87 research outputs found

    Local star-forming galaxies build up central mass concentration most actively near M∗=1010M⊙M_{*}=10^{10}M_{\odot}

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    To understand in what mass regime star-forming galaxies (SFGs) build up central mass concentration most actively, we present a study on the luminosity-weighted stellar age radial gradient (∇age\nabla_{\rm age}) distribution of ∼3600\sim3600 low-redshift SFGs using the MaNGA Pipe3D data available in the SDSS DR17. The mean age gradient is negative, with ∇age=−0.14\nabla_{\rm age}=-0.14log Gyr/ReR_{\rm e}, consistent with the inside-out disk formation scenario. Specifically, SFGs with positive ∇age\nabla_{\rm age} consist of ∼28%\sim 28\% at log(M∗/M⊙)<9.5(M_{*}/M_{\odot})<9.5, while this fraction rises up to its peak (∼40%\sim 40\%) near log(M∗/M⊙)=10(M_{*}/M_{\odot})=10 and then decreases to ∼15%\sim 15\% at log(M∗/M⊙)=11(M_{*}/M_{\odot})=11. At fixed M∗M_{*}, SFGs with positive ∇age\nabla_{\rm age} typically have more compact sizes and more centrally concentrated star formation than their counterparts, indicative of recent central mass build-up events. These results suggest that the build-up of central stellar mass concentration in local SFGs is mostly active near M∗=1010M⊙M_{*}=10^{10}M_{\odot}. Our findings provide new insights on the origin of morphological differences between low-mass and high-mass SFGs.Comment: 10 pages, 8 figures, accepted by Ap

    Nature vs. Nurture: Revisiting the environmental impact on star formation activities of galaxies

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    We present a systematic study of the environmental impact on star formation activities of galaxies using a mass-complete sample of ∼\sim170k galaxies at z<4z<4 from the latest COSMOS2020 catalog. At z<1z<1, we find that the mean star-formation rate (SFR) of all galaxies decreases with increasing density of the environment. However when we consider only star-forming galaxies, the mean SFR becomes independent of the environment at z2z2 we observe a clear positive correlation between the SFR and density of the environment for all the galaxies. On the other hand, stellar mass of the galaxies increases significantly with the environments at all redshifts except for star-forming galaxies at z<1z<1. The fraction of quiescent galaxies increases with increasing density of environment at z<2z<2, and the ``morphology-density'' relation is confirmed to be present up to z∼1z\sim1. We also find that environmental quenching is negligible at z>1z>1, whereas mass quenching is the dominant quenching mechanism for massive galaxies at all redshifts. Based on these results, we argue that stellar mass regulated physical processes might be the major driving force for star formation activities of galaxies. At low redshift (z<1z<1) massive galaxies are quenched primarily due to their high mass, resulting in a normal ``SFR-density'' relation. At high redshift (z>2z>2) most of the galaxies are star-forming ones tightly following the star-forming main sequence, and the difference in their stellar mass at different environments naturally leads to a reversal of ``SFR-density'' relation.Comment: 16 pages, 7 figures, accepted for publication in Ap

    Deep CFHT Y-band imaging of VVDS-F22 field: I. data products and photometric redshifts

