1,722,424 research outputs found

    Resolving Clumpy vs. Extended Ly-α\alpha In Strongly Lensed, High-Redshift Ly-α\alpha Emitters

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    We present six strongly gravitationally lensed Ly-α\alpha Emitters (LAEs) at z45z\sim4-5 with HST narrowband imaging isolating Ly-α\alpha. Through complex radiative transfer Ly-α\alpha encodes information about the spatial distribution and kinematics of the neutral hydrogen upon which it scatters. We investigate the galaxy properties and Ly-α\alpha morphologies of our sample. Many previous studies of high-redshift LAEs have been limited in Ly-α\alpha spatial resolution. In this work we take advantage of high-resolution Ly-α\alpha imaging boosted by lensing magnification, allowing us to probe sub-galactic scales that are otherwise inaccessible at these redshifts. We use broadband imaging from HST (rest-frame UV) and Spitzer (rest-frame optical) in SED fitting; providing estimates on the stellar masses (108109M\sim 10^8 - 10^9 M_{\odot}), stellar population ages (t50<40t_{50} <40 Myr), and amounts of dust (AV0.10.6A_V \sim 0.1 - 0.6, statistically consistent with zero). We employ non-parametric star-formation histories to probe the young stellar-populations which create Ly-α\alpha. We also examine the offsets between the Ly-α\alpha and stellar continuum, finding small upper limits of offsets (<0.1"< 0.1") consistent with studies of low-redshift LAEs; indicating our galaxies are not interacting or merging. Finally, we find a bimodality in our sample's Ly-α\alpha morphologies: clumpy and extended. We find a suggestive trend: our LAEs with clumpy Ly-α\alpha are generally younger than the LAEs with extended Ly-α\alpha, suggesting a possible correlation with age.Comment: 17 pages (2 for references), 5 figures, 6 table

    GREEN PEA GALAXIES REVEAL SECRETS OF Ly alpha ESCAPE

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    We analyze archival Ly alpha spectra of 12 "Green Pea" galaxies observed with the Hubble Space Telescope, model their Ly alpha profiles with radiative transfer models, and explore the dependence of the Ly alpha escape fraction on various properties. Green Pea galaxies are nearby compact starburst galaxies with [O III] lambda 5007 equivalent widths (EWs) of hundreds of angstrom. All 12 Green Pea galaxies in our sample show Ly alpha lines in emission, with an Ly alpha EW distribution similar to high-redshift Ly alpha emitters. Combining the optical and UV spectra of Green Pea galaxies, we estimate their Ly alpha escape fractions and find correlations between Ly alpha escape fraction and kinematic features of Ly alpha profiles. The escape fraction of Ly alpha in these galaxies ranges from 1.4% to 67%. We also find that the Ly alpha escape fraction depends strongly on metallicity and moderately on dust extinction. We compare their high-quality Ly alpha profiles with single H I shell radiative transfer models and find that the Ly alpha escape fraction anticorrelates with the derived H I column densities. Single-shell models fit most Ly alpha profiles well, but not the ones with the. highest escape fractions of Ly alpha. Our results suggest that low H I column density and low metallicity are essential for Ly alpha escape. and make a galaxy an Ly alpha emitter.China Scholarship CouncilNSF

    UV & Lyα\alpha halos of Lyα\alpha emitters across environments at z=2.84

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    We present UV and Lyα\alpha radial surface brightness (SB) profiles of Lyα\alpha emitters (LAEs) at z=2.84z=2.84 detected with the Hyper Suprime-Cam (HSC) on the Subaru Telescope. The depth of our data, together with the wide field coverage including a protocluster, enable us to study the dependence of Lyα\alpha halos (LAHs) on various galaxy properties, including Mpc-scale environments. UV and Lyα\alpha images of 3490 LAEs are extracted, and stacking the images yields SB sensitivity of 1×1020 erg s1 cm2 arcsec2\sim1\times10^{-20}\mathrm{~erg~s^{-1}~cm^{-2}~arcsec^{-2}} in Lyα\alpha, reaching the expected level of optically thick gas illuminated by the UV background at z3z\sim3. Fitting of the two-component exponential function gives the scale-lengths of 1.56±0.011.56\pm0.01 and 10.4±0.310.4\pm0.3 pkpc. Dividing the sample according to their photometric properties, we find that while the dependence of halo scale-length on environment outside of the protocluster core is not clear, LAEs in the central regions of protoclusters appear to have very large LAHs which could be caused by combined effects of source overlapping and diffuse Lyα\alpha emission from cool intergalactic gas permeating the forming protocluster core irradiated by active members. For the first time, we identify ``UV halos'' around bright LAEs which are probably due to a few lower-mass satellite galaxies. Through comparison with recent numerical simulations, we conclude that, while scattered Lyα\alpha photons from the host galaxies are dominant, star formation in satellites evidently contributes to LAHs, and that fluorescent Lyα\alpha emission may be boosted within protocluster cores at cosmic noon and/or near bright QSOs.Comment: 29 pages, 20 Figures, Accepted for publication in Ap

