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Monthly Notices of the Royal Astronomical Society | 2013

Massive starburst galaxies in a z = 2.16 proto-cluster unveiled by panoramic Hα mapping

Yusei Koyama; Tadayuki Kodama; Ken-ichi Tadaki; Masao Hayashi; M. Tanaka; Ian Smail; Ichi Tanaka; J. Kurk

We present a panoramic narrow-band study of Hα emitters in the field of the z = 2.16 proto-cluster around PKS 1138−262 using MOIRCS on the Subaru Telescope. We find 83 Hα emitters down to a star formation rate of SFR (Hα) ∼ 10 M⊙ yr−1 across a ∼ 7 × 7 arcmin2 region centred on the radio galaxy, and identify ∼10-Mpc scale filaments of emitters running across this region. By examining the properties of Hα emitters within the large-scale structure, we find that galaxies in the higher density environments at z = 2.16 tend to have redder colours and higher stellar masses compared to galaxies in more underdense regions. We also find a population of Hα emitters with red colours [(J − Ks) ≳ 1], which are much more frequent in the denser environments and which have apparently very high stellar masses with M* ≳ 1011 M⊙, implying that these cluster galaxies have already formed a large part of their stellar mass before z ∼ 2. Spitzer Space Telescope 24-μm data suggest that many of these red Hα emitters are bright, dusty starbursts (rather than quiescent sources). We also find that the proto-cluster galaxies follow the same correlation between SFR and M* (the ‘main sequence’) of z ∼ 2 field star-forming galaxies, but with an excess of massive galaxies. These very massive star-forming galaxies are not seen in our similar, previous study of z ∼ 1 clusters, suggesting that their star formation activity has been shut off at 1 ≲ z ≲ 2. We infer that the massive red (but active) galaxies in this rich proto-cluster are likely to be the products of environmental effects, and they represent the accelerated galaxy formation and evolution in a biased high-density region in the early Universe.


Nature | 2017

Strongly baryon-dominated disk galaxies at the peak of galaxy formation ten billion years ago

R. Genzel; N. M. Förster Schreiber; Hannah Übler; P. Lang; Thorsten Naab; Ralf Bender; L. J. Tacconi; Emily Wisnioski; Stijn Wuyts; T. Alexander; A. Beifiori; Sirio Belli; Gabriel B. Brammer; Andreas Burkert; C. M. Carollo; J. Chan; R. Davies; Matteo Fossati; Audrey Galametz; Shy Genel; Ortwin Gerhard; D. Lutz; J. T. Mendel; Ivelina Momcheva; Erica J. Nelson; A. Renzini; R. P. Saglia; A. Sternberg; Sandro Tacchella; Ken-ichi Tadaki

In the cold dark matter cosmology, the baryonic components of galaxies—stars and gas—are thought to be mixed with and embedded in non-baryonic and non-relativistic dark matter, which dominates the total mass of the galaxy and its dark-matter halo. In the local (low-redshift) Universe, the mass of dark matter within a galactic disk increases with disk radius, becoming appreciable and then dominant in the outer, baryonic regions of the disks of star-forming galaxies. This results in rotation velocities of the visible matter within the disk that are constant or increasing with disk radius—a hallmark of the dark-matter model. Comparisons between the dynamical mass, inferred from these velocities in rotational equilibrium, and the sum of the stellar and cold-gas mass at the peak epoch of galaxy formation ten billion years ago, inferred from ancillary data, suggest high baryon fractions in the inner, star-forming regions of the disks. Although this implied baryon fraction may be larger than in the local Universe, the systematic uncertainties (owing to the chosen stellar initial-mass function and the calibration of gas masses) render such comparisons inconclusive in terms of the mass of dark matter. Here we report rotation curves (showing rotation velocity as a function of disk radius) for the outer disks of six massive star-forming galaxies, and find that the rotation velocities are not constant, but decrease with radius. We propose that this trend arises because of a combination of two main factors: first, a large fraction of the massive high-redshift galaxy population was strongly baryon-dominated, with dark matter playing a smaller part than in the local Universe; and second, the large velocity dispersion in high-redshift disks introduces a substantial pressure term that leads to a decrease in rotation velocity with increasing radius. The effect of both factors appears to increase with redshift. Qualitatively, the observations suggest that baryons in the early (high-redshift) Universe efficiently condensed at the centres of dark-matter haloes when gas fractions were high and dark matter was less concentrated.


