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We compare the near-infrared (NIR)
H-band photometric and morphological properties of low-
z (
z < 0.3) 3CR radio galaxies with samples of BL Lac
objects and quasar host galaxies, merger remnants, quiescent
elliptical galaxies, and brightest cluster galaxies drawn from the
literature. In general, the 3CR host galaxies are consistent with
luminous (~
L) elliptical galaxies. The vast majority of FR II's (~80%)
occupy the most massive ellipticals and form a homogeneous
population that is comparable to the population of radio-loud
quasar (RLQ) host galaxies in the literature. However, a
significant minority (~20%) of the 3CR FR II's appears
under-luminous with respect to quasar host galaxies. All FR II
objects in this faint tail are either unusually red, or appear to
be the brightest objects within a group. We discuss the apparent
differences between the radio galaxy and RLQ host galaxy
populations. RLQs appear to require
10
11M host galaxies (and ~10
9M black holes), whereas radio galaxies and radio-quiet quasars
can exist in galaxies down to ~3 × 10
10M. This may be due to biases in the measured quasar host
galaxy luminosities or populations studied, or due to a genuine
difference in host galaxy. If due to a genuine difference, it would
support the idea that radio and optical active galactic nuclei are
two separate populations with a significant overlap.
We present 30 GHz measurements of the angular power spectrum of
the cosmic microwave background (CMB) obtained with the
Sunyaev-Zel'dovich Array. The measurements are sensitive to
arcminute angular scales, where secondary anisotropy from the
Sunyaev-Zel'dovich effect (SZE) is expected to dominate. For a
broad bin centered at multipole 4066, we find 67
+77–50 μK
2; of which 26 ± 5 μK
2 is the expected contribution from primary CMB
anisotropy and 80 ± 54 μK
2 is the expected contribution from undetected radio
sources. These results imply an upper limit of 155 μK
2 (95% CL) on the secondary contribution to the
anisotropy in our maps. This level of SZE anisotropy power is
consistent with expectations based on recent determinations of the
normalization of the matter power spectrum, i.e., σ
8 ~ 0.8.
Recent observations of the black hole (BH)-bulge scaling
relations usually report positive redshift evolution, with higher
redshift galaxies harboring more massive BHs than expected from the
local relations. All of these studies focus on broad line quasars
with BH mass estimated from virial estimators based on single-epoch
spectra. Since the sample selection is largely based on quasar
luminosity, the cosmic scatter in the BH-bulge relation introduces
a statistical bias leading to on average more massive BHs given
galaxy properties at high redshift (i.e., the Lauer et al. bias).
We here emphasize a previously underappreciated statistical bias
resulting from the uncertainty of single-epoch virial BH mass
estimators and the shape of the underlying (true) BH mass function,
which leads to on average overestimation of the true BH masses at
the high-mass end. We demonstrate that the latter virial mass bias
can contribute a substantial amount to the observed excess in BH
mass at fixed bulge properties, comparable to the Lauer et al.
bias. The virial mass bias is independent of the Lauer et al. bias;
hence if both biases are at work, they can largely (or even fully)
account for the observed BH mass excess at high redshift.
We examine the effects of density stratification on
magnetohydrodynamic turbulence driven by the magnetorotational
instability in local simulations that adopt the shearing box
approximation. Our primary result is that, even in the absence of
explicit dissipation, the addition of vertical gravity leads to
convergence in the turbulent energy densities and stresses as the
resolution increases, contrary to results for zero net flux,
unstratified boxes. The ratio of total stress to midplane pressure
has a mean of ~0.01, although there can be significant fluctuations
on long (
50 orbits)
timescales. We find that the time-averaged stresses are largely
insensitive to both the radial and the vertical aspect ratios of
our simulation domain. For simulations with explicit dissipation,
we find that stratification extends the range of Reynolds and
magnetic Prandtl numbers for which turbulence is sustained, but the
behavior of such simulations on long timescales is highly variable.
Confirming the results of previous studies, we find oscillations in
the large-scale toroidal field with periods of ~10 orbits and
describe the dynamo process that underlies these cycles. We discuss
possible origins for the different convergence properties of the
stratified and unstratified domains and identify open questions
that remain to be answered.
Using the
Hubble Space Telescope (HST) Advanced Camera for Surveys
imaging of the GOODS North and South fields during Cycles 11, 12,
and 13, we derive empirical constraints on the delay-time
distribution function for type Ia supernovae (SNe Ia). We
extend our previous analysis to the three-year sample of 56
SNe Ia over the range 0.2 <
z < 1.8, using a Markov chain Monte Carlo to determine
the best-fit unimodal delay-time distribution function. The test,
which ultimately compares the star formation rate density history
to the unbinned volumetric SN Ia rate history from the GOODS/
HST SN survey, reveals a SN Ia delay-time distribution
that is tightly confined to 3-4 Gyr (to >95% confidence).
This result is difficult to resolve with any intrinsic delay-time
distribution function (bimodal or otherwise), in which a
substantial fraction (e.g., >10%) of events are "prompt,"
requiring less than approximately 1 Gyr to develop from
formation to explosion. The result is, however, strongly motivated
by the decline in the number of SNe Ia at
z > 1.2. Sub-samples of the
HST SN data confined to lower redshifts (
z < 1) show plausible delay-time distributions that are
dominated by prompt events, which is more consistent with results
from low-redshift supernova samples and supernova host galaxy
properties. Scenarios in which a substantial fraction of
z > 1.2 supernovae are extraordinarily obscured by dust
may partly explain the differences in low-
z and high-
z results. Other possible resolutions may include
environmental dependences (such as gas-phase metallicity) that
affect the progenitor mechanism efficiency, especially in the early
universe.