    Lyα\alpha Emission at z=713z=7-13: Clear Lyα\alpha Equivalent Width Evolution Indicating the Late Cosmic Reionization History

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    We present the evolution of Lyα\alpha emission derived from 53 galaxies at z=6.613.2z=6.6-13.2 that are identified by multiple JWST/NIRSpec spectroscopy programs of ERS, GO, DDT, and GTO. These galaxies fall on the star-formation main sequence and are the typical star-forming galaxies with UV magnitudes of 22.5MUV17.0-22.5\leq M_\mathrm{UV}\leq-17.0. We find that 15 out of 53 galaxies show Lyα\alpha emission at the >3σ>3\sigma levels, and obtain Lyα\alpha equivalent width (EW) measurements and stringent 3σ3\sigma upper limits for the 15 and 38 galaxies, respectively. Confirming that Lyα\alpha velocity offsets and line widths of our galaxies are comparable with those of low-redshift Lyα\alpha emitters, we investigate the redshift evolution of the Lyα\alpha EW. We find that Lyα\alpha EWs statistically decrease towards high redshifts on the Lyα\alpha EW vs. MUVM_{\rm UV} plane for various probability distributions of the uncertainties. We then evaluate neutral hydrogen fractions xHIx_{\rm HI} with the Lyα\alpha EW redshift evolution and the cosmic reionization simulation results on the basis of a Bayesian inference framework, and obtain xHI<0.79x_{\rm HI}<0.79, =0.620.36+0.15=0.62^{+0.15}_{-0.36}, and 0.930.07+0.040.93^{+0.04}_{-0.07} at z7z\sim7, 88, and 9139-13, respectively. These moderately large xHIx_{\rm HI} values are consistent with the Planck CMB optical depth measurement and previous xHIx_{\rm HI} constraints from galaxy and QSO Lyα\alpha damping wing absorptions, and strongly indicate a late reionization history. Such a late reionization history suggests that major sources of reionization would emerge late and be hosted by moderately massive halos in contrast with the widely-accepted picture of abundant low-mass objects for the sources of reionization.Comment: Accepted for publication in Ap

    The Lyα\alpha non-detection by JWST NIRSpec of a strong Lyα\alpha emitter at z=5.66z=5.66 confirmed by MUSE

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    The detections of Lyman-α\alpha (Lyα\rm Ly\alpha) emission in galaxies with redshifts above 5 are of utmost importance for constraining the cosmic reionization timeline, yet such detections are usually based on slit spectroscopy. Here we investigate the significant bias induced by slit placement on the estimate of Lyα\rm Ly\alpha escape fraction ( fescLyαf_{\rm esc}^{\mathrm{Ly\alpha}}), by presenting a galaxy (dubbed A2744-z6Lya) at z=5.66z=5.66 where its deep JWST NIRSpec prism spectroscopy completely misses the strong Lyα\rm Ly\alpha emission detected in the MUSE data. A2744-z6Lya exhibits a pronounced UV continuum with an extremely steep spectral slope of β=2.5740.008+0.008\beta=-2.574_{-0.008}^{+0.008}, and it has a stellar mass of 108.82 M\mathrm{\sim10^{8.82}~M_\odot}, a star-formation rate of 8.35 Myr1\mathrm{\sim8.35~M_\odot yr^{-1}} and gas-phase metallicity of 12+log(O/H)7.88\mathrm{12+log\,(O/H)\sim7.88}. The observed flux and rest-frame equivalent width of its Lyα\alpha from MUSE spectroscopy are 1.2×1016erg s1cm21.2\times \rm 10^{-16} erg~s^{-1}cm^{-2} and 75\r{A}, equivalent to fescLyα=78±4%f_{\rm esc}^{\mathrm{Ly\alpha}}=78\pm4 \%. However, its Lyα\alpha non-detection from JWST NIRSpec gives a 5-σ\sigma upper limit of <13%<13 \%, in stark contrast to that derived from MUSE. To explore the reasons for this bias, we perform spatially resolved stellar population analysis of A2744-z6Lya using the JWST NIRCam imaging data to construct 2-dimensional maps of SFR, dust extinction and neutral hydrogen column density. We find that the absence of Lyα\alpha in the slit regions probably stems from both the resonance scattering effect of neutral hydrogen and dust extinction. Through analyzing an extreme case in detail, this work highlights the important caveat of inferring fescLyαf_{\rm esc}^{\mathrm{Ly\alpha}} from slit spectroscopy, particularly when using the JWST multiplexed NIRSpec microshutter assembly.Comment: 10 pages, 4 figures, 1 tabl

