38 research outputs found

    On the ages of bright galaxies 500\sim 500 Myr after the Big Bang: insights into star formation activity at z15z \gtrsim 15 with JWST

    Full text link
    With JWST, new opportunities to study the formation and evolution of galaxies in the early Universe are now emerging. Spitzer constraints on rest-optical properties of z7z \gtrsim 7 galaxies demonstrated the power of using stellar masses and star formation histories (SFHs) of galaxies to indirectly infer the star formation history of the Universe. However, only the brightest individual objects at z8z \gtrsim 8 could be detected with Spitzer, making it difficult to robustly constrain past activity at z10z \gtrsim 10. Here, we leverage the greatly improved rest-optical sensitivity of JWST at z8z \gtrsim 8 to constrain the ages and SFHs of eleven UV-bright (MUV19.5M_\text{UV} \lesssim -19.5) galaxies selected to lie at z8.511z \sim 8.5 - 11, then investigate implications for star formation activity at z15z \gtrsim 15. We infer the properties of individual objects in our sample with two spectral energy distribution modelling codes, then infer a distribution of ages for bright z8.511z \sim 8.5 - 11 galaxies. We find a median age of 30\sim 30 Myr, younger than that inferred at z7z \sim 7 with a similar analysis, which is consistent with an evolution towards larger specific star formation rates at early times. The age distribution suggests that only 9\sim 9 percent of bright z8.511z \sim 8.5 - 11 galaxies would be similarly luminous at z15z \gtrsim 15, implying that the number density of bright galaxies declines by approximately an order of magnitude between z8.511z \sim 8.5 - 11 and z15z \sim 15. This evolution is challenging to reconcile with some early JWST results suggesting that the abundance of bright galaxies does not significantly decrease towards very early times, but we suggest this tension may be eased if young stellar populations form on top of older stellar components, or if bright galaxies at z15z \sim 15 are observed during a burst of star formation.Comment: 13 pages, 9 figure

    Insight from JWST/NIRCam into galaxy overdensities around bright Lyα\alpha emitters during reionization: implications for ionized bubbles at z9z \sim 9

    Full text link
    Several studies have detected Lyman-alpha (Lyα\alpha) from bright (MUV21.5M_\mathrm{UV}\lesssim-21.5) galaxies during the early stages of reionization despite the significantly neutral intergalactic medium. To explain these detections, it has been suggested that z>7z>7 Lyα\alpha emitters (LAEs) inhabit physical Mpc (pMpc)-scale ionized regions powered by overdensities of faint galaxies, but systematic searches for these overdensities near LAEs have been challenging. Here, we use CEERS JWST/NIRCam imaging to search for large-scale galaxy overdensities near two very UV-bright, z=8.7z=8.7 LAEs in the EGS field. We colour select 27 z=8.49.1z=8.4-9.1 candidates, including the one LAE in the footprint (EGSY8p7). From SED models, we infer moderately faint UV luminosities (21.2MUV19.1-21.2\lesssim{M_\mathrm{UV}}\lesssim -19.1) and stellar masses of M107.58.8M_*\approx10^{7.5-8.8} M_\odot. All are efficient ionizing agents (ξion1025.526.0\xi_{\mathrm{ion}}^{*}\approx10^{25.5-26.0} Hz erg1^{-1}) and are generally morphologically simple with only one compact (re140r_e\lesssim140 to 650\sim650 pc) star-forming component. 13 candidates lie within 5 arcmin of EGSY8p7, leading to a factor-of-four galaxy overdensity at 5\lesssim 5 arcmin (1.4\sim 1.4 projected pMpc at z8.7z\sim8.7) separations from EGSY8p7. Separations of 101510-15 arcmin (2.74.1\sim2.7-4.1 projected pMpc) are consistent with an average field. The spatial distribution of our sample may qualitatively suggest an R2R\geq2 pMpc ionized bubble encompassing both LAEs in EGS, which is theoretically unexpected but may be possible for a galaxy population 4×4\times more numerous than the average to create with moderate escape fractions (fesc0.15f_\mathrm{esc}\gtrsim0.15) over long times (200\gtrsim200 Myr). Upcoming spectroscopic follow-up will characterize the size of any ionized bubble that may exist and the properties of the galaxies powering such a bubble.Comment: 20 pages, 7 main figures, 3 appendices, accepted to MNRA

