S. Marchesi
Clemson University
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Featured researches published by S. Marchesi.
The Astrophysical Journal | 2016
F. Civano; S. Marchesi; A. Comastri; Meg Urry; M. Elvis; N. Cappelluti; S. Puccetti; M. Brusa; G. Zamorani; Guenther Hasinger; T. Aldcroft; D. M. Alexander; V. Allevato; H. Brunner; P. Capak; Alexis Finoguenov; F. Fiore; Antonella Fruscione; R. Gilli; K. Glotfelty; Richard E. Griffiths; Heng Hao; Fiona A. Harrison; Knud Jahnke; J. Kartaltepe; A. Karim; Stephanie M. LaMassa; G. Lanzuisi; Takamitsu Miyaji; P. Ranalli
The COSMOS-Legacy survey is a 4.6 Ms Chandra program that has imaged 2.2 deg2 of the COSMOS field with an effective exposure of ≃ 160 ks over the central 1.5 deg^2 and of ≃ 80 ks in the remaining area. The survey is the combination of 56 new observations obtained as an X-ray Visionary Project with the previous C-COSMOS survey. We describe the reduction and analysis of the new observations and the properties of 2273 point sources detected above a spurious probability of 2 × 10^(−5). We also present the updated properties of the C-COSMOS sources detected in the new data. The whole survey includes 4016 point sources (3814, 2920 and 2440 in the full, soft, and hard band). The limiting depths are 2.2 × 10^(−16), 1.5 × 10^(−15), and 8.9 × 10^(−16) erg cm^(-2)s^(-1) in the 0.5–2, 2–10, and 0.5–10 keV bands, respectively. The observed fraction of obscured active galactic nuclei with a column density >10^(22) cm^(−2) from the hardness ratio (HR) is 50_(-16)^(+17)%. Given the large sample we compute source number counts in the hard and soft bands, significantly reducing the uncertainties of 5%–10%. For the first time we compute number counts for obscured (HR > −0.2) and unobscured (HR < −0.2) sources and find significant differences between the two populations in the soft band. Due to the unprecedent large exposure, COSMOS-Legacy area is three times larger than surveys at similar depths and its depth is three times fainter than surveys covering similar areas. The area-flux region occupied by COSMOS-Legacy is likely to remain unsurpassed for years to come.
The Astrophysical Journal | 2016
S. Marchesi; F. Civano; M. Elvis; M. Salvato; M. Brusa; A. Comastri; R. Gilli; G. Hasinger; G. Lanzuisi; Takamitsu Miyaji; Ezequiel Treister; Claudia M. Urry; C. Vignali; G. Zamorani; V. Allevato; N. Cappelluti; Carolin N. Cardamone; A. Finoguenov; Richard E. Griffiths; A. Karim; C. Laigle; Stephanie M. LaMassa; Knud Jahnke; P. Ranalli; Kevin Schawinski; Eva Schinnerer; J. D. Silverman; Vernesa Smolčić; Hyewon Suh; Benny Trakhtenbrot
We present the catalog of optical and infrared counterparts of the Chandra COSMOS-Legacy Survey, a 4.6 Ms Chandra program on the 2.2 deg2 of the COSMOS field, combination of 56 new overlapping observations obtained in Cycle 14 with the previous C-COSMOS survey. In this Paper we report the i, K, and 3.6 μm identifications of the 2273 X-ray point sources detected in the new Cycle 14 observations. We use the likelihood ratio technique to derive the association of optical/infrared (IR) counterparts for 97% of the X-ray sources. We also update the information for the 1743 sources detected in C-COSMOS, using new K and 3.6 μm information not available when the C-COSMOS analysis was performed. The final catalog contains 4016 X-ray sources, 97% of which have an optical/IR counterpart and a photometric redshift, while sime54% of the sources have a spectroscopic redshift. The full catalog, including spectroscopic and photometric redshifts and optical and X-ray properties described here in detail, is available online. We study several X-ray to optical (X/O) properties: with our large statistics we put better constraints on the X/O flux ratio locus, finding a shift toward faint optical magnitudes in both soft and hard X-ray band. We confirm the existence of a correlation between X/O and the the 2–10 keV luminosity for Type 2 sources. We extend to low luminosities the analysis of the correlation between the fraction of obscured AGNs and the hard band luminosity, finding a different behavior between the optically and X-ray classified obscured fraction.