The Astrophysical Journal | 2012

A STARBURSTING PROTO-CLUSTER IN MAKING ASSOCIATED WITH A RADIO GALAXY AT z = 2.53 DISCOVERED BY Hα IMAGING

Masao Hayashi; Tadayuki Kodama; Ken-ichi Tadaki; Yusei Koyama; Ichi Tanaka

We report a discovery of a proto-cluster in vigorous assembly and hosting strong star-forming activities, associated with a radio galaxy USS 1558-003 at z = 2.53, as traced by wide-field narrow-band H? imaging with MOIRCS on the Subaru Telescope. We find 68 H? emitters with dust-uncorrected star formation rates (SFRs) down to 8.6 M ??yr?1. Their spatial distribution indicates that there are three prominent clumps of H? emitters: one surrounding the radio galaxy, the second located at ~1.5?Mpc away to the southwest, and the third located between the two. These contiguous three systems are very likely to merge together in the near future and may grow to a single more massive cluster at a later time. While most H? emitters reside in the blue cloud on the color-magnitude diagram, some emitters have very red colors with J ? Ks > 1.38(AB). Interestingly, such red H? emitters are located toward the faint end of the red sequence, and they tend to be located in high density clumps. We do not see any statistically significant difference in the distributions of individual SFRs or stellar masses of the H? emitters between the dense clumps and the other regions, suggesting that this is one of the notable sites where the progenitors of massive galaxies in the present-day clusters were in their vigorous formation phase. Finally, we find that H? emission of the radio galaxy is fairly extended spatially over ~45. However, it is not as widespread as its Ly? halo, meaning that the Ly? emission is indeed severely extended by resonant scattering.


The Astrophysical Journal | 2018

PHIBSS: Unified Scaling Relations of Gas Depletion Time and Molecular Gas Fractions

L. J. Tacconi; R. Genzel; A. Saintonge; Francoise Combes; Santiago Garcia-Burillo; R. Neri; Alberto D. Bolatto; T. Contini; N. M. Förster Schreiber; S. J. Lilly; D. Lutz; Stijn Wuyts; Gioacchino Accurso; J. Boissier; F. Boone; N. Bouché; F. Bournaud; Andreas Burkert; Marcella Carollo; Michael C. Cooper; P. Cox; C. Feruglio; J. Freundlich; R. Herrera-Camus; S. Juneau; Magdalena Lippa; Thorsten Naab; A. Renzini; P. Salomé; A. Sternberg

This paper provides an update of our previous scaling relations (Genzel et al.2015) between galaxy integrated molecular gas masses, stellar masses and star formation rates, in the framework of the star formation main-sequence (MS), with the main goal to test for possible systematic effects. For this purpose our new study combines three independent methods of determining molecular gas masses from CO line fluxes, far-infrared dust spectral energy distributions, and ~1mm dust photometry, in a large sample of 1444 star forming galaxies (SFGs) between z=0 and 4. The sample covers the stellar mass range log(M*/M_solar)=9.0-11.8, and star formation rates relative to that on the MS, delta_MS=SFR/SFR(MS), from 10^{-1.3} to 10^{2.2}. Our most important finding is that all data sets, despite the different techniques and analysis methods used, follow the same scaling trends, once method-to-method zero point offsets are minimized and uncertainties are properly taken into account. The molecular gas depletion time t_depl, defined as the ratio of molecular gas mass to star formation rate, scales as (1+z)^{-0.6}x(delta_MS)^{-0.44}, and is only weakly dependent on stellar mass. The ratio of molecular-to-stellar mass mu_gas depends on (1+z)^{2.5}x (delta_MS)^{0.52}x(M*)^{-0.36}, which tracks the evolution of the specific star formation rate. The redshift dependence of mu_gas requires a curvature term, as may the mass-dependences of t_depl and mu_gas. We find no or only weak correlations of t_depl and mu_gas with optical size R or surface density once one removes the above scalings, but we caution that optical sizes may not be appropriate for the high gas and dust columns at high-z.


The Astrophysical Journal | 2014

THE SCUBA-2 COSMOLOGY LEGACY SURVEY: ULTRALUMINOUS STAR-FORMING GALAXIES IN A z =1.6 CLUSTER

Ian Smail; J. E. Geach; A. M. Swinbank; Ken-ichi Tadaki; V. Arumugam; W. Hartley; Omar Almaini; Malcolm N. Bremer; Edward L. Chapin; S. C. Chapman; A. L. R. Danielson; A. C. Edge; D. Scott; Chris Simpson; J. M. Simpson; Christopher J. Conselice; James Dunlop; R. J. Ivison; A. Karim; Tadayuki Kodama; Alice Mortlock; E. I. Robson; I. G. Roseboom; A. P. Thomson; P. van der Werf; Tracy Margaret Anne Webb

