scholarly journals Resolved [C ii] Emission from z > 6 Quasar Host–Companion Galaxy Pairs

2019 ◽  
Vol 882 (1) ◽  
pp. 10 ◽  
Author(s):  
Marcel Neeleman ◽  
Eduardo Bañados ◽  
Fabian Walter ◽  
Roberto Decarli ◽  
Bram P. Venemans ◽  
...  
Keyword(s):  
2000 ◽  
Vol 119 (1) ◽  
pp. 59-62 ◽  
Author(s):  
Gabriela Canalizo ◽  
Alan Stockton ◽  
M. S. Brotherton ◽  
Wil van Breugel
Keyword(s):  

2001 ◽  
Vol 205 ◽  
pp. 346-347
Author(s):  
P. Planesas ◽  
J. Martin-Pintado ◽  
R. Neri ◽  
L. Colina

Molecular gas in the host galaxy of the lensed quasar QSO 0957+561 has been detected at the redshift of 1.414 using the IRAM Plateau de Bure interferometer. This detection shows the extended nature of the molecular gas distribution. The molecular gas mass is 2-4 109 M⊙ and it is distributed in a disk that is several kiloparsecs in diameter. A second, weaker component of CO is interpreted as arising from a close companion galaxy moving at a velocity 440 km s−1 higher than the host galaxy.


1990 ◽  
Vol 124 ◽  
pp. 231-244
Author(s):  
V. P. Reshetnikov ◽  
V. A. Yakovleva

Polar-ring galaxies (PRG) are among the most interesting examples of interaction between galaxies. A PRG is a galaxy with an elongated main body surrounded by a ring (or a disk) of stars, gas, and dust rotating in a near-polar plane (Schweizer, Whitmore, and Rubin, 1983). Accretion of matter by a massive lenticular galaxy from either intergalactic medium or a companion galaxy is usually considered as an explanation of the observed structure of PRG. In the latter case there are two possibilities: (1) capture and merging of a neighbor galaxy, and (2) accretion of mass from a companion galaxy during a close encounter. Two PRG formation scenarios just mentioned are illustrated here by the results of our observations of the peculiar galaxies NGC 2685 and NGC 3808B.


1990 ◽  
Vol 124 ◽  
pp. 437-440
Author(s):  
W. Kollatschny ◽  
K.J. Fricke

The occurrence and quantitative properties of Seyfert 1 and Seyfert 2 galaxies as a function of the galaxy environment have been studied in a systematic way. For this investigation we have selected from the Catalogue of Quasars and Active Nuclei (Veron & Veron, 1989) all Seyfert galaxies with the following properties:(i) mV ≤ 15,(ii) listed classification as Sey 1, Sey 2, or Sey 3,(iii) vrad ≤ 20000 km s-1.This results in a sample size of 242 Seyfert galaxies. For all these objects their galaxy environment has been inspected on POSS and ESO/SRC plates.The vicinity of each sample Seyfert galaxy was searched for companion galaxies out to at least 0.5 Mpc. Lacking redshift information we adopted as a companion galaxy any galaxy in this area having a size between 20 and 200 percent of the Seyfert galaxy size.


2019 ◽  
Vol 628 ◽  
pp. L6 ◽  
Author(s):  
F. Vito ◽  
W. N. Brandt ◽  
F. E. Bauer ◽  
R. Gilli ◽  
B. Luo ◽  
...  

While theoretical arguments predict that most of the early growth of supermassive black holes (SMBHs) happened during heavily obscured phases of accretion, current methods used for selecting z >  6 quasars (QSOs) are strongly biased against obscured QSOs, thus considerably limiting our understanding of accreting SMBHs during the first gigayear of the Universe from an observational point of view. We report the Chandra discovery of the first heavily obscured QSO candidate in the early universe, hosted by a close (≈5 kpc) galaxy pair at z = 6.515. One of the members is an optically classified type-1 QSO, PSO167–13. The companion galaxy was first detected as a [C II] emitter by Atacama large millimeter array (ALMA). An X-ray source is significantly (P = 0.9996) detected by Chandra in the 2–5 keV band, with < 1.14 net counts in the 0.5–2 keV band, although the current positional uncertainty does not allow a conclusive association with either PSO167–13 or its companion galaxy. From X-ray photometry and hardness-ratio arguments, we estimated an obscuring column density of NH >  2 × 1024 cm−2 and NH >  6 × 1023 cm−2 at 68% and 90% confidence levels, respectively. Thus, regardless of which of the two galaxies is associated with the X-ray emission, this source is the first heavily obscured QSO candidate at z >  6.


1990 ◽  
Vol 124 ◽  
pp. 473-477
Author(s):  
C.L. Carilli ◽  
J.H. van Gorkom ◽  
E.M. Hauxthausen ◽  
J.T. Stocke ◽  
J. Salzer

There are a number of known quasars for which our line of sight to the high redshift quasar passes within a few Holmberg radii of a low redshift galaxy. In a few of these cases, spectra of the quasar reveal absorption by gas associated with the low redshift galaxy. A number of these pairs imply absorption by gas which lies well outside the optical disk of the associated galaxy, leading to models of galaxies with ‘halos’ or ‘disks’ of gas extending to large radii. We present observations of 4 such pairs. In three of the four cases, we find that the associated galaxy is highly disturbed, typically due to a gravitational interaction with a companion galaxy, while in the fourth case the absorption can be explained by clouds in the optical disk of the associated galaxy. We are led to an alternative hypothesis concerning the origin of the low redshift absorption line systems: the absorption is by gas clouds which have been gravitationally stripped from the associated galaxy. These galaxies are rapidly evolving, and should not be used as examples of absorption by clouds in halos of field spirals. We conclude by considering the role extended gas in interacting systems plays in the origin of higher redshift quasar absorption line systems.


2004 ◽  
Vol 128 (6) ◽  
pp. 2704-2711 ◽  
Author(s):  
Youichi Ohyama ◽  
Yoshiaki Taniguchi ◽  
Yasuhiro Shioya

1995 ◽  
Vol 447 (1) ◽  
pp. L1-L4 ◽  
Author(s):  
John N. Bahcall ◽  
Sofia Kirhakos ◽  
Donald P. Schneider
Keyword(s):  

1996 ◽  
Vol 471 (2) ◽  
pp. L87-L90 ◽  
Author(s):  
Reginald J. Dufour ◽  
César Esteban ◽  
Héctor O. Castañeda
Keyword(s):  

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