    Searching for Extremely Blue UV Continuum Slopes at z=711z=7-11 in JWST/NIRCam Imaging: Implications for Stellar Metallicity and Ionizing Photon Escape in Early Galaxies

    Full text link
    The ultraviolet (UV) continuum slope (β\beta where fλλβ_\lambda\propto \lambda^\beta) of galaxies is sensitive to a variety of properties, from the metallicity and age of the stellar population to the attenuation from dust through the galaxy. Considerable attention has focused on identifying reionization-era galaxies with very blue UV slopes (β<3\beta<-3). Not only do such systems provide a signpost of low metallicity stars, but they also identify galaxies that likely have ionizing photons leaking from their HII regions as such blue UV slopes can only be seen if the reddening effect of nebular continuum has been diminished. In this paper we present a search for reionization-era galaxies with very blue UV colors in recent JWST/NIRCam imaging of the EGS field. We characterize UV slopes for a large sample of z711z\simeq 7-11 galaxies, finding a median value of β=2.1\beta =-2.1. Three of the lower luminosity (MUV19.5_{\rm{UV}}\simeq -19.5) and lower stellar mass (5-6×107\times10^7M_\odot) systems exhibit both extremely blue UV slopes (β=3.1\beta=-3.1 to 3.2-3.2) and rest-optical photometry indicating weak nebular line emission. Each system is very compact (re<_e<260 pc) with very high star formation rate surface densities. We model the SEDs with a suite of BEAGLE models with varying levels of ionizing photon escape. The SEDs cannot be reproduced with our fiducial (fesc,HII_{\rm{esc,HII}}=0) or alpha enhanced (Z<ZISM_*<Z_{\rm{ISM}}) models. The combined blue UV slopes and weak nebular emission are best-fit by models with significant ionizing photon escape from HII regions (fesc,HII_{\rm{esc,HII}}=0.6-0.8) and extremely low metallicity massive stars (Z_*=0.01-0.06 Z_\odot). The discovery of these galaxies highlights the potential for JWST to identify large numbers of candidate Lyman Continuum leaking galaxies in the reionization era and suggests low metallicity stellar populations may be veryComment: 11 pages, 8 figures, 2 tables; Submitted to Ap

    JWST spectroscopy of z58z\sim 5-8 UV-selected galaxies: New constraints on the evolution of the Lyα\alpha escape fraction in the reionization era

    Full text link
    We describe {\it JWST}/NIRSpec prism measurements of Lyα\alpha emission in z5z\gtrsim 5 galaxies. We identify Lyα\alpha detections in 10 out of 69 galaxies with robust rest-optical emission line redshift measurements at 5z<75\leq z<7 in the CEERS and DDT-2750 observations of the EGS field. Galaxies at z6z\simeq 6 with faint continuum (F150W == 27--29 mag) are found with extremely large rest-frame Lyα\alpha equivalent widths (ranging up to 286 A). Likely Lyα\alpha detections are also seen in two new z>7z>7 galaxies (z=z= 7.49 and 7.17) from the second epoch of CEERS observations, both showing large Lyα\alpha equivalent widths that likely indicate significant transmission through the IGM. We measure high Lyα\alpha escape fractions in the 12 Lyα\alpha emitters in our sample (median 0.28), two of which show fescLyαf_{\rm esc}^{ {\rm Ly}\alpha} near unity (>0.80>0.80). We find that 5011+1150_{-11}^{+11}% of z6z\simeq 6 galaxies with [OIII]+Hβ\beta EW >> 1000 A have fescLyαf_{\rm esc}^{ {\rm Ly}\alpha} >0.2>0.2, consistent with the fractions found in lower-redshift samples with matched [OIII]+Hβ\beta EWs. While uncertainties are still significant, we find that only 105+910_{-5}^{+9}% of z>7z>7 galaxies with similarly strong rest optical emission lines show such large fescLyαf_{\rm esc}^{ {\rm Ly}\alpha}, as may be expected if IGM attenuation of Lyα\alpha increases towards higher redshifts. We identify photometric galaxy overdensities near the z7z\gtrsim 7 Lyα\alpha emitters, potentially providing the ionizing flux necessary to create large ionized sightlines that facilitate Lyα\alpha transmission. Finally, we investigate the absence of Lyα\alpha emission in a comparable (and spectroscopically confirmed) galaxy overdensity at z=7.88z=7.88 in the Abell 2744 field, discussing new prism spectra of the field obtained with the UNCOVER program.Comment: main text 20 pages, 13 figures; accepted for publication by MNRA