We analyze new SCUBA-2 submillimeter and archival SPIRE far-infrared imaging of a z = 1.62 cluster, Cl 0218.3–0510, which lies in the UKIRT Infrared Deep Sky Survey/Ultra-Deep Survey field of the SCUBA-2 Cosmology Legacy Survey. Combining these tracers of obscured star-formation activity with the extensive photometric and spectroscopic information available for this field, we identify 31 far-infrared/submillimeter-detected probable cluster members with bolometric luminosities 1012 L ☉ and show that by virtue of their dust content and activity, these represent some of the reddest and brightest galaxies in this structure. We exploit ALMA submillimeter continuum observations, which cover one of these sources, to confirm the identification of a SCUBA-2-detected ultraluminous star-forming galaxy in this structure. Integrating the total star-formation activity in the central region of the structure, we estimate that it is an order of magnitude higher (in a mass-normalized sense) than clusters at z ~ 0.5-1. However, we also find that the most active cluster members do not reside in the densest regions of the structure, which instead host a population of passive and massive, red galaxies. We suggest that while the passive and active populations have comparable near-infrared luminosities at z = 1.6, MH ~ –23, the subsequent stronger fading of the more active galaxies means that they will evolve into passive systems at the present day that are less luminous than the descendants of those galaxies that were already passive at z ~ 1.6 (MH ~ –20.5 and MH ~ –21.5, respectively, at z ~ 0). We conclude that the massive galaxy population in the dense cores of present-day clusters were already in place at z = 1.6 and that in Cl 0218.3–0510 we are seeing continuing infall of less extreme, but still ultraluminous, star-forming galaxies onto a pre-existing structure.


The Astrophysical Journal | 2016

The evolution of metallicity and metallicity gradients from z = 2.7 to 0.6 with KMOS3D

Eva Wuyts; Emily Wisnioski; Matteo Fossati; Natascha M. Förster Schreiber; R. Genzel; R. I. Davies; J. Trevor Mendel; Thorsten Naab; Bernhard Röttgers; David J. Wilman; Stijn Wuyts; K. Bandara; A. Beifiori; Sirio Belli; Ralf Bender; Gabriel B. Brammer; Andreas Burkert; J. Chan; Audrey Galametz; Sandesh K. Kulkarni; P. Lang; D. Lutz; Ivelina Momcheva; Erica J. Nelson; D. Rosario; R. P. Saglia; S. Seitz; L. J. Tacconi; Ken-ichi Tadaki; Hannah Übler

We present measurements of the [N II]/H alpha ratio as a probe of gas-phase oxygen abundance for a sample of 419 star-forming galaxies at z = 0.6-2.7 from the KMOS3D near-IR multi-integral field unit (IFU) survey. The mass-metallicity relation (MZR) is determined consistently with the same sample selection, metallicity tracer, and methodology over the wide redshift range probed by the survey. We find good agreement with long-slit surveys in the literature, except for the low-mass slope of the relation at z similar to 2.3, where this sample is less biased than previous samples based on optical spectroscopic redshifts. In this regime we measure a steeper slope than some literature results. Excluding the contribution from active galactic nuclei from the MZR reduces sensitivity at the high-mass end, but produces otherwise consistent results. There is no significant dependence of the [N II]/H alpha ratio on star formation rate. at fixed redshift and stellar mass. The IFU data allow spatially resolved measurements of [N II]/H alpha, from which we can infer abundance gradients for 180. galaxies, thus tripling the current sample in the literature. The observed gradients are on average flat, with only 15 gradients statistically offset from zero at > 3 sigma. We have modeled the effect of beam. smearing, assuming a smooth intrinsic radial gradient and known seeing, inclination, and effective radius for each galaxy. Our seeing-limited observations can recover up to 70% of the intrinsic gradient for the largest, face-on disks, but only 30% for the smaller, more inclined galaxies. We do not find significant trends between observed or corrected gradients and any stellar population, dynamical, or structural galaxy parameters, mostly in agreement with existing studies with much smaller sample sizes. In cosmological simulations, strong feedback is generally required to produce flat gradients at high redshift.


Monthly Notices of the Royal Astronomical Society | 2015

An early phase of environmental effects on galaxy properties unveiled by near-infrared spectroscopy of protocluster galaxies at z > 2

Rhythm Shimakawa; Tadayuki Kodama; Ken-ichi Tadaki; Masao Hayashi; Yusei Koyama; Ichi Tanaka

