TY - JOUR
T1 - A Lyα blob and zabs ≈ zem damped Lyα absorber in the dark matter halo of the binary quasar Q 0151+048
AU - Zafar, T.
AU - Møller, P.
AU - Ledoux, C.
AU - Fynbo, J. P. U.
AU - Nilsson, K. K.
AU - Christensen, L.
AU - D'Odorico, S.
AU - Milvang-Jensen, B.
AU - Michałowski, M. J.
AU - Ferreira, D. D. M.
PY - 2011/8/1
Y1 - 2011/8/1
N2 - Context. Q 0151+048 is a physical quasar (QSO) pair at z ~ 1.929 with a
separation of 3.3 arcsec on the sky. In the spectrum of the brighter
member of this pair, Q 0151+048A, a damped Lyα absorber (DLA) is
observed at a higher redshift. We have previously detected the host
galaxies of both QSOs, as well as a Lyα blob whose emission
surrounding Q 0151+048A extends over 5 × 3.3 arcsec. Aims:
We seek to constrain the geometry of the system and understand the
possible relations between the DLA, the Lyα blob, and the two
QSOs. We also aim at characterizing the former two objects in more
detail. Methods: To study the nature of the Lyα blob, we
performed low-resolution, long-slit spectroscopy with the slit aligned
with the extended emission. We also observed the whole system using the
medium-resolution VLT/X-shooter spectrograph and the slit aligned with
the two QSOs. The systemic redshift of both QSOs was determined from
rest-frame optical emission lines redshifted into the NIR. We employed
line-profile fitting technique, to measure metallicities and the
velocity width of low-ionization metal absorption lines associated to
the DLA and photo-ionization modeling to characterize the DLA further.
Results: We measure systemic redshifts of zem(A) =
1.92924 ± 0.00036 and zem(B) = 1.92863 ±
0.00042 from the H β and H α emission lines, respectively. In
other words, the two QSOs have identical redshifts within 2σ. From
the width of Balmer emission lines and the strength of the rest-frame
optical continuum, we estimate the masses of the black holes of the two
QSOs to be 109.33 M&sun; and 108.38
M&sun; for Q 0151+048A and Q 0151+048B, respectively. We then
use the correlation between black hole mass and dark matter halo mass to
infer the mass of the dark matter halos hosting the two QSOs:
1013.74 M&sun; and 1013.13
M&sun; for Q 0151+048A and Q 0151+048B, respectively. We
observe a velocity gradient along the major axis of the Lyα blob
consistent with the rotation curve of a large disk galaxy, but it may
also be caused by gas inflow or outflow. We detect residual continuum in
the DLA trough, which we interpret as emission from the host galaxy of Q
0151+048A. The derived H0 column density of the DLA is log
NH0 = 20.34 ± 0.02 cm-2. Metal
column densities are also determined for a number of low-ionization
species resulting in an overall metallicity of 0.01 Z&sun;.
We detect C ii ∗ , which allows us to make a physical
model of the DLA cloud. Conclusions: From the systemic redshifts
of the QSOs, we conclude that the Lyα blob is associated with Q
0151+048A rather than with the DLA. The DLA must be located in front of
both the Lyα blob and Q 0151+048A at a distance greater than 30
kpc and has a velocity relative to the blob of 640 ± 70 km
s-1. The two quasars accrete at normal Eddington ratios. The
DM halo of this double quasar will grow to the mass of our local
supercluster at z = 0. We point out that those objects therefore form an
ideal laboratory to study the physical interactions in a z = 2 precursor
of our local supercluster.
Based on observations done with i) European Southern Observatory (ESO)
utilizing 8.2m Very Large Telescope (VLT) X-shooter spectrograph on
Cerro Paranal in the Atacama Desert, northern Chile. ii) 2.56 m Nordic
Optical Telescope (NOT), a scientific association between Denmark,
Finland, Iceland, Norway and Sweden, operated at Observatorio del Roque
de Los Muchachos on the island of La Palma, Spain.