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    We present our deep YY-band imaging data of a two square degree field within the F22 region of the VIMOS VLT Deep Survey. The observations were conducted using the WIRCam instrument mounted at the Canada--France--Hawaii Telescope (CFHT). The total on-sky time was 9 hours, distributed uniformly over 18 tiles. The scientific goals of the project are to select faint quasar candidates at redshift z>2.2z>2.2, and constrain the photometric redshifts for quasars and galaxies. In this paper, we present the observation and the image reduction, as well as the photometric redshifts that we derived by combining our YY-band data with the CFHTLenS u∗g′r′i′z′u^*g'r'i'z' optical data and UKIDSS DXS JHKJHK near-infrared data. With JJ-band image as reference total ∼\sim80,000 galaxies are detected in the final mosaic down to YY-band 5σ5\sigma point source limiting depth of 22.86 mag. Compared with the ∼\sim3500 spectroscopic redshifts, our photometric redshifts for galaxies with z<1.5z<1.5 and i′≲24.0i'\lesssim24.0 mag have a small systematic offset of ∣Δz∣≲0.2|\Delta{z}|\lesssim0.2, 1σ\sigma scatter 0.03<σΔz<0.060.03<\sigma_{\Delta z} < 0.06, and less than 4.0% of catastrophic failures. We also compare to the CFHTLenS photometric redshifts, and find that ours are more reliable at z≳0.6z\gtrsim0.6 because of the inclusion of the near-infrared bands. In particular, including the YY-band data can improve the accuracy at z∼1.0−2.0z\sim 1.0-2.0 because the location of the 4000\AA-break is better constrained. The YY-band images, the multi-band photometry catalog and the photometric redshifts are released at \url{http://astro.pku.edu.cn/astro/data/DYI.html}.Comment: 16 pages, 12 figures, 4 tables. AJ accepted. Updated access to the data: https://zenodo.org/record/140003

    Spectroscopic Confirmation of two Extremely Massive Protoclusters BOSS1244 and BOSS1542 at z=2.24z=2.24

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    We present spectroscopic confirmation of two new massive galaxy protoclusters at z=2.24±0.02z=2.24\pm0.02, BOSS1244 and BOSS1542, traced by groups of Coherently Strong Lyα\alpha Absorption (CoSLA) systems imprinted in the absorption spectra of a number of quasars from the SDSS III and identified as overdensities of narrowband-selected Hα\alpha emitters (HAEs). Using MMT/MMIRS and LBT/LUCI near-infrared (NIR) spectroscopy, we confirm 46 and 36 HAEs in the BOSS1244 and BOSS1542 fields, respectively. BOSS1244 displays a South-West (SW) component at z=2.230±0.002z=2.230\pm0.002 and another North-East (NE) component at z=2.246±0.001z=2.246\pm0.001 with the line-of-sight velocity dispersions of 405±202405\pm202 km s−1^{-1} and 377±99377\pm99 km s−1^{-1}, respectively. Interestingly, we find that the SW region of BOSS1244 contains two substructures in redshift space, likely merging to form a larger system. In contrast, BOSS1542 exhibits an extended filamentary structure with a low velocity dispersion of 247±32247\pm32 km s−1^{-1} at z=2.241±0.001z=2.241\pm0.001, providing a direct confirmation of a large-scale cosmic web in the early Universe. The galaxy overdensities δg\delta_{\rm g} on the scale of 15 cMpc are 22.9±4.922.9\pm4.9, 10.9±2.510.9\pm2.5, and 20.5±3.920.5\pm3.9 for the BOSS1244 SW, BOSS1244 NE, and BOSS1542 filament, respectively. They are the most overdense galaxy protoclusters (δg>20\delta_{\rm g}>20) discovered to date at z>2z>2. These systems are expected to become virialized at z∼0z\sim0 with a total mass of MSW=(1.59±0.20)×1015M_{\rm SW}=(1.59\pm0.20)\times10^{15} M⊙M_{\odot}, MNE=(0.83±0.11)×1015M_{\rm NE} =(0.83\pm0.11)\times10^{15} M⊙M_{\odot} and Mfilament=(1.42±0.18)×1015M_{\rm filament}=(1.42\pm0.18)\times10^{15} M⊙M_{\odot}, respectively. Together with BOSS1441 described in Cai et al. (2017a), these extremely massive overdensities at z=2−3z=2-3 exhibit different morphologies, indicating that they are in different assembly stages in the formation of early galaxy clusters.Comment: 28 pages, 13 figures, 6 tables, accepted for publication in ApJ. The complete Abstract is presented in the manuscrip