Astronomy and Astrophysics | 2015
G. Lanzuisi; P. Ranalli; I. Georgantopoulos; A. Georgakakis; I. Delvecchio; T. Akylas; S. Berta; A. Bongiorno; M. Brusa; N. Cappelluti; F. Civano; A. Comastri; R. Gilli; C. Gruppioni; G. Hasinger; Kazushi Iwasawa; Anton M. Koekemoer; E. Lusso; S. Marchesi; V. Mainieri; Andrea Merloni; M. Mignoli; E. Piconcelli; F. Pozzi; D. Rosario; M. Salvato; J. D. Silverman; Benny Trakhtenbrot; C. Vignali; G. Zamorani
Heavily obscured, Compton thick (CT, NH > 10 24 cm −2 ) active galactic nuclei (AGN) may represent an important phase in AGN/galaxy co-evolution and are expected to provide a significant contribution to the cosmic X-ray background at its peak. However, unambiguously identifying CT AGN beyond the local Universe is a challenging task even in the deepest X-ray surveys, and given the expected low spatial density of these sources in the 2−10 keV band, large area surveys are needed to collect sizable samples. Through direct X-ray spectra analysis, we selected 39 heavily obscured AGN (NH > 3 × 10 23 cm −2 ) at bright X-ray fluxes (F2−10 > 10 −14 erg s −1 cm −2 )i n the 2d eg 2 XMM-COSMOS survey. After selecting CT AGN based on the fit of a simple absorbed two power law model to the shallow XMM-Newton data, the presence of bona fide CT AGN was confirmed in 80% of the sources using deeper Chandra data and more complex models. The final sample comprises ten CT AGN (six of them also have a detected Fe Kα line with EW ∼ 1 keV), spanning a wide range of redshifts (z ∼ 0.1−2.5) and luminosity (L2−10 ∼ 10 43.5 −10 45 erg s −1 )a nd is complemented by 29 heavily obscured AGN spanning the same redshift and luminosity range. We collected the rich multi-wavelength information available for all these sources, in order to study the distribution of super massive black hole and host properties, such as black hole mass (MBH), Eddington ratio (λEdd), stellar mass (M∗), specific star formation rate (sSFR) in comparison with a sample of unobscured AGN. We find that highly obscured sources tend to have significantly smaller MBH and higher λEdd with respect to unobscured sources, while a weaker evolution in M∗ is observed. The sSFR of highly obscured sources is consistent with the one observed in the main sequence of star forming galaxies, at all redshifts. We also present and briefly discuss optical spectra, broadband spectral energy distribution (SED) and morphology for the sample of ten CT AGN. Both the optical spectra and SED agree with the classification as highly obscured sources: all the available optical spectra are dominated by the stellar component of the host galaxy, and to reproduce the broadband SED, a highly obscured torus component is needed for all the CT sources. Exploiting the high resolution Hubble-ACS images available, we are able to show that these highly obscured sources have a significantly larger merger fraction with respect to other X-ray selected samples of AGN. Finally we discuss the implications of our findings in the context of AGN/galaxy co-evolutionary models, and compare our results with the predictions of X-ray background synthesis models.
