115 research outputs found

    The [OIII]++Hβ\beta Equivalent Width Distribution at z\simeq7: Implications for the Contribution of Galaxies to Reionization

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    We quantify the distribution of [OIII]+Hβ\beta line strengths at z\simeq7 using a sample of 20 bright (MUV_{\mathrm{UV}} \lesssim -21) galaxies. We select these systems over wide-area fields (2.3 deg2^2 total) using a new colour-selection which precisely selects galaxies at z\simeq6.63-6.83, a redshift range where blue Spitzer/IRAC [3.6]-[4.5] colours unambiguously indicate strong [OIII]++Hβ\beta emission. These 20 galaxies suggest a log-normal [OIII]++Hβ\beta EW distribution with median EW = 759113+112^{+112}_{-113} A˚\mathrm{\mathring{A}} and standard deviation = 0.260.05+0.06^{+0.06}_{-0.05} dex. We find no evidence for strong variation in this EW distribution with UV luminosity. The typical [OIII]+Hβ\beta EW at z\simeq7 implied by our sample is considerably larger than that in massive star forming galaxies at z\simeq2, consistent with a shift toward larger average sSFR (4.4 Gyr1^{-1}) and lower metallicities (0.16 Z_\odot). We also find evidence for the emergence of a population with yet more extreme nebular emission ([OIII]+Hβ\beta EW>>1200 A˚\mathrm{\mathring{A}}) that is rarely seen at lower redshifts. These objects have extremely large sSFR (>>30 Gyr1^{-1}), as would be expected for systems undergoing a burst or upturn in star formation. While this may be a short-lived phase, our results suggest that 20% of the z\simeq7 population has such extreme nebular emission, implying that galaxies likely undergo intense star formation episodes regularly at z>>6. We argue that this population may be among the most effective ionizing agents in the reionization era, both in terms of photon production efficiency and escape fraction. We furthermore suggest that galaxies passing through this large sSFR phase are likely to be very efficient in forming bound star clusters.Comment: 20 pages, 11 figures. Accepted in MNRAS with minor revision

    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

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    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

    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

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    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

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

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    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

    Radio and Far-IR Emission Associated with a Massive Star-forming Galaxy Candidate at z\simeq6.8: A Radio-Loud AGN in the Reionization Era?

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    We report the identification of radio (0.144-3 GHz), mid-IR, far-IR, and sub-mm (24-850μ\mum) emission at the position of one of 41 UV-bright (MUV21.25_\mathrm{UV}^{}\lesssim-21.25) z6.66.9z\simeq6.6-6.9 Lyman-break galaxy candidates in the 1.5 deg2^2 COSMOS field. This source, COS-87259, exhibits a sharp flux discontinuity (factor >>3) between two narrow/intermediate bands at 9450 and 9700 Angstroms and is undetected in all nine bands blueward of 9600 Angstroms, as expected from a Lyman-alpha break at z6.8z\simeq6.8. The full multi-wavelength (X-ray through radio) data of COS-87529 can be self-consistently explained by a very massive (M=1010.8_{\ast}=10^{10.8} M_{\odot}) and extremely red (rest-UV slope β=0.59\beta=-0.59) z6.8z\simeq6.8 galaxy with hyperluminous infrared emission (LIR=1013.6_{\mathrm{IR}}=10^{13.6} L_{\odot}) powered by both an intense burst of highly-obscured star formation (SFR\approx1800 M_{\odot} yr1^{-1}) and an obscured (τ9.7μm=7.7±2.5\tau_{\mathrm{9.7\mu m}}=7.7\pm2.5) radio-loud (L1.4 GHz1025.4_{\mathrm{1.4\ GHz}}\approx10^{25.4} W Hz1^{-1}) AGN. The radio emission is compact (1.04±\pm0.12 arcsec) and exhibits an ultra-steep spectrum between 1.32-3 GHz (α=1.570.21+0.22\alpha=-1.57^{+0.22}_{-0.21}) that flattens at lower frequencies (α=0.860.16+0.22\alpha=-0.86^{+0.22}_{-0.16} between 0.144-1.32 GHz), consistent with known z>4z>4 radio galaxies. We also demonstrate that COS-87259 may reside in a significant (11×\times) galaxy overdensity at z6.66.9z\simeq6.6-6.9, as common for systems hosting radio-loud AGN. Nonetheless, a spectroscopic redshift will ultimately be required to establish the true nature of COS-87259 as we cannot yet completely rule out low-redshift solutions. If confirmed to lie at z6.8z\simeq6.8, the properties of COS-87259 would be consistent with a picture wherein AGN and highly-obscured star formation activity are fairly common among very massive (M>1010_{\ast}>10^{10} M_{\odot}) reionization-era galaxies.Comment: 14 pages, 6 figures. Accepted in MNRAS with minor revisions. This accepted version considers very recent data from LOFAR and MeerKAT which improve our analyses on the radio slope and luminosit