    Deep Imaging of the HCG 95 Field.I.Ultra-diffuse Galaxies

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    We present a detection of 89 candidates of ultra-diffuse galaxies (UDGs) in a 4.9 degree2^2 field centered on the Hickson Compact Group 95 (HCG 95) using deep gg- and rr-band images taken with the Chinese Near Object Survey Telescope. This field contains one rich galaxy cluster (Abell 2588 at zz=0.199) and two poor clusters (Pegasus I at zz=0.013 and Pegasus II at zz=0.040). The 89 candidates are likely associated with the two poor clusters, giving about 50 −- 60 true UDGs with a half-light radius re>1.5r_{\rm e} > 1.5 kpc and a central surface brightness μ(g,0)>24.0\mu(g,0) > 24.0 mag arcsec−2^{-2}. Deep zz'-band images are available for 84 of the 89 galaxies from the Dark Energy Camera Legacy Survey (DECaLS), confirming that these galaxies have an extremely low central surface brightness. Moreover, our UDG candidates are spread over a wide range in g−rg-r color, and ∼\sim26% are as blue as normal star-forming galaxies, which is suggestive of young UDGs that are still in formation. Interestingly, we find that one UDG linked with HCG 95 is a gas-rich galaxy with H I mass 1.1×109M⊙1.1 \times 10^{9} M_{\odot} detected by the Very Large Array, and has a stellar mass of M⋆∼1.8×108M_\star \sim 1.8 \times 10^{8} M⊙M_{\odot}. This indicates that UDGs at least partially overlap with the population of nearly dark galaxies found in deep H I surveys. Our results show that the high abundance of blue UDGs in the HCG 95 field is favored by the environment of poor galaxy clusters residing in H I-rich large-scale structures.Comment: Published in Ap

    BayeSED-GALAXIES I. Performance test for simultaneous photometric redshift and stellar population parameter estimation of galaxies in the CSST wide-field multiband imaging survey

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    The forthcoming CSST wide-field multiband imaging survey will produce seven-band photometric spectral energy distributions (SEDs) for billions of galaxies. The effective extraction of astronomical information from these massive datasets of SEDs relies on the techniques of both SED synthesis (or modeling) and analysis (or fitting). We evaluate the performance of the latest version of BayeSED code combined with SED models with increasing complexity for simultaneously determining the photometric redshifts and stellar population parameters of galaxies in this survey. By using an empirical statistics-based mock galaxy sample without SED modeling errors, we show finding that the random observational errors in photometries are more important sources of errors than the parameter degeneracies and Bayesian analysis method and tool. By using a Horizon-AGN hydrodynamical simulation-based mock galaxy sample with SED modeling errors about the star formation histories (SFHs) and dust attenuation laws (DALs), the simple typical assumptions lead to significantly worse parameter estimation with CSST photometries only. The SED models with more flexible (or complicated) forms of SFH/DAL do not necessarily lead to better estimation of redshift and stellar population parameters. We discuss the selection of the best SED model by means of Bayesian model comparison in different surveys. Our results reveal that the Bayesian model comparison with Bayesian evidence may favor SED models with different complexities when using photometries from different surveys. Meanwhile, the SED model with the largest Bayesian evidence tends to give the best performance of parameter estimation, which is more clear for photometries with larger discriminative power.Comment: Accepted for publication in ApJS (49 pages, 23 figures, 5 tables). Comments are welcome! The new version of BayeSED code, documents, and the scripts used for the performance tests presented in this work will be publicly available at https://bitbucket.org/hanyk/bayesed/, https://bayesed.readthedocs.io/, and https://github.com/hanyk/BayeSED-performance-test/, respectivel

    Galaxy formation and evolution since z=1

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    Determination of the star formation rate can be done using mid-IR photometry or Balmer line luminosity after a proper correction for extinction effects. Both methods show convergent results while those based on UV or on [OII]3727 luminosities underestimate the SFR by factors ranging from 5 to 40 for starbursts and for luminous IR galaxies, respectively. Most of the evolution of the cosmic star formation density is related to the evolution of luminous compact galaxies and to luminous IR galaxies. Because they were metal deficient and were forming stars at very high rates (40 to 100 solar mass per year), it is probable that these (massive) galaxies were actively forming the bulk of their stellar/metal content at z < 1.Comment: 6 pages, 3 figures. To appear in the proceedings of the Venice conference "Multiwavelength Mapping of Galaxy Formation and Evolution", October 13-16, 200
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