This work presents the results from our near-infrared spectroscopy of narrow-band selected Hα emitters (HAEs) in two rich protoclusters (PKS 1138–262 at z=2.2 and USS 1558–003 at z = 2.5) with the Multi-Object Infrared Camera and Spectrograph (MOIRCS) on the Subaru telescope. These protoclusters are the ancestors of the most massive class of galaxy clusters seen today. The identified HAEs at z > 2 show very high excitation levels as characterized by much higher [Oiii]/Hβ line ratios than those of low-z galaxies. Such a high excitation level is qualitatively driven by their high specific star formation rates (sSFRs) and lower gaseous metallicities. Furthermore, we investigate the environmental dependence of gaseous metallicities by comparing the HAEs in the protoclustrers with those in the general field at similar redshifts. We find that the gaseous metallicities of protocluster galaxies are more chemically enriched than those of field galaxies at a given stellar mass in the range of M⋆ . 10 11 M⊙. This can be attributed to many processes, such as intrinsic (or nature) effects, external (or nurture) effects, and some systematic effects (sampling bias). The intrinsic (nature) effects include the advanced stage of “downsizing” galaxy evolution. On the other hands, the external (nurture) effects include the recycling of chemically enriched gas due to the higher pressure of inter galactic medium or stripping of outer gas in the reservoir in protoclusters. Although, none of the interpretation is perfect, the external effects such as gas recycling or stripping seem to be favored.


The Astrophysical Journal | 2013

Nature of Hα Selected Galaxies at z > 2. I. Main-sequence and Dusty Star-forming Galaxies

Ken-ichi Tadaki; Tadayuki Kodama; Ichi Tanaka; Masao Hayashi; Yusei Koyama; Rhythm Shimakawa

We present the results from our narrow-band imaging surveys of Hα emitters (HAEs) at z = 2.2 and z = 2.5 in the Subaru/XMM-Newton Deep survey Field with near-infrared camera MOIRCS on the Subaru Telescope. We have constructed a clean sample of 63 star-forming galaxies at z = 2.2 and 46 at z = 2.5. For 12 (or ~92%) out of 13 HAEs at z = 2.2, their Hα emission lines have been successfully detected by the spectroscopy. While about 42% of the red, massive HAEs with M * > 1010.8 M ☉ contain active galactic nuclei (AGNs), most of the blue, less massive ones are likely to be star-forming galaxies. This suggests that the AGN may play an important role in galaxy evolution at the late stage of truncation. For the HAEs excluding possible AGNs, we estimate the gas-phase metallicities on the basis of [N II]/Hα ratios, and find that the metallicities of the Hα selected galaxies at z = 2.2 are lower than those of local star-forming galaxies at fixed stellar mass, as shown by previous studies. Moreover, we present and discuss the so-called main sequence of star-forming galaxies at z > 2 based on our unique sample of HAEs. By correlating the level of dust extinction with the location on the main sequence, we find that there are two kinds/modes of dusty star-forming galaxies: starbursting galaxies and metal-rich normal star-forming galaxies.


Monthly Notices of the Royal Astronomical Society | 2014

Star formation in the cluster CLG0218.3-0510 at z = 1.62 and its large-scale environment: the infrared perspective

J. S. Santos; B. Altieri; M. Tanaka; I. Valtchanov; A. Saintonge; Mark Dickinson; S. Foucaud; Tadayuki Kodama; T. D. Rawle; Ken-ichi Tadaki

The galaxy cluster CLG0218.3-0510 at z=1.62 is one of the most distant galaxy clusters known, with a rich muti-wavelength data set that confirms a mature galaxy population already in place. Using very deep, wide area (20x20 Mpc) imaging by Spitzer/MIPS at 24um, in conjunction with Herschel 5-band imaging from 100-500um, we investigate the dust-obscured, star-formation properties in the cluster and its associated large scale environment. Our galaxy sample of 693 galaxies at z=1.62 detected at 24um (10 spectroscopic and 683 photo-z) includes both cluster galaxies (i.e. within r <1 Mpc projected clustercentric radius) and field galaxies, defined as the region beyond a radius of 3 Mpc. The star-formation rates (SFRs) derived from the measured infrared luminosity range from 18 to 2500 Ms/yr, with a median of 55 Ms/yr, over the entire radial range (10 Mpc). The cluster brightest FIR galaxy, taken as the centre of the galaxy system, is vigorously forming stars at a rate of 256


The Astrophysical Journal | 2017

Galaxy Environment in the 3D-HST Fields: Witnessing the Onset of Satellite Quenching at z ~ 1–2

Matteo Fossati; David J. Wilman; J. T. Mendel; R. P. Saglia; Audrey Galametz; A. Beifiori; Ralf Bender; J. Chan; M. Fabricius; K. Bandara; Gabriel B. Brammer; R. Davies; N. M. Förster Schreiber; R. Genzel; W. G. Hartley; Sandesh K. Kulkarni; P. Lang; I. G. Momcheva; Erica J. Nelson; R. Skelton; L. J. Tacconi; Ken-ichi Tadaki; Hannah Übler; P. G. van Dokkum; Emily Wisnioski; Katherine E. Whitaker; Eva Wuyts; Stijn Wuyts

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Tadayuki Kodama

Graduate University for Advanced Studies

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Rhythm Shimakawa

Graduate University for Advanced Studies

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Moegi Yamamoto

Graduate University for Advanced Studies

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