    ALMA Confirmation of an Obscured Hyperluminous Radio-Loud AGN at z=6.853z=6.853 Associated with a Dusty Starburst in the 1.5 deg2^2 COSMOS Field

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    We present band 6 ALMA observations of a heavily-obscured radio-loud (L1.4 GHz=1025.4L_{1.4\ \mathrm{GHz}}=10^{25.4} W Hz1^{-1}) AGN candidate at zphot=6.83±0.06z_\mathrm{phot}=6.83\pm0.06 found in the 1.5 deg2^2 COSMOS field. The ALMA data reveal detections of exceptionally strong [CII]158μ\mum (z[CII]=6.8532z_\mathrm{[CII]}=6.8532) and underlying dust continuum emission from this object (COS-87259), where the [CII] line luminosity, line width, and 158μ\mum continuum luminosity are comparable to that seen from z7z\sim7 sub-mm galaxies and quasar hosts. The 158μ\mum continuum detection suggests a total infrared luminosity of 9×10129\times10^{12} LL_\odot with corresponding very large obscured star formation rate (1300 MM_\odot/yr) and dust mass (2×1092\times10^9 MM_\odot). The strong break seen between the VIRCam and IRAC photometry perhaps suggests that COS-87259 is an extremely massive reionization era galaxy with M1.7×1011M_\ast\approx1.7\times10^{11} MM_\odot. Moreover, the MIPS, PACS, and SPIRE detections imply that this object harbors an AGN that is heavily obscured (τ9.7μm=2.3\tau_{_{\mathrm{9.7\mu m}}}=2.3) with a bolometric luminosity of approximately 5×10135\times10^{13} LL_\odot. Such a very high AGN luminosity suggests this object is powered by an \approx1.6 ×\times 109^9 MM_\odot black hole if accreting near the Eddington limit, and is effectively a highly-obscured version of an extremely UV-luminous (M145027.3M_{1450}\approx-27.3) z7z\sim7 quasar. Notably, these z7z\sim7 quasars are an exceedingly rare population (\sim0.001 deg2^{-2}) while COS-87259 was identified over a relatively small field. Future very wide-area surveys with, e.g., Roman and Euclid have the potential to identify many more extremely red yet UV-bright z7z\gtrsim7 objects similar to COS-87259, providing richer insight into the occurrence of intense obscured star formation and supermassive black hole growth among this population.Comment: 12 pages, 7 figures, 1 table. Updated to accepted version (MNRAS

    Unveiling the Phase Transition of the Universe During the Reionization Epoch with Lyman-alpha

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    The epoch of reionization (6 < z < 10) marks the period in our universe when the first large galaxies grew to fruition, and began to affect the universe around them. Massive stars, and potentially accreting supermassive black holes, filled the universe with ionizing radiation, burning off the haze of neutral gas that had filled the intergalactic medium (IGM) since recombination (z~1000). The evolution of this process constrains key properties of these earliest luminous sources, thus observationally constraining reionization is a key science goal for the next decade. The measurement of Lyman-alpha emission from photometrically-identified galaxies is a highly constraining probe of reionization, as a neutral IGM will resonantly scatter these photons, reducing detectability. While significant work has been done with 8-10m telescopes, these observations require extremely large telescopes (ELTs); the flux limits available from today's 10m class telescopes are sufficient for only the brightest known galaxies (m < 26). Ultra-deep surveys with the Giant Magellan Telescope (GMT) and Thirty Meter Telescope (TMT) will be capable of detecting Lyman-alpha emission from galaxies 2-3 magnitudes fainter than today's deepest surveys. Wide-field fiber spectroscopy on the GMT combined with narrow-field AO-assisted slit spectroscopy on the TMT will be able to probe the expected size of ionized bubbles throughout the epoch of reionization, following up degree scale deep imaging surveys with the Wide Field Infrared Space Telescope. These data will provide the first resolved Lyman-alpha-based maps of the ionized intergalactic medium throughout the epoch of reionization, constraining models of both the temporal and spatial evolution of this phase change.Comment: White paper submitted to the Astro2020 Decadal Review of the National Academy of Science
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