Jerome J. Fang
University of California, Santa Cruz
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Featured researches published by Jerome J. Fang.
The Astrophysical Journal | 2013
Guillermo Barro; S. M. Faber; P. G. Pérez-González; David C. Koo; Christina C. Williams; Dale D. Kocevski; Jonathan R. Trump; Mark Mozena; Elizabeth J. McGrath; Arjen van der Wel; Stijn Wuyts; Eric F. Bell; Darren J. Croton; Daniel Ceverino; Avishai Dekel; M. L. N. Ashby; Edmond Cheung; Henry C. Ferguson; A. Fontana; Jerome J. Fang; Mauro Giavalisco; Norman A. Grogin; Yicheng Guo; Nimish P. Hathi; Philip F. Hopkins; Kuang-Han Huang; Anton M. Koekemoer; J. Kartaltepe; Kyoung-Soo Lee; Jeffrey A. Newman
We combine high-resolution Hubble Space Telescope/WFC3 images with multi-wavelength photometry to track the evolution of structure and activity of massive (M > 1010 M ?) galaxies at redshifts z = 1.4-3 in two fields of the Cosmic Assembly Near-infrared Deep Extragalactic Legacy Survey. We detect compact, star-forming galaxies (cSFGs) whose number densities, masses, sizes, and star formation rates (SFRs) qualify them as likely progenitors of compact, quiescent, massive galaxies (cQGs) at z = 1.5-3. At z 2, cSFGs present SFR = 100-200 M ? yr?1, yet their specific star formation rates (sSFR ~ 10?9?yr?1) are typically half that of other massive SFGs at the same epoch, and host X-ray luminous active galactic nuclei (AGNs) 30?times (~30%) more frequently. These properties suggest that cSFGs are formed by gas-rich processes (mergers or disk-instabilities) that induce a compact starburst and feed an AGN, which, in turn, quench the star formation on dynamical timescales (few 108?yr). The cSFGs are continuously being formed at z = 2-3 and fade to cQGs down to z ~ 1.5. After this epoch, cSFGs are rare, thereby truncating the formation of new cQGs. Meanwhile, down to z = 1, existing cQGs continue to enlarge to match local QGs in size, while less-gas-rich mergers and other secular mechanisms shepherd (larger) SFGs as later arrivals to the red sequence. In summary, we propose two evolutionary tracks of QG formation: an early (z 2), formation path of rapidly quenched cSFGs fading into cQGs that later enlarge within the quiescent phase, and a late-arrival (z 2) path in which larger SFGs form extended QGs without passing through a compact state.
The Astrophysical Journal | 2013
Jerome J. Fang; S. M. Faber; David C. Koo; Avishai Dekel
We study the correlation between galaxy structure and the quenching of star formation using a sample of Sloan Digital Sky Survey central galaxies with stellar masses 9.75 < log M */M ? < 11.25 and redshifts z < 0.075. Galaxy Evolution Explorer UV data are used to cleanly divide the sample into star-forming and quenched galaxies and to identify galaxies in transition (the green valley). Despite a stark difference in visual appearance between blue and red galaxies, their average radial stellar mass density profiles are remarkably similar (especially in the outer regions) at fixed mass. The inner stellar mass surface density within a radius of 1?kpc, ?1, is used to quantify the growth of the bulge as galaxies evolve. When galaxies are divided into narrow mass bins, their distribution in?the color-?1 plane at fixed mass forms plausible evolutionary tracks. ?1 seems to grow as galaxies evolve through the blue cloud, and once it crosses a threshold value, galaxies are seen to quench at fixed ?1. The ?1 threshold for quenching grows with stellar mass, . However, the existence of some star-forming galaxies above the threshold ?1 implies that a dense bulge is necessary but not sufficient to quench a galaxy fully. This would be consistent with a two-step quenching process in which gas within a galaxy is removed or stabilized against star formation by bulge-driven processes (such as a starburst, active galactic nucleus feedback, or morphological quenching), whereas external gas accretion is suppressed by separate halo-driven processes (such as halo gas shock heating). Quenching thus depends on an interplay between the inner structure of a galaxy and its surrounding dark matter halo, and lack of perfect synchrony between the two could produce the observed scatter in color versus ?1.