The Astrophysical Journal | 2016
Mar Mezcua; F. Civano; G. Fabbiano; Takamitsu Miyaji; S. Marchesi
We study a sample of
The Astrophysical Journal | 2016
Stephanie M. LaMassa; C. Megan Urry; N. Cappelluti; H. Böhringer; A. Comastri; Eilat Glikman; Gordon T. Richards; Tonima Tasnim Ananna; M. Brusa; Carie Cardamone; Gayoung Chon; F. Civano; D. Farrah; M. Gilfanov; Paul J. Green; S. Komossa; Paulina Lira; Martin Makler; S. Marchesi; Robert Pecoraro; P. Ranalli; M. Salvato; Kevin Schawinski; Daniel Stern; Ezequiel Treister; M. Viero
\sim
Astronomy and Astrophysics | 2017
Vernesa Smolčić; I. Delvecchio; G. Zamorani; N. Baran; Mladen Novak; J. Delhaize; E. Schinnerer; S. Berta; Marco Bondi; P. Ciliegi; P. Capak; F. Civano; A. Karim; O. Le Fèvre; O. Ilbert; C. Laigle; S. Marchesi; H. J. McCracken; L. Tasca; M. Salvato; Eleni Vardoulaki
50,000 dwarf starburst and late-type galaxies drawn from the COSMOS survey with the aim of investigating the presence of nuclear accreting black holes (BHs) as those seed BHs from which supermassive BHs could grow in the early Universe. We divide the sample into five complete redshift bins up to
Astronomy and Astrophysics | 2017
J. Delhaize; Vernesa Smolčić; I. Delvecchio; Mario Novak; M. Sargent; N. Baran; B. Magnelli; G. Zamorani; E. Schinnerer; E. J. Murphy; M. Aravena; S. Berta; Marco Bondi; P. Capak; C. L. Carilli; P. Ciliegi; F. Civano; O. Ilbert; A. Karim; C. Laigle; O. Le Fèvre; S. Marchesi; H. J. McCracken; M. Salvato; N. Seymour; L. Tasca
z=1.5
The Astrophysical Journal | 2017
G. B. Lansbury; D. Stern; James Aird; D. M. Alexander; C. Fuentes; Fiona A. Harrison; Ezequiel Treister; F. E. Bauer; John A. Tomsick; M. Baloković; A. Del Moro; P. Gandhi; M. Ajello; A. Annuar; D. R. Ballantyne; S. E. Boggs; W. N. Brandt; M. Brightman; Chien-Ting J. Chen; Finn Erland Christensen; F. Civano; A. Comastri; William W. Craig; K. Forster; Brian W. Grefenstette; Charles J. Hailey; R. C. Hickox; B. Jiang; Hyunsung David Jun; Michael Koss
and perform an X-ray stacking analysis using the \textit{Chandra} COSMOS-Legacy survey data. After removing the contribution from X-ray binaries and hot gas to the stacked X-ray emission, we still find an X-ray excess in the five redshift bins that can be explained by nuclear accreting BHs. This X-ray excess is more significant for
The Astrophysical Journal | 2016
S. Marchesi; F. Civano; M. Salvato; Francesco Shankar; A. Comastri; M. Elvis; G. Lanzuisi; Benny Trakhtenbrot; C. Vignali; G. Zamorani; V. Allevato; M. Brusa; F. Fiore; R. Gilli; Richard E. Griffiths; Guenther Hasinger; Takamitsu Miyaji; Kevin Schawinski; Ezequiel Treister; Claudia M. Urry
z<0.5
The Astrophysical Journal | 2017
N. Cappelluti; Yanxia Li; Angelo Ricarte; Bhaskar Agarwal; V. Allevato; Tonima Tasnim Ananna; M. Ajello; F. Civano; A. Comastri; Martin Elvis; Alexis Finoguenov; R. Gilli; Guenther Hasinger; S. Marchesi; Priyamvada Natarajan; Fabio Pacucci; Ezequiel Treister; C. Megan Urry
. At higher redshifts, these active galactic nuclei could suffer mild obscuration, as indicated by the analysis of their hardness ratios. The average nuclear X-ray luminosities in the soft band are in the range 10