30 research outputs found

    Hubble Space Telescope Observations of Tadpole Galaxies Kiso 3867, SBS0, SBS1, and UM461

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    Tadpole galaxies are metal-poor dwarfs with typically one dominant star-forming region, giving them a head-tail structure when inclined. A metallicity drop in the head suggests that gas accretion with even lower metallicity stimulated the star formation. Here we present multiband HST WFC3 and ACS images of four nearby (<25 Mpc) tadpoles, SBS0, SBS1, Kiso 3867, and UM461, selected for their clear metallicity drops shown in previous spectroscopic studies. Properties of the star complexes and compact clusters are measured. Each galaxy contains from 3 to 10 young stellar complexes with 10^3-10^5 Msun of stars ~3-10 Myr old. Between the complexes, the disk has a typical age of ~3 Gyr. Numerous star clusters cover the galaxies, both inside and outside the complexes. The combined cluster mass function, made by normalizing the masses and counts before stacking, is a power law with a slope of -1.12+-0.14 on a log-log plot and the combined distribution function of cluster lifetime decays with age as t^{-0.65+-0.24}. A comparison between the summed theoretical Lyman continuum (LyC) emission from all the clusters, given their masses and ages, is comparable to or exceeds the LyC needed to excite the observed Halpha in some galaxies, suggesting LyC absorption by dust or undetected gas in the halo, or perhaps galaxy escape.Comment: 20 pages, 16 figures, accepted by Ap

    Lyman Continuum Emission from AGN at 2.3\lesssimz\lesssim3.7 in the UVCANDELS Fields

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    We present the results of our search for Lyman continuum (LyC) emitting AGN at redshifts 2.3\lesssimz\lesssim4.9 from HST WFC3 F275W observations in the UVCANDELS fields. We also include LyC emission from AGN using HST WFC3 F225W, F275W, and F336W found in the ERS and HDUV data. We performed exhaustive queries of the Vizier database to locate AGN with high quality spectroscopic redshifts. In total, we found 51 AGN that met our criteria within the UVCANDELS and ERS footprints. Of these 51, we find 12 AGN had \geq4σ\sigma detected LyC flux in the WFC3/UVIS images. Using space- and ground-based data from X-ray to radio, we fit the multi-wavelength photometric data of each AGN to a CIGALE SED and correlate various SED parameters to the LyC flux. KS-tests of the SED parameter distributions for the LyC-detected and non-detected AGN showed they are likely not distinct samples. However, we find that X-ray luminosity, star-formation onset age, and disk luminosity show strong correlations relative to their emitted LyC flux. We also find strong correlation of the LyC flux to several dust parameters, i.e., polar and toroidal dust emission, 6 μm\mu m luminosity, and anti-correlation with metallicity and AFUVA_{FUV}. We simulate the LyC escape fraction (fescf_{esc}) using the CIGALE and IGM transmission models for the LyC-detected AGN and find an average fescf_{esc}\simeq18%, weighted by uncertainties. We stack the LyC flux of subsamples of AGN according to the wavelength continuum region in which they are detected and find no significant distinctions in their LyC emission, although our submm detectedsub-mm\ detected F336W sample shows the brightest stacked LyC flux. These findings indicate that LyC-production and -escape in AGN is more complicated than the simple assumption of thermal emission and a 100% escape fraction. Further testing of AGN models with larger samples than presented here is needed.Comment: 21 pages, 6 figures, 3 tables. Accepted for publication in The Astrophysical Journa