The Astrophysical Journal | 2015
Yicheng Guo; Henry C. Ferguson; Eric F. Bell; David C. Koo; Christopher J. Conselice; Mauro Giavalisco; Susan A. Kassin; Yu Lu; Ray A. Lucas; Nir Mandelker; Daniel M. McIntosh; Joel R. Primack; Swara Ravindranath; Guillermo Barro; Daniel Ceverino; Avishai Dekel; Sandra M. Faber; Jerome J. Fang; Anton M. Koekemoer; Kai G. Noeske; Marc Rafelski; Amber N. Straughn
Although giant clumps of stars are crucial to galaxy formation and evolution, the most basic demographics of clumps are still uncertain, mainly because the definition of clumps has not been thoroughly discussed. In this paper, we study the basic demographics of clumps in star-forming galaxies (SFGs) at 0.5 0.5. The redshift evolution of Fclumpy changes with the stellar mass (M*) of the galaxies. Low-mass (log(M*/Msun)<9.8) galaxies keep an almost constant Fclumpy of about 60% from z~3.0 to z~0.5. Intermediate-mass and massive galaxies drop their Fclumpy from 55% at z~3.0 to 40% and 15%, respectively, at z~0.5. We find that (1) the trend of disk stabilization predicted by violent disk instability matches the Fclumpy trend of massive galaxies; (2) minor mergers are a viable explanation of the Fclumpy trend of intermediate-mass galaxies at z<1.5, given a realistic observability timescale; and (3) major mergers are unlikely responsible for the Fclumpy trend in all masses at z<1.5. The clump contribution to the rest-frame UV light of SFGs shows a broad peak around galaxies with log(M*/Msun)~10.5 at all redshifts, possibly linked to the molecular gas fraction of the galaxies. (Abridged)
The Astrophysical Journal | 2014
Guillermo Barro; Jonathan R. Trump; David C. Koo; Avishai Dekel; Susan A. Kassin; Dale D. Kocevski; Sandra M. Faber; Arjen van der Wel; Yicheng Guo; P. G. Pérez-González; Elisa Toloba; Jerome J. Fang; Camilla Pacifici; Raymond C. Simons; Randy Campbell; Daniel Ceverino; Steven L. Finkelstein; Bob Goodrich; Marc Kassis; Anton M. Koekemoer; Nicholas P. Konidaris; Rachael Livermore; James Edward Lyke; Bahram Mobasher; Hooshang Nayyeri; Michael Peth; Joel R. Primack; Luca Rizzi; Rachel S. Somerville; Gregory D. Wirth
We present Keck-I MOSFIRE near-infrared spectroscopy for a sample of 13 compact star-forming galaxies (SFGs) at redshift 2 ≤ z ≤ 2.5 with star formation rates of SFR ~ 100 M_☉ yr^(–1) and masses of log(M/M_☉) ~10.8. Their high integrated gas velocity dispersions of σ_(int_ =230^(+40)_(-30) km s^(–1), as measured from emission lines of Hα and [O III], and the resultant M_* -σ_(int) relation and M_*-M_(dyn) all match well to those of compact quiescent galaxies at z ~ 2, as measured from stellar absorption lines. Since log(M*/M_(dyn)) =–0.06 ± 0.2 dex, these compact SFGs appear to be dynamically relaxed and evolved, i.e., depleted in gas and dark matter (<13^(+17)_(-13)%), and present larger σ_(int) than their non-compact SFG counterparts at the same epoch. Without infusion of external gas, depletion timescales are short, less than ~300 Myr. This discovery adds another link to our new dynamical chain of evidence that compact SFGs at z ≳ 2 are already losing gas to become the immediate progenitors of compact quiescent galaxies by z ~ 2.
The Astrophysical Journal | 2014
Hassen M. Yesuf; S. M. Faber; Jonathan R. Trump; David C. Koo; Jerome J. Fang; F. S. Liu; Vivienne Wild; Christopher C. Hayward
Post-starbursts are galaxies in transition from the blue cloud to the red sequence. Although they are rare today, integrated over time they may be an important pathway to the red sequence. This work uses SDSS, GALEX, and WISE observations to identify the evolutionary sequence from starbursts to fully quenched post-starbursts in the narrow mass range logM(M⊙) = 10.3 − 10.7, and identifies “transiting” post-starbursts which are intermediate between these two populations. In this mass range, ∼ 0.3% of galaxies are starbursts, ∼ 0.1% are quenched post-starbursts, and ∼ 0.5% are the transiting types in between. The transiting post-starbursts have stellar properties that are predicted for fast-quenching starbursts and morphological characteristics that are already typical of early-type galaxies. The AGN fraction, as estimated from optical line ratios, of these post-starbursts is about 3 times higher (& 36 ± 8%) than that of normal star-forming galaxies of the same mass, but there is a significant delay between the starburst phase and the peak of nuclear optical AGN activity (median age difference of & 200±100Myr), in agreement with previous studies. The time delay is inferred by comparing the broad-band