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Featured researches published by Li-Ting Hsu.


The Astrophysical Journal | 2013

CANDELS: The Progenitors of Compact Quiescent Galaxies at z 2

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.


Astronomy and Astrophysics | 2014

X-ray spectral modelling of the AGN obscuring region in the CDFS: Bayesian model selection and catalogue

Jörg Büchner; A. Georgakakis; Kirpal Nandra; Li-Ting Hsu; Cyprian Rangel; M. Brightman; Andrea Merloni; M. Salvato; J. L. Donley; D. D. Kocevski

Aims. Active galactic nuclei are known to have complex X-ray spectra that depend on both the properties of the accreting super-massive black hole (e.g. mass, accretion rate) and the distribution of obscuring material in its vicinity (i.e. the “torus”). Often however, simple and even unphysical models are adopted to represent the X-ray spectra of AGN, which do not capture the complexity and diversity of the observations. In the case of blank field surveys in particular, this should have an impact on e.g. the determination of the AGN luminosity function, the inferred accretion history of the Universe and also on our understanding of the relation between AGN and their host galaxies. Methods. We develop a Bayesian framework for model comparison and parameter estimation of X-ray spectra. We take into account uncertainties associated with both the Poisson nature of X-ray data and the determination of source redshift using photometric methods. We also demonstrate how Bayesian model comparison can be used to select among ten di erent physically motivated X-ray spectral models the one that provides a better representation of the observations. This methodology is applied to X-ray AGN in the 4 Ms Chandra Deep Field South. Results. For the 350 AGN in that field, our analysis identifies four components needed to represent the diversity of the observed X-ray spectra: (1) an intrinsic power law; (2) a cold obscurer which reprocesses the radiation due to photo-electric absorption, Compton scattering and Fe-K fluorescence; (3) an unabsorbed power law associated with Thomson scattering o ionised clouds; and (4) Compton reflection, most noticeable from a stronger-than-expected Fe-K line. Simpler models, such as a photo-electrically absorbed power law with a Thomson scattering component, are ruled out with decisive evidence (B > 100). We also find that ignoring the Thomson scattering component results in underestimation of the inferred column density, NH, of the obscurer. Regarding the geometry of the obscurer, there is strong evidence against both a completely closed (e.g. sphere), or entirely open (e.g. blob of material along the line of sight), toroidal geometry in favour of an intermediate case. Conclusions. Despite the use of low-count spectra, our methodology is able to draw strong inferences on the geometry of the torus. Simpler models are ruled out in favour of a geometrically extended structure with significant Compton scattering. We confirm the presence of a soft component, possibly associated with Thomson scattering o ionised clouds in the opening angle of the torus. The additional Compton reflection required by data over that predicted by toroidal geometry models, may be a sign of a density gradient in the torus or reflection o the accretion disk. Finally, we release a catalogue of AGN in the CDFS with estimated parameters such as the accretion luminosity in the 2 10 keV band and the column density, NH, of the obscurer.


The Astrophysical Journal | 2015

Obscuration-dependent Evolution of Active Galactic Nuclei

Johannes Buchner; A. Georgakakis; Kirpal Nandra; M. Brightman; Marie-Luise Menzel; Zhu Liu; Li-Ting Hsu; M. Salvato; Cyprian Rangel; James Aird; Andrea Merloni; Nicholas P. Ross

We aim to constrain the evolution of AGN as a function of obscuration using an X-ray selected sample of


The Astrophysical Journal | 2015

STELLAR MASSES FROM THE CANDELS SURVEY: THE GOODS-SOUTH AND UDS FIELDS

P. Santini; Henry C. Ferguson; A. Fontana; Bahram Mobasher; Guillermo Barro; M. Castellano; Steven L. Finkelstein; A. Grazian; Li-Ting Hsu; Bomee Lee; Sang-Gak Lee; Janine Pforr; M. Salvato; Tommy Wiklind; Stijn Wuyts; Omar Almaini; Michael C. Cooper; Audrey Galametz; Benjamin J. Weiner; R. Amorin; K. Boutsia; Christopher J. Conselice; Tomas Dahlen; M. Dickinson; Mauro Giavalisco; Norman A. Grogin; Yicheng Guo; Nimish P. Hathi; Dale D. Kocevski; Anton M. Koekemoer

\sim2000


The Astrophysical Journal | 2014

CANDELS/GOODS-S, CDFS, and ECDFS: photometric redshifts for normal and x-ray-detected galaxies

