--8 from most cosmological simulations. The gas-phase metallicity gradients are consistent with being flat in the main sources of each system. Flat metallicity gradients are thought to arise from gas mixing processes on galaxy scales, such as mergers or galactic outflows and supernova winds driven by intense stellar feedback, which wash out any gradient formed in the galaxy. The existence of flat gradients at $z$ sim 6--8 sets also important constraints on future cosmological simulations and chemical evolution models, whose predictions on the cosmic evolution of metallicity gradients often differ significantly, especially at high redshift, but are mostly limited to z lesssim 3 so far.
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