32 research outputs found
Obscuration beyond the nucleus: infrared quasars can be buried in extreme compact starbursts
\ua9 The Author(s) 2023. In the standard quasar model, the accretion disc obscuration is due to the canonical dusty torus. Here, we argue that a substantial part of the quasar obscuration can come from the interstellar medium (ISM) when the quasars are embedded in compact starbursts. We use an obscuration-unbiased sample of 578 infrared (IR) quasars at z ≈ 1–3 and archival Atacama Large Millimetre/submillimetre Array submillimetre host galaxy sizes to investigate the ISM contribution to the quasar obscuration. We calculate star formation rates (SFR) and ISM column densities for the IR quasars and a control sample of submillimetre galaxies (SMGs) not hosting quasar activity and show that: (1) the quasar obscured fraction is constant up to SFR ≈ 300 M☉ yr−1, and then increases towards higher SFR, suggesting that the ISM obscuration plays a significant role in starburst host galaxies, and (2) at SFR ≳ 300 M☉ yr−1, the SMGs and IR quasars have similarly compact submillimetre sizes (Re ≈ 0.5–3 kpc) and consequently, the ISM can heavily obscure the quasar, even reaching Compton-thick (NH > 1024 cm−2) levels in extreme cases. Based on our results, we infer that ≈10–30 per cent of the IR quasars with SFR ≳ 300 M☉ yr−1 are obscured solely by the ISM
Discrete sources as the origin of the Galactic X-ray ridge emission
An unresolved X-ray glow (at energies above a few kiloelectronvolts) was
discovered about 25 years ago and found to be coincident with the Galactic disk
-the Galactic ridge X-ray emission. This emission has a spectrum characteristic
of a 1e8 K optically thin thermal plasma, with a prominent iron emission line
at 6.7 keV. The gravitational well of the Galactic disk, however, is far too
shallow to confine such a hot interstellar medium; instead, it would flow away
at a velocity of a few thousand kilometres per second, exceeding the speed of
sound in gas. To replenish the energy losses requires a source of 10^{43}
erg/s, exceeding by orders of magnitude all plausible energy sources in the
Milky Way. An alternative is that the hot plasma is bound to a multitude of
faint sources, which is supported by the recently observed similarities in the
X-ray and near-infrared surface brightness distributions (the latter traces the
Galactic stellar distribution). Here we report that at energies of 6-7 keV,
more than 80 per cent of the seemingly diffuse X-ray emission is resolved into
discrete sources, probably accreting white dwarfs and coronally active stars.Comment: 16 pages, 3 figures. Draft version of the paper that will appear in
Nature, Issue April 30, 200
Observations of Ly Emitters at High Redshift
In this series of lectures, I review our observational understanding of
high- Ly emitters (LAEs) and relevant scientific topics. Since the
discovery of LAEs in the late 1990s, more than ten (one) thousand(s) of LAEs
have been identified photometrically (spectroscopically) at to . These large samples of LAEs are useful to address two major astrophysical
issues, galaxy formation and cosmic reionization. Statistical studies have
revealed the general picture of LAEs' physical properties: young stellar
populations, remarkable luminosity function evolutions, compact morphologies,
highly ionized inter-stellar media (ISM) with low metal/dust contents, low
masses of dark-matter halos. Typical LAEs represent low-mass high- galaxies,
high- analogs of dwarf galaxies, some of which are thought to be candidates
of population III galaxies. These observational studies have also pinpointed
rare bright Ly sources extended over kpc, dubbed
Ly blobs, whose physical origins are under debate. LAEs are used as
probes of cosmic reionization history through the Ly damping wing
absorption given by the neutral hydrogen of the inter-galactic medium (IGM),
which complement the cosmic microwave background radiation and 21cm
observations. The low-mass and highly-ionized population of LAEs can be major
sources of cosmic reionization. The budget of ionizing photons for cosmic
reionization has been constrained, although there remain large observational
uncertainties in the parameters. Beyond galaxy formation and cosmic
reionization, several new usages of LAEs for science frontiers have been
suggested such as the distribution of {\sc Hi} gas in the circum-galactic
medium and filaments of large-scale structures. On-going programs and future
telescope projects, such as JWST, ELTs, and SKA, will push the horizons of the
science frontiers.Comment: Lecture notes for `Lyman-alpha as an Astrophysical and Cosmological
Tool', Saas-Fee Advanced Course 46. Verhamme, A., North, P., Cantalupo, S., &
Atek, H. (eds.) --- 147 pages, 103 figures. Abstract abridged. Link to the
lecture program including the video recording and ppt files :
https://obswww.unige.ch/Courses/saas-fee-2016/program.cg
Narrow-line region gas kinematics of 24 264 optically selected AGN: The radio connection
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X-RAY DETECTED ACTIVE GALACTIC NUCLEI IN DWARF GALAXIES AT 0 < z < 1
We present a sample of accreting supermassive black holes (SMBHs) in dwarf galaxies at z < 1. We identify dwarf galaxies in the NEWFIRM Medium Band Survey with stellar masses of M-star < 3 x 10(9) M-circle dot that have spectroscopic redshifts from the DEEP2 survey and lie within the region covered by deep ( flux limit of similar to 5 x 10(-17)-6 x 10(-16) erg cm(-2) s(-1)) archival Chandra X-ray data. From our sample of 605 dwarf galaxies, 10 exhibit X-ray emission consistent with that arising from active galactic nucleus (AGN) activity. If black-hole mass scales roughly with stellar mass, then we expect that these AGNs are powered by SMBHs with masses of similar to 10(5)-10(6) M-circle dot and typical Eddington ratios of similar to 5%. Furthermore, we find an AGN fraction consistent with extrapolations of other searches of similar to 0.6%-3% for 10(9) M-circle dot. M-star <= 3 x 10(9) M-circle dot and 0.1 < z < 0.6. Our AGN fraction is in good agreement with a semi-analytic model, suggesting that, as we search larger volumes, we may use comparisons between observed AGN fractions and models to understand seeding mechanisms in the early universe