AB - Context. Q 0151+048 is a physical quasar (QSO) pair at z ~ 1.929 with a
separation of 3.3 arcsec on the sky. In the spectrum of the brighter
member of this pair, Q 0151+048A, a damped Lyα absorber (DLA) is
observed at a higher redshift. We have previously detected the host
galaxies of both QSOs, as well as a Lyα blob whose emission
surrounding Q 0151+048A extends over 5 × 3.3 arcsec. Aims:
We seek to constrain the geometry of the system and understand the
possible relations between the DLA, the Lyα blob, and the two
QSOs. We also aim at characterizing the former two objects in more
detail. Methods: To study the nature of the Lyα blob, we
performed low-resolution, long-slit spectroscopy with the slit aligned
with the extended emission. We also observed the whole system using the
medium-resolution VLT/X-shooter spectrograph and the slit aligned with
the two QSOs. The systemic redshift of both QSOs was determined from
rest-frame optical emission lines redshifted into the NIR. We employed
line-profile fitting technique, to measure metallicities and the
velocity width of low-ionization metal absorption lines associated to
the DLA and photo-ionization modeling to characterize the DLA further.
Results: We measure systemic redshifts of zem(A) =
1.92924 ± 0.00036 and zem(B) = 1.92863 ±
0.00042 from the H β and H α emission lines, respectively. In
other words, the two QSOs have identical redshifts within 2σ. From
the width of Balmer emission lines and the strength of the rest-frame
optical continuum, we estimate the masses of the black holes of the two
QSOs to be 109.33 M&sun; and 108.38
M&sun; for Q 0151+048A and Q 0151+048B, respectively. We then
use the correlation between black hole mass and dark matter halo mass to
infer the mass of the dark matter halos hosting the two QSOs:
1013.74 M&sun; and 1013.13
M&sun; for Q 0151+048A and Q 0151+048B, respectively. We
observe a velocity gradient along the major axis of the Lyα blob
consistent with the rotation curve of a large disk galaxy, but it may
also be caused by gas inflow or outflow. We detect residual continuum in
the DLA trough, which we interpret as emission from the host galaxy of Q
0151+048A. The derived H0 column density of the DLA is log
NH0 = 20.34 ± 0.02 cm-2. Metal
column densities are also determined for a number of low-ionization
species resulting in an overall metallicity of 0.01 Z&sun;.
We detect C ii ∗ , which allows us to make a physical
model of the DLA cloud. Conclusions: From the systemic redshifts
of the QSOs, we conclude that the Lyα blob is associated with Q
0151+048A rather than with the DLA. The DLA must be located in front of
both the Lyα blob and Q 0151+048A at a distance greater than 30
kpc and has a velocity relative to the blob of 640 ± 70 km
s-1. The two quasars accrete at normal Eddington ratios. The
DM halo of this double quasar will grow to the mass of our local
supercluster at z = 0. We point out that those objects therefore form an
ideal laboratory to study the physical interactions in a z = 2 precursor
of our local supercluster.
Based on observations done with i) European Southern Observatory (ESO)
utilizing 8.2m Very Large Telescope (VLT) X-shooter spectrograph on
Cerro Paranal in the Atacama Desert, northern Chile. ii) 2.56 m Nordic
Optical Telescope (NOT), a scientific association between Denmark,
Finland, Iceland, Norway and Sweden, operated at Observatorio del Roque
de Los Muchachos on the island of La Palma, Spain.
UR - http://www.scopus.com/inward/record.url?scp=79960634310&partnerID=8YFLogxK
U2 - 10.1051/0004-6361/201016332
DO - 10.1051/0004-6361/201016332
M3 - Article
SN - 0004-6361
VL - 532
SP - 51
JO - Astronomy & Astrophysics
JF - Astronomy & Astrophysics
ER -