    A JWST/NIRCam Study of Key Contributors to Reionization: The Star-forming and Ionizing Properties of UV-faint z78z\sim7-8 Galaxies

    Full text link
    Spitzer/IRAC imaging has revealed that the brightest z78z\sim7-8 galaxies often exhibit young ages and strong nebular line emission, hinting at high ionizing efficiency among early galaxies. However, IRAC's limited sensitivity has long hindered efforts to study the fainter, more numerous population often thought largely responsible for reionization. Here we use CEERS JWST/NIRCam data to characterize 116 UV-faint (median MUV=19.5_{UV}=-19.5) z6.58z\sim6.5-8 galaxies. The SEDs are typically dominated by young (\sim10-50 Myr), low-mass (M108 MM_\ast\sim10^8\ M_\odot) stellar populations, and we find no need for extremely high stellar masses (1011M\sim10^{11} M_\odot). Considering previous studies of UV-bright (MUV22_{UV}\sim-22) z78z\sim7-8 galaxies, we find evidence for a strong (5-10×\times) increase in specific star formation rate toward lower luminosities (median sSFR=103 Gyr1^{-1} in CEERS). The larger sSFRs imply a more dominant contribution from OB stars in the relatively numerous UV-faint population, perhaps suggesting that these galaxies are very efficient ionizing agents (median ξion=1025.7\xi_{ion}=10^{25.7} erg1^{-1} Hz). In spite of their much larger sSFRs, we find no significant increase in [OIII]++Hβ\beta EWs towards fainter MUV_{UV} (median \approx780 A˚\mathring{A}). If confirmed, this may indicate that a substantial fraction of our CEERS galaxies possess extremely low metallicities (\lesssim3% ZZ_\odot) where [OIII] emission is suppressed. Alternatively, high ionizing photon escape fractions or bursty star formation histories can also weaken the nebular lines in a subset of our CEERS galaxies. While the majority of our objects are very blue (median β=2.0\beta=-2.0), we identify a significant tail of very dusty galaxies (β1\beta\sim-1) at \approx0.5LUVL_{UV}^\ast which may contribute significantly to the z78z\sim7-8 star formation rate density.Comment: Accepted in MNRAS. Updated to use the most recent NIRCam zeropoints. There are no significant changes to the conclusions relative to v

    JADES: Using NIRCam Photometry to Investigate the Dependence of Stellar Mass Inferences on the IMF in the Early Universe

    Full text link
    The detection of numerous and relatively bright galaxies at redshifts z > 9 has prompted new investigations into the star-forming properties of high-redshift galaxies. Using local forms of the initial mass function (IMF) to estimate stellar masses of these galaxies from their light output leads to galaxy masses that are at the limit allowed for the state of the LambdaCDM Universe at their redshift. We explore how varying the IMF assumed in studies of galaxies in the early universe changes the inferred values for the stellar masses of these galaxies. We infer galaxy properties with the SED fitting code Prospector using varying IMF parameterizations for a sample of 102 galaxies from the JWST Advanced Deep Extragalactic Survey (JADES) spectroscopically confirmed to be at z > 6.7, with additional photometry from the JWST Extragalactic Medium Band Survey (JEMS) for twenty-one galaxies. We demonstrate that models with stellar masses reduced by a factor of three or more do not affect the modeled spectral energy distribution (SED).Comment: The Significance statement is required for PNAS submissio