Li-Ting Hsu; M. Salvato; Kirpal Nandra; M. Brusa; Ralf Bender; Johannes Buchner; J. L. Donley; Dale D. Kocevski; Yicheng Guo; Nimish P. Hathi; Cyprian Rangel; S. P. Willner; M. Brightman; A. Georgakakis; Tamas Budavari; Alexander S. Szalay; Matthew L. N. Ashby; Guillermo Barro; Tomas Dahlen; Sandra M. Faber; Henry C. Ferguson; Audrey Galametz; Andrea Grazian; Norman A. Grogin; Kuang-Han Huang; Anton M. Koekemoer; Ray A. Lucas; Elizabeth J. McGrath; Bahram Mobasher; Michael Peth

AGN from a multi-tiered survey including the CDFS, AEGIS-XD, COSMOS and XMM-XXL fields. The spectra of individual X-ray sources are analysed using a Bayesian methodology with a physically realistic model to infer the posterior distribution of the hydrogen column density and intrinsic X-ray luminosity. We develop a novel non-parametric method which allows us to robustly infer the distribution of the AGN population in X-ray luminosity, redshift and obscuring column density, relying only on minimal smoothness assumptions. Our analysis properly incorporates uncertainties from low count spectra, photometric redshift measurements, association incompleteness and the limited sample size. We find that obscured AGN with


Monthly Notices of the Royal Astronomical Society | 2014

Compton thick active galactic nuclei in Chandra surveys

M. Brightman; Kirpal Nandra; M. Salvato; Li-Ting Hsu; James Aird; Cyprian Rangel

N_{H}>{\rm 10^{22}\, cm^{-2}}


Monthly Notices of the Royal Astronomical Society | 2015

The X-ray luminosity function of active galactic nuclei in the redshift interval z=3-5

A. Georgakakis; James Aird; Johannes Buchner; M. Salvato; Marie-Luise Menzel; W. N. Brandt; Ian D. McGreer; Tom Dwelly; G. Mountrichas; C. Koki; I. Georgantopoulos; Li-Ting Hsu; Andrea Merloni; Z. Liu; Kirpal Nandra; Nicholas P. Ross

account for


The Astronomical Journal | 2015

A WFC3 GRISM EMISSION LINE REDSHIFT CATALOG IN THE GOODS-SOUTH FIELD

Aaron M. Morris; Dale D. Kocevski; Jonathan R. Trump; Benjamin J. Weiner; Nimish P. Hathi; Guillermo Barro; Tomas Dahlen; Sandra M. Faber; Steven L. Finkelstein; A. Fontana; Henry C. Ferguson; Norman A. Grogin; Ruth Grützbauch; Yicheng C. Guo; Li-Ting Hsu; Anton M. Koekemoer; David C. Koo; Bahram Mobasher; Janine Pforr; M. Salvato; Tommy Wiklind; Stijn Wuyts

{77}^{+4}_{-5}\%


Astrophysical Journal Supplement Series | 2015

AEGIS-X: DEEP CHANDRA IMAGING OF THE CENTRAL GROTH STRIP

K. Nandra; E. S. Laird; James Aird; M. Salvato; A. Georgakakis; Guillermo Barro; P. G. Pérez-González; Pauline Barmby; R.-R. Chary; Alison L. Coil; Michael C. Cooper; M. Davis; M. Dickinson; S. M. Faber; Giovanni G. Fazio; Puragra Guhathakurta; Stephen D. J. Gwyn; Li-Ting Hsu; J.-S. Huang; R. J. Ivison; David C. Koo; J. A. Newman; C. Rangel; Toru Yamada; Christopher N. A. Willmer

of the number density and luminosity density of the accretion SMBH population with


Monthly Notices of the Royal Astronomical Society | 2014

Investigating Evidence for Different Black Hole Accretion Modes since Redshift z ∼ 1

A. Georgakakis; P. G. Pérez-González; N. Fanidakis; M. Salvato; James Aird; H. Messias; Jennifer M. Lotz; Guillermo Barro; Li-Ting Hsu; Kirpal Nandra; D. Rosario; Michael C. Cooper; D. D. Kocevski; J. A. Newman

L_{{\rm X}}>10^{43}\text{ erg/s}

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Anton M. Koekemoer

Association of Universities for Research in Astronomy

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David C. Koo

University of California

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Henry C. Ferguson

Space Telescope Science Institute

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Nimish P. Hathi

Space Telescope Science Institute

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Norman A. Grogin

Space Telescope Science Institute

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