    Ciii]λ1909\lambda1909 emission as an alternative to Lyα\alpha in the reionization era: the dependence of Ciii] and Lyα\alpha at 3<z<43<z<4 from the VANDELS survey

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    The velocity offset of Lyα\alpha emission from a galaxy's systemic redshift is an excellent tracer of conditions that enable the escape of Lyα\alpha photons from the galaxy, and potentially hydrogen ionizing Lyman continuum photons. However at z6z\geq6, Lyα\alpha is often heavily attenuated by the neutral intergalactic medium. Here we investigate the utility of Ciii],λλ1907,1909\lambda\lambda1907,1909 emission, usually the brightest UV line after Lyα\alpha, as a proxy estimating the Lyα\alpha velocity offset (ΔvLyα\Delta v_{\rm{Ly}\alpha}). To do so, we use analogues of reionization era galaxies based upon 52 star-forming galaxies with robust Ciii] detections drawn from the VANDELS survey. Our sample spans a broad UV magnitude range of 18.5<MUV<22.0-18.5 < M_{\rm{UV}} < -22.0, with a sample average value of EW(Ciii]) =5.3=5.3\,{\AA}. We find a slight increase of EW(Ciii]) with increasing EW(Lyα\alpha), but find a large range of EW(Ciii]) \sim1-13\,{\AA} particularly at EW(Lyα\alpha) <10<10\,{\AA}. Using the Ciii] line peak as the systemic redshift, we calculate ΔvLyα\Delta v_{\rm{Ly}\alpha} and recover the previously reported trend of decreasing ΔvLyα\Delta v_{\rm{Ly}\alpha} with increasing EW(Lyα\alpha). Interestingly, we find an anti-correlation between ΔvLyα\Delta v_{\rm{Ly}\alpha} and EW(Ciii]), which also displays a dependence on the UV absolute magnitude. We derive a multi-variate fit to obtain ΔvLyα\Delta v_{\rm{Ly}\alpha} using both EW(Ciii]) and MUVM_{\rm{UV}}, finding that ΔvLyα\Delta v_{\rm{Ly}\alpha} is more strongly dependent on EW(Ciii]), with a weaker but non-negligible dependence on MUVM_{\rm{UV}}. We find that for a fixed EW(Ciii]), UV-bright Lyα\alpha emitting galaxies show smaller values of ΔvLyα\Delta v_{\rm{Ly}\alpha},which suggests that such galaxies may be undergoing more bursty star-formation compared to the UV-fainter ones, akin to a population of extremely UV-bright galaxies identified at z>10z>10.Comment: 11 pages, 7 figure

    Challenging the LyC-Lyα\alpha relation: strong Lyα\alpha emitters without LyC leakage at z \sim 2.3