    JWST Reveals a Possible z ∼ 11 Galaxy Merger in Triply Lensed MACS0647-JD

    Get PDF
    MACS0647–JD is a triply lensed z ∼ 11 galaxy originally discovered with the Hubble Space Telescope. The three lensed images are magnified by factors of ∼8, 5, and 2 to AB mag 25.1, 25.6, and 26.6 at 3.5 μm. The brightest is over a magnitude brighter than other galaxies recently discovered at similar redshifts z > 10 with JWST. Here, we report new JWST imaging that clearly resolves MACS0647–JD as having two components that are either merging galaxies or stellar complexes within a single galaxy. The brighter larger component “A” is intrinsically very blue (β ∼ −2.6 ± 0.1), likely due to very recent star formation and no dust, and is spatially extended with an effective radius ∼70 ± 24 pc. The smaller component “B” (r ∼ 20-+58 pc) appears redder (β ∼ −2 ± 0.2), likely because it is older (100–200 Myr) with mild dust extinction (AV ∼ 0.1 mag). With an estimated stellar mass ratio of roughly 2:1 and physical projected separation ∼400 pc, we may be witnessing a galaxy merger 430 million years after the Big Bang. We identify galaxies with similar colors in a high-redshift simulation, finding their star formation histories to be dissimilar, which is also suggested by the spectral energy distribution fitting, suggesting they formed further apart. We also identify a candidate companion galaxy “C” ∼3 kpc away, likely destined to merge with A and B. Upcoming JWST Near Infrared Spectrograph observations planned for 2023 January will deliver spectroscopic redshifts and more physical properties for these tiny magnified distant galaxies observed in the early universe.We are grateful and indebted to all 20,000 people who worked to make JWST an incredible discovery machine. We dedicate these JWST observations to Rob Hawkins, former lead developer of the Astronomer’s Proposal Tool (APT). Rob lost his life in 2020 November while astronomers around the world were using APT to prepare observations we proposed for JWST Cycle 1. This work is based on observations made with the NASA/ESA/CSA James Webb Space Telescope (JWST) and Hubble Space Telescope (HST). The data were obtained from theMikulski Archive for Space Telescopes (MAST) at the Space Telescope Science Institute (STScI), which is operated by the Association of Universities for Research in Astronomy (AURA), Inc., under NASA contract NAS 5-03127 for JWST. These observations are associated with programs JWST-GO1433 and HST-GO 9722, 10493, 10793, and 12101. T.H. and A. were funded by a grant for JWST-GO-01433 provided by STScI under NASA contract NAS 5-03127. L.W. acknowledges support from the National Science Foundation Graduate Research Fellowship under grant No. DGE-2137419. A.A. acknowledges support from the Swedish Research Council (Vetenskapsrådet project grant No. 2021-05559). P. D. acknowledges support from the NWO grant 016. VIDI.189.162 (“ODIN”) and the European Commission’s and University of Groningen’s CO-FUND Rosalind Franklin program and warmly thanks the Institute for Advanced Study (IAS) Princeton, where a part of this work was carried out, for their generous hospitality and support through the Bershadsky Fund. The Cosmic Dawn Center is funded by the Danish National Research Foundation (DNRF) under grant #140. E.Z. and A.V. ackowledge support from the Swedish National Space Agency. M.B. acknowledges support from the Slovenian national research agency ARRS through grant No. N1-0238. M.O. acknowledges support from JSPS KAKENHI grant Nos. JP22H01260, JP20H05856, JP20H00181, and JP22K21349. A. Z., A.K.M., and L.J.F. acknowledge support by grant No. 2020750 from the United States-Israel Binational Science Foundation (BSF) and grant No. 2109066 from the United States National Science Foundation (NSF), and by the Ministry of Science & Technology, Israel. E.V. and M.N. acknowledge financial support through grant Nos. PRIN-MIUR 2017WSCC32 and 2020SKSTHZ and INAF “main-stream” grant Nos. 1.05.01.86.20 and 1.05.01.86.31. Y.J.-T. acknowl edges financial support from the European Union’s Horizon 2020 research and innovation program under the Marie Sklodowska-Curie grant agreement No. 898633, the MSCA IF Extensions Program of the Spanish National Research Council (CSIC), and the State Agency for Research of the Spanish MCIU through the Center of Excellence Severo Ochoa award to the Instituto de Astrofísica de Andalucía (SEV-2017- 0709). A.C.C. thanks the Leverhulme Trust for their support via a Leverhulme Early Career Fellowshi