    The mass-metallicity relation at z~1-2 and its dependence on star formation rate

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    We present a new measurement of the gas-phase mass-metallicity relation (MZR), and its dependence on star formation rates (SFRs) at 1.3 < z < 2.3. Our sample comprises 1056 galaxies with a mean redshift of z = 1.9, identified from the Hubble Space Telescope Wide Field Camera 3 (WFC3) grism spectroscopy in the Cosmic Assembly Near-Infrared Deep Extragalactic Survey (CANDELS) and the WFC3 Infrared Spectroscopic Parallel Survey (WISP). This sample is four times larger than previous metallicity surveys at z ~ 2, and reaches an order of magnitude lower in stellar mass (10^8 M_sun). Using stacked spectra, we find that the MZR evolves by 0.3 dex relative to z ~ 0.1. Additionally, we identify a subset of 49 galaxies with high signal-to-noise (SNR) spectra and redshifts between 1.3 < z < 1.5, where H-alpha emission is observed along with [OIII] and [OII]. With accurate measurements of SFR in these objects, we confirm the existence of a mass-metallicity-SFR (M-Z-SFR) relation at high redshifts. These galaxies show systematic differences from the local M-Z-SFR relation, which vary depending on the adopted measurement of the local relation. However, it remains difficult to ascertain whether these differences could be due to redshift evolution, as the local M-Z-SFR relation is poorly constrained at the masses and SFRs of our sample. Lastly, we reproduced our sample selection in the IllustrisTNG hydrodynamical simulation, demonstrating that our line flux limit lowers the normalization of the simulated MZR by 0.2 dex. We show that the M-Z-SFR relation in IllustrisTNG has an SFR dependence that is too steep by a factor of around three.Comment: Accepted for publication in ApJ; 41 pages, 20 figure

    First Sample of Hα\alpha+[O III] λ\lambda5007 Line Emitters at z>6z > 6 through JWST/NIRCam Slitless Spectroscopy: Physical Properties and Line Luminosity Functions

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    We present a sample of four emission-line galaxies at z=6.116.35z=6.11-6.35 that were serendipitously discovered using the commissioning data for the JWST/NIRCam wide-field slitless spectroscopy (WFSS) mode. One of them (at z=6.11z=6.11) has been reported previously while the others are new discoveries. These sources are selected by the secure detections of both [O III] λ\lambda5007 and Hα\alpha lines with other fainter lines tentatively detected in some cases (e.g., [O II] λ\lambda3727, [O III] λ\lambda4959 and [N II] λ\lambda6583). In the [O III]/Hβ\beta - [N II]/Hα\alpha Baldwin-Phillips-Terlevich diagram, these galaxies occupy the same parameter space as that of z2z\sim2 star-forming galaxies, indicating that they have been enriched rapidly to sub-solar metallicities (\sim0.6 ZZ_{\odot}), similar to galaxies with comparable stellar masses at much lower redshifts. The detection of strong Hα\alpha lines suggests a higher ionizing photon production efficiency within galaxies in the early Universe. We find brightening of the [O III] λ\lambda5007 line luminosity function (LF) from z=3z=3 to 6, and no or weak redshift evolution of the Hα\alpha line LF from z=2z=2 to 6. Both LFs are under-predicted at z6z\sim6 by a factor of \sim10 in certain cosmological simulations. This further indicates a global Lyα\alpha photon escape fraction of 5-7% at z6z\sim6, much lower than previous estimates through the comparison of the UV-derived star-formation rate density and Lyα\alpha luminosity density. Our sample recovers 8857+16488^{+164}_{-57}% of z=6.06.6z=6.0-6.6 galaxies in the survey volume with stellar masses greater than 5×1085\times10^8 MM_{\odot}, suggesting the ubiquity of strong Hα\alpha and [O III] line emitters in the Epoch of Reionization, which will be further uncovered in the era of JWST.Comment: 25 pages, 11 figures, submitted to Ap