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    The escape fraction of LyC ionizing radiation fLyCescf_{LyC}^{esc} is crucial for understanding reionization, yet impossible to measure at z \gtrsim 5.3. Recently, studies have focused on calibrating indirect indicators of fLyCescf_{LyC}^{esc} at z \sim 0.3, finding that Lyα\alpha is closely linked to it. What is still unclear is whether the LyC - Lyα\alpha relation evolves with redshift, and if Lyα\alpha is truly applicable as an fLyCescf_{LyC}^{esc} indicator during the reionization epoch. In this study, we investigate seven 21MUV19-21 \lesssim M_{UV} \lesssim -19 gravitationally lensed galaxies from the BELLS GALLERY survey at z \sim 2.3. Our targets have rest-frame Lyα\alpha equivalent widths ranging from 10 \r{A} to 100 \r{A} and low dust content (2.5β1.9-2.5 \lesssim \beta \lesssim -1.9), both indicative of high LyC escape. Surprisingly, direct estimates of fLyCescf_{LyC}^{esc} using Hubble Space Telescope imaging with F275W and F225W reveal that our targets are not LyC emitters, with absolute fLyCescf_{LyC}^{esc} \lesssim 6.5% at 3σ\sigma significance (with two sources having absolute fLyCescf_{LyC}^{esc}(3σ\sigma) \lesssim 10% and \lesssim 16%). The low fLyCescf_{LyC}^{esc}, coupled with the high Lyα\alpha escape fraction and equivalent width could potentially be attributed to the redshift evolution of the neutral hydrogen column density and dust content. Our results challenge previous studies based on local samples, suggesting that the extrapolation of z ~ 0 Lyα\alpha-based LyC indirect estimators into the reionization epoch might not be correct.Comment: 19 Pages, 8 Figures. Submitted to Ap

    Construction of the Damped Lyα\alpha Absorber Catalog for DESI DR2 Lyα\alpha BAO

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    International audienceWe present the Damped Lyα\alpha Toolkit for automated detection and characterization of Damped Lyα\alpha absorbers (DLA) in quasar spectra. Our method uses quasar spectral templates with and without absorption from intervening DLAs to reconstruct observed quasar forest regions. The best-fitting model determines whether a DLA is present while estimating the redshift and HI column density. With an optimized quality cut on detection significance (Δχr2>0.03\Delta \chi_{r}^2>0.03), the technique achieves an estimated 72% purity and 71% completeness when evaluated on simulated spectra with S/N>2>2 that are free of broad absorption lines (BAL). We provide a catalog containing candidate DLAs from the DLA Toolkit detected in DESI DR1 quasar spectra, of which 21,719 were found in S/N>2>2 spectra with predicted log10(NHI)>20.3\log_{10} (N_\texttt{HI}) > 20.3 and detection significance Δχr2>0.03\Delta \chi_{r}^2 >0.03. We compare the Damped Lyα\alpha Toolkit to two alternative DLA finders based on a convolutional neural network (CNN) and Gaussian process (GP) models. We present a strategy for combining these three techniques to produce a high-fidelity DLA catalog from DESI DR2 for the Lyα\alpha forest baryon acoustic oscillation measurement. The combined catalog contains 41,152 candidate DLAs with log10(NHI)>20.3\log_{10} (N_\texttt{HI}) > 20.3 from quasar spectra with S/N>2>2. We estimate this sample to be approximately 76% pure and 71% complete when BAL quasars are excluded

    On the origin of metallicity in ly alpha forest systems

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    Restricted Access. An open-access version is available at arXiv.org (one of the alternative locations)We investigate the hypothesis that Ly alpha absorption lines arise in two populations of halos---minihalos of small circular velocity (Vc <~ 55 km s-1), in which star formation and metal production are inhibited by photoionization of the UV background radiation, and large galactic halos (55 <~ Vc <~ 250 km s-1) that contain stars and metals. Based on the model of Ly alpha -absorbing gas confined in both populations of halos, we attempt to explain the recent observations of (1) associations of visible galaxies with Ly alpha lines at low redshifts z <~ 1 and (2) metal lines associated with a nonnegligible fraction of low H I column density Ly alpha lines at z ~ 3. For galactic halos, we find that photoionized gas clouds confined in the pressure of ambient hot gas can produce Ly alpha absorption for H I column densities as low as 1014 cm-2 and that the impact parameter of a sight line for such absorptions matches well with the observed radius of the gaseous envelope of a typical luminous galaxy. Using the Press-Schechter prescription for the mass function of halos, we also show that the fraction of Ly alpha lines with associated metal lines can be understood in terms of the fraction of Ly alpha absorbers associated with galactic halos. In particular, the reported fraction of ~0.5--0.75 at z ~ 3 is reproduced when the boundary value of Vc to separate minihalos or galactic halos is 40--60 km s-1, which is consistent with the theoretical prediction of galaxy formation under photoionization. The average metallicity of both Ly alpha forest and damped Ly alpha systems at z ~ 3 is explained in terms of the model of halo-formation history combined with the age-metallicity relationship of Galactic halo stars. Possible methods to test this hypothesis and alternative scenarios are also discussed
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