    The UV continuum slopes of early star-forming galaxies in JADES

    Get PDF
    © 2024 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society. This is an open access article distributed under the terms of the Creative Commons Attribution License (CC BY), https://creativecommons.org/licenses/by/4.0/The power-law slope of the rest-ultraviolet (UV) continuum (fλ ∝ λβ) is a key metric of early star-forming galaxies, providing one of our only windows into the stellar populations and physical conditions of z ≳ 10 galaxies. Expanding upon previous studies with limited sample sizes, we leverage deep imaging from the JWST Advanced Deep Extragalactic Survey (JADES) to investigate the UV slopes of 179 z ≳ 9 galaxies with apparent magnitudes of mF200W ≃ 26–31, which display a median UV slope of β = −2.4. We compare to a statistical sample of z ≃ 5–9 galaxies, finding a shift towards bluer rest-UV colours at all MUVM_{\rm UV}. The most UV-luminous z ≳ 9 galaxies are significantly bluer than their lower redshift counterparts, representing a dearth of moderately red galaxies within the first 500 Myr. At yet earlier times, the z ≳ 11 galaxy population exhibits very blue UV slopes, implying very low impact from dust attenuation. We identify a robust sample of 44 galaxies with β ≲ −2.8, which have spectral energy distributions requiring models of density-bounded H ii regions and median ionizing photon escape fractions of 0.51 to reproduce. Their rest-optical colours imply that this sample has weaker emission lines (median mF356W − mF444W = 0.19 mag) than typical galaxies (median mF356W − mF444W = 0.39 mag), consistent with the inferred escape fractions. This sample consists of relatively low stellar masses (median log(M/M)=7.5±0.2\log (M/{\rm M}_{\odot })=7.5\pm 0.2), and specific star formation rates (sSFRs; median =79Gyr1=79 \, \rm Gyr^{-1}) nearly twice that of our full galaxy sample (median sSFRs =44Gyr1=44 \, \rm Gyr^{-1}), suggesting these objects are more common among systems experiencing a recent upturn in star formation. We demonstrate that the shutoff of star formation provides an alternative solution for modelling of extremely blue UV colours, making distinct predictions for the rest-optical emission of these galaxies. Future spectroscopy will be required to distinguish between these physical pictures.Peer reviewe

    The UV Continuum Slopes of Early Star-Forming Galaxies in JADES

    Full text link
    The power-law slope of the rest-UV continuum (fλλβf_{\lambda}\propto\lambda^{\beta}) is a key metric of early star forming galaxies, providing one of our only windows into the stellar populations and physical conditions of z>10z>10 galaxies. Expanding upon previous studies with limited sample sizes, we leverage deep imaging from JADES to investigate the UV slopes of 179 z>9z>9 galaxies with apparent magnitudes of mF200W=2631m_{\rm F200W}=26-31, which display a median UV slope of β=2.4\beta=-2.4. We compare to a statistical sample of z=59z=5-9 galaxies, finding a shift toward bluer rest-UV colors at all  MUV\rm~M_{UV}. The most UV-luminous z>9z>9 galaxies are significantly bluer than their lower-redshift counterparts, representing a dearth of moderately-red galaxies in the first 500 500~Myr. At yet earlier times, the z>11z>11 galaxy population exhibits very blue UV slopes, implying very low attenuation from dust. We identify a robust sample of 44 galaxies with β<2.8\beta<-2.8, which have SEDs requiring models of density-bounded HII regions and median ionizing photon escape fractions of 0.510.51 to reproduce. Their rest-optical colors imply that this sample has weaker emission lines (median mF356WmF444W=0.19m_{\rm F356W}-m_{\rm F444W}=0.19 mag) than typical galaxies (median mF356WmF444W=0.39m_{\rm F356W}-m_{\rm F444W}=0.39 mag), consistent with the inferred escape fractions. This sample has relatively low stellar masses (median log(M/M)=7.5\log(M/M_{\odot})=7.5), and specific star-formation rates (median=79/Gyr=79\rm/Gyr) nearly twice that of our full sample (median=44/Gyr=44\rm/Gyr), suggesting they are more common among systems experiencing a recent upturn in star formation. We demonstrate that the shutoff of star formation provides an alternative solution for modelling of extremely blue UV colors, making distinct predictions for the rest-optical emission of these galaxies. Future spectroscopy will be required to distinguish between these physical pictures.Comment: 17 pages, 13 figures; submitted to MNRA
    corecore