    CEERS: 7.7 μ{\mu}m PAH Star Formation Rate Calibration with JWST MIRI

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    We test the relationship between UV-derived star formation rates (SFRs) and the 7.7 μ{\mu}m polycyclic aromatic hydrocarbon (PAH) luminosities from the integrated emission of galaxies at z ~ 0 - 2. We utilize multi-band photometry covering 0.2 - 160 μ{\mu}m from HST, CFHT, JWST, Spitzer, and Herschel for galaxies in the Cosmic Evolution Early Release Science (CEERS) Survey. We perform spectral energy distribution (SED) modeling of these data to measure dust-corrected far-UV (FUV) luminosities, LFUVL_{FUV}, and UV-derived SFRs. We then fit SED models to the JWST/MIRI 7.7 - 21 μ{\mu}m CEERS data to derive rest-frame 7.7 μ{\mu}m luminosities, L770L_{770}, using the average flux density in the rest-frame MIRI F770W bandpass. We observe a correlation between L770L_{770} and LFUVL_{FUV}, where log L770L_{770} is proportional to (1.27+/-0.04) log LFUVL_{FUV}. L770L_{770} diverges from this relation for galaxies at lower metallicities, lower dust obscuration, and for galaxies dominated by evolved stellar populations. We derive a "single-wavelength" SFR calibration for L770L_{770} which has a scatter from model estimated SFRs (σΔSFR{{\sigma}_{{\Delta}SFR}}) of 0.24 dex. We derive a "multi-wavelength" calibration for the linear combination of the observed FUV luminosity (uncorrected for dust) and the rest-frame 7.7 μ{\mu}m luminosity, which has a scatter of σΔSFR{{\sigma}_{{\Delta}SFR}} = 0.21 dex. The relatively small decrease in σ{\sigma} suggests this is near the systematic accuracy of the total SFRs using either calibration. These results demonstrate that the rest-frame 7.7 μ{\mu}m emission constrained by JWST/MIRI is a tracer of the SFR for distant galaxies to this accuracy, provided the galaxies are dominated by star-formation with moderate-to-high levels of attenuation and metallicity.Comment: 20 pages, 11 figures, 2 tables, submitted to Ap

    CEERS: Spatially Resolved UV and mid-IR Star Formation in Galaxies at 0.2 < z < 2.5: The Picture from the Hubble and James Webb Space Telescopes

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    We present the mid-IR (MIR) morphologies for 64 star-forming galaxies at 0.210^{9}~M_\odot} using JWST MIRI observations from the Cosmic Evolution Early Release Science survey (CEERS). The MIRI bands span the MIR (7.7--21~μ\mum), enabling us to measure the effective radii (ReffR_{\rm{eff}}) and S\'{e}rsic indexes of these SFGs at rest-frame 6.2 and 7.7 μ\mum, which contains strong emission from Polycyclic aromatic hydrocarbon (PAH) features, a well-established tracer of star formation in galaxies. We define a ``PAH-band'' as the MIRI bandpass that contains these features at the redshift of the galaxy. We then compare the galaxy morphologies in the PAH-bands to those in rest-frame Near-UV (NUV) using HST ACS/F435W or ACS/F606W and optical/near-IR using HST WFC3/F160W imaging from UVCANDELS and CANDELS, where the NUV-band and F160W trace the profile of (unobscured) massive stars and the stellar continuum, respectively. The ReffR_{\rm{eff}} of galaxies in the PAH-band are slightly smaller (\sim10\%) than those in F160W for galaxies with M109.5 M\rm{M_*\gtrsim10^{9.5}~M_\odot} at z1.2z\leq1.2, but the PAH-band and F160W have a similar fractions of light within 1 kpc. In contrast, the ReffR_{\rm{eff}} of galaxies in the NUV-band are larger, with lower fractions of light within 1 kpc compared to F160W for galaxies at z1.2z\leq1.2. Using the MIRI data to estimate the SFRIR\rm{SFR_{\rm{IR}}} surface density, we find the correlation between the SFRIR\rm{SFR_{\rm{IR}}} surface density and stellar mass has a steeper slope than that of the SFRUV\rm{SFR_{\rm{UV}}} surface density and stellar mass, suggesting more massive galaxies having increasing amounts of obscured fraction of star formation in their inner regions. This paper demonstrates how the high-angular resolution data from JWST/MIRI can reveal new information about the morphology of obscured-star formation.Comment: 28 pages, 11 figures, Accepted by Ap