near NUV-to-optical photometry with stellar population synthesis models. We also find that starbursts and post-starbursts are significantly more dust-obscured than normal star-forming galaxies in the same mass range. About 20% of the starbursts and 15% of the transiting post-starbursts can be classified as the “Dust-Obscured Galaxies” (DOGs), with near-UV to mid-IR flux ratio of & 900, while only 0.8% of normal galaxies are DOGs. The time delay between the starburst phase and AGN activity suggests that AGN do not play a primary role in the original quenching of starbursts but may be responsible for quenching later low-level star formation by removing gas and dust during the post-starburst phase. Subject headings: galaxies: active, galaxies: evolution, galaxies: formation, galaxies: starburst, galaxies: stellar content, galaxies: structure
Monthly Notices of the Royal Astronomical Society | 2015
Edmond Cheung; Jonathan R. Trump; E. Athanassoula; Steven P. Bamford; Eric F. Bell; Albert Bosma; Carolin N. Cardamone; Kevin R. V. Casteels; S. M. Faber; Jerome J. Fang; L. Fortson; Dale D. Kocevski; David C. Koo; Seppo Laine; Chris Lintott; Karen L. Masters; Thomas Melvin; Robert C. Nichol; Kevin Schawinski; Brooke Simmons; Rebecca J. Smethurst; Kyle W. Willett
We present a new study investigating whether active galactic nuclei (AGN) beyond the local universe are preferentially fed via large-scale bars. Our investigation combines data from Chandra and Galaxy Zoo: Hubble (GZH) in the AEGIS (All-wavelength Extended Groth strip International Survey), COSMOS (Cosmological Evolution Survey), and (Great Observatories Origins Deep Survey-South) GOODS-S surveys to create samples of face-on, disc galaxies at 0.2 1, our findings suggest that large-scale bars have likely never directly been a dominant fuelling mechanism for supermassive black hole growth.
arXiv: Astrophysics of Galaxies | 2015
Guillermo Barro; S. M. Faber; David C. Koo; Avishai Dekel; Jerome J. Fang; Jonathan R. Trump; P. G. Pérez-González; Camilla Pacifici; Joel R. Primack; Rachel S. Somerville; Haojing Yan; Yicheng Guo; F. Liu; Daniel Ceverino; Dale D. Kocevski; E. McGrath
We study the evolution of the scaling relations that compare the effective density (Sigma(e), r 9.6 -9.3M(circle dot) kpc(-2), allowing the most efficient identification of compact SFGs and quiescent galaxies at every redshift.
The Astrophysical Journal | 2013
Jonathan R. Trump; Alexander D. Hsu; Jerome J. Fang; S. M. Faber; David C. Koo; Dale D. Kocevski
We present the first quantified, statistical map of broad-line active galactic nucleus (AGN) frequency with host galaxy color and stellar mass in nearby (0.01 < z < 0.11) galaxies. Aperture photometry and z-band concentration measurements from the Sloan Digital Sky Survey are used to disentangle AGN and galaxy emission, resulting in estimates of uncontaminated galaxy rest-frame color, luminosity, and stellar mass. Broad-line AGNs are distributed throughout the blue cloud and green valley at a given stellar mass, and are much rarer in quiescent (red sequence) galaxies. This is in contrast to the published host galaxy properties of weaker narrow-line AGNs, indicating that broad-line AGNs occur during a different phase in galaxy evolution. More luminous broad-line AGNs have bluer host galaxies, even at fixed mass, suggesting that the same processes that fuel nuclear activity also efficiently form stars. The data favor processes that simultaneously fuel both star formation activity and rapid supermassive black hole accretion. If AGNs cause feedback on their host galaxies in the nearby universe, the evidence of galaxy-wide quenching must be delayed until after the broad-line AGN phase.
The Astrophysical Journal | 2016
Guillermo Barro; Sandra M. Faber; Avishai Dekel; Camilla Pacifici; P. G. Pérez-González; Elisa Toloba; David C. Koo; Jonathan R. Trump; Shigeki Inoue; Yicheng Guo; F. S. Liu; Joel R. Primack; Anton M. Koekemoer; Gabriel B. Brammer; A. Cava; N. Cardiel; Daniel Ceverino; C. Eliche; Jerome J. Fang; Steven L. Finkelstein; Dale D. Kocevski; Rachael Livermore; Elizabeth J. McGrath
We present Keck-I MOSFIRE spectroscopy in the Y and H bands of GDN-8231, a massive, compact, star-forming galaxy (SFG) at a redshift
The Astrophysical Journal | 2017
Guillermo Barro; S. M. Faber; David C. Koo; Avishai Dekel; Jerome J. Fang; Jonathan R. Trump; P. G. Pérez-González; Camilla Pacifici; Joel R. Primack; Rachel S. Somerville; Haojing Yan; Yicheng Guo; F. S. Liu; Daniel Ceverino; Dale D. Kocevski; Elizabeth J. McGrath
z\sim1.7