    The Ultraviolet Luminosity Function at 0.6 < z < 1 from UVCANDELS

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    © 2024. The Author(s). Published by the American Astronomical Society. This work is licensed under the terms of under the terms of the Creative Commons Attribution 4.0 licence: https://creativecommons.org/licenses/by/4.0/UVCANDELS is a Hubble Space Telescope Cycle-26 Treasury Program awarded 164 orbits of primary ultraviolet (UV) F275W imaging and coordinated parallel optical F435W imaging in four CANDELS fields—GOODS-N, GOODS-S, EGS, and COSMOS—covering a total area of ∼426 arcmin2. This is ∼2.7 times larger than the area covered by previous deep-field space UV data combined, reaching a depth of about 27 and 28 ABmag (5σ in 0.”2 apertures) for F275W and F435W, respectively. Along with new photometric catalogs, we present an analysis of the rest-frame UV luminosity function (LF), relying on our UV-optimized aperture photometry method, yielding a factor of 1.5 increase over H-isophot aperture photometry in the signal-to-noise ratios of galaxies in our F275W imaging. Using well-tested photometric redshift measurements, we identify 5810 galaxies at redshifts 0.6 < z < 1, down to an absolute magnitude of M UV = −14.2. In order to minimize the effect of uncertainties in estimating the completeness function, especially at the faint end, we restrict our analysis to sources above 30% completeness, which provides a final sample of 4726 galaxies at −21.5 < M UV < −15.5. We performed a maximum likelihood estimate to derive the best-fit parameters of the UV LF. We report a best-fit faint-end slope of α=−1.359−0.041+0.041 at z ∼ 0.8. Creating subsamples at z ∼ 0.7 and z ∼ 0.9, we observe a possible evolution of α with redshift. The unobscured UV luminosity density at M UV < −10 is derived as ρUV=1.339−0.030+0.027(×1026ergs−1Hz−1Mpc−3) using our best-fit LF parameters. The new F275W and F435 photometric catalogs from UVCANDELS have been made publicly available on the Barbara A. Mikulski Archive for Space Telescopes.Peer reviewe

    The Lyman Continuum Escape Fraction of Star-forming Galaxies at 2.4z3.72.4\lesssim z\lesssim3.7 from UVCANDELS

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    The UltraViolet Imaging of the Cosmic Assembly Near-infrared Deep Extragalactic Legacy Survey Fields (UVCANDELS) survey is a Hubble Space Telescope (HST) Cycle-26 Treasury Program, allocated in total 164 orbits of primary Wide-Field Camera 3 Ultraviolet and Visible light F275W imaging with coordinated parallel Advanced Camera for Surveys F435W imaging, on four of the five premier extragalactic survey fields: GOODS-N, GOODS-S, EGS, and COSMOS. We introduce this survey by presenting a thorough search for galaxies at z2.4z\gtrsim2.4 that leak significant Lyman continuum (LyC) radiation, as well as a stringent constraint on the LyC escape fraction (fescf_{\rm esc}) from stacking the UV images of a population of star-forming galaxies with secure redshifts. Our extensive search for LyC emission and stacking analysis benefit from the catalogs of high-quality spectroscopic redshifts compiled from archival ground-based data and HST slitless spectroscopy, carefully vetted by dedicated visual inspection efforts. We report a sample of five galaxies as individual LyC leaker candidates, showing fescrel60%f_{\rm esc}^{\rm rel}\gtrsim60\% estimated using detailed Monte Carlo analysis of intergalactic medium attenuation. We develop a robust stacking method to apply to five samples of in total 85 non-detection galaxies in the redshift range of z[2.4,3.7]z\in[2.4,3.7]. Most stacks give tight 2-σ\sigma upper limits below fescrel<6%f_{\rm esc}^{\rm rel}<6\%. A stack for a subset of 32 emission-line galaxies shows tentative LyC leakage detected at 2.9-σ\sigma, indicating fescrel=5.7%f_{\rm esc}^{\rm rel}=5.7\% at z2.65z\sim2.65, supporting the key role of such galaxies in contributing to the cosmic reionization and maintaining the UV ionization background. These new F275W and F435W imaging mosaics from UVCANDELS have been made publicly available on the Barbara A. Mikulski Archive for Space Telescopes.Comment: 33 pages, 21 figures, and 5 tables. Resubmitted after addressing the referee repor

    The Science Performance of JWST as Characterized in Commissioning

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    This paper characterizes the actual science performance of the James Webb Space Telescope (JWST), as determined from the six month commissioning period. We summarize the performance of the spacecraft, telescope, science instruments, and ground system, with an emphasis on differences from pre-launch expectations. Commissioning has made clear that JWST is fully capable of achieving the discoveries for which it was built. Moreover, almost across the board, the science performance of JWST is better than expected; in most cases, JWST will go deeper faster than expected. The telescope and instrument suite have demonstrated the sensitivity, stability, image quality, and spectral range that are necessary to transform our understanding of the cosmos through observations spanning from near-earth asteroids to the most distant galaxies.Comment: 5th version as accepted to PASP; 31 pages, 18 figures; https://iopscience.iop.org/article/10.1088/1538-3873/acb29
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