272 research outputs found
Radiation Pressure Confinement - I. Ionized Gas in the ISM of AGN Hosts
We analyze the hydrostatic effect of AGN radiation pressure on optically
thick gas in the host galaxy. We show that in luminous AGN, the radiation
pressure likely confines the ionized layer of the illuminated gas. Radiation
pressure confinement (RPC) has two main implications. First, the gas density
near the ionization front is 7x10^4 L_{i,45} r_{50}^{-2} cm^{-3}, where
L_{i,45} is the ionizing luminosity in units of 10^45 erg/s and r_{50} is the
distance of the gas from the nucleus in units of 50 pc. Second, as shown by
Dopita et al., the solution of the ionization structure within each slab is
unique, independent of the ambient pressure. We show that the RPC density vs.
distance relation is observed over a dynamical range of ~10^4 in distance, from
sub-pc to kpc from the nucleus, and a range of ~10^8 in gas density, from 10^3
to 10^11 cm^{-3}. This relation implies that the radiative force of luminous
AGN can compress giant molecular clouds in the host galaxy, and possibly affect
the star formation rate. The unique ionization structure in RPC includes a
highly ionized X-ray emitting surface, an intermediate layer which emits
coronal lines, and a lower ionization inner layer which emits optical lines.
This structure can explain the observed overlap of the extended X-ray and
optical narrow line emission in nearby AGN. We further support RPC by comparing
the predicted ratios of the narrow lines strength and narrow line widths with
available observations. We suggest a new method, based on the narrow line
widths, to estimate the black hole mass of low luminosity AGN.Comment: Accepted for publication in MNRAS. The first author will be on
regular email contact from December 201
Radiation pressure confinement - IV. Application to broad absorption line outflows
A fraction of quasars present broad absorption lines, produced by outflowing
gas with typical velocities of 3000 - 10,000 km/s. If the outflowing gas fills
a significant fraction of the volume where it resides, then it will be highly
ionized by the quasar due to its low density, and will not produce the observed
UV absorption. The suggestion that the outflow is shielded from the ionizing
radiation was excluded by recent observations. The remaining solution is a
dense outflow with a filling factor . What produces such a small
? Here we point out that radiation pressure confinement (RPC) inevitably
leads to gas compression and the formation of dense thin gas sheets/filaments,
with a large gradient in density and ionization along the line of sight. The
total column of ionized dustless gas is a few times cm,
consistent with the observed X-ray absorption and detectable P V absorption.
The predicted maximal columns of various ions show a small dependence on the
system parameters, and can be used to test the validity of RPC as a solution
for the overionization problem. The ionization structure of the outflow implies
that if the outflow is radiatively driven, then broad absorption line quasars
should have .Comment: Accepted for publication in MNRA
Radiation pressure confinement - II. Application to the broad line region in active galactic nuclei
Active galactic nuclei (AGN) are characterized by similar broad emission
lines properties at all luminosities (- erg s). What
produces this similarity over a vast range of in luminosity?
Photoionization is inevitably associated with momentum transfer to the
photoionized gas. Yet, most of the photoionized gas in the Broad Line Region
(BLR) follows Keplerian orbits, which suggests that the BLR originates from gas
with a large enough column for gravity to dominate. The photoionized surface
layer of the gas must develop a pressure gradient due to the incident radiation
force. We present solutions for the structure of such a hydrostatic
photoionized gas layer in the BLR. The gas is stratified, with a low-density
highly-ionized surface layer, a density rise inwards, and a uniform-density
cooler inner region, where the gas pressure reaches the incident radiation
pressure. This radiation pressure confinement (RPC) of the photoionized layer
leads to a universal ionization parameter in the inner photoionized
layer, independent of luminosity and distance. Thus, RPC appears to explain the
universality of the BLR properties in AGN. We present predictions for the BLR
emission per unit covering factor, as a function of distance from the ionizing
source, for a range of ionizing continuum slopes and gas metallicity. The
predicted mean strength of most lines (excluding H), and their different
average-emission radii, are consistent with the available observations.Comment: Accepted for publication in MNRAS. A paragraph was added to the
beginning of Section 2; Sections 4.3 and 4.4 were adde
Evolutionary morphology of trichomycterid catfishes: about hanging on and digging in
The catfi shes (Siluriformes) comprise a particularly diverse teleost clade, from a taxonomic, morphological, biogeographical, ecological and behavioural perspective. The Neotropical Trichomycteridae (the “parasitic” catfi shes) are emblematic of this diversity, including fi shes with some of the most specialized habits and habitats among teleosts (e. g. hematophagy, lepidophagy, miniaturization, fossorial habitats, altitudinal extremes). Relatively little information is available on general trichomycterid morphology, as most work so far has concentrated on phylogenetically informative characters, with little concern about general descriptive anatomy. In this paper we provide a synthesis of new and previously-available data in order to build a general picture of basal crown group trichomycterid morphology and of its main modifi cations. We focus on the evolutionary morphology in two relatively distal trichomycterid lineages, i. e. the hematophagous Vandelliinae and the miniature, substrate dwelling Glanapteryginae. New evidence is discussed in relation to the evolution of the opercular system as well as morphological modifi cations in miniature species exhibiting an interstitial life style
Secondary Eclipse Photometry of the Exoplanet WASP-5b with Warm Spitzer
We present secondary eclipse photometry of the extrasolar planet WASP-5b taken in the 3.6 and 4.5 μm bands with the Spitzer Space Telescope's Infrared Array Camera as part of the extended warm mission. By estimating the depth of the secondary eclipse in these two bands we can place constraints on the planet's atmospheric pressure-temperature profile and chemistry. We measure secondary eclipse depths of 0.197% ± 0.028% and 0.237% ± 0.024% in the 3.6 μm and 4.5 μm bands, respectively. For the case of a solar-composition atmosphere and chemistry in local thermal equilibrium, our observations are best matched by models showing a hot dayside and, depending on our choice of model, a weak thermal inversion or no inversion at all. We measure a mean offset from the predicted center of eclipse of 3.7 ± 1.8 minutes, corresponding to ecos ω = 0.0025 ± 0.0012 and consistent with a circular orbit. We conclude that the planet's orbit is unlikely to have been perturbed by interactions with another body in the system as claimed by Fukui et al
Complex and sustained quantum beating patterns in a classic IVR system: the 3¹5¹ Level in S₁ p-difluorobenzene
Using picosecond time-resolved photoelectron imaging we have studied the intramolecular vibrational energy redistribution (IVR) dynamics that occur following the excitation of the 3151 level which lies 2068 cm-1 above the S1 origin in p difluorobenzene. Our technique, which has superior time resolution to that of earlier studies but retains sufficient energy resolution to identify the behavior of individual vibrational states, enables us to determine six distinct beating periods in photoelectron intensity, only one of which has been observed previously. Analysis shows that the IVR dynamics are restricted among only a handful of vibrational levels, despite the relatively high excitation energy. This is deduced to be a consequence of the high symmetry and rigid structure of p-difluorobenzene
Type 1 low z AGN. I. Emission properties
We analyze the emission properties of a new sample of 3,579 type 1 AGN,
selected from the SDSS DR7 based on the detection of broad H-alpha emission.
The sample extends over a broad H-alpha luminosity L_bHa of 10^40 - 10^44 erg
s^-1 and a broad H-alpha FWHM of 1,000 - 25,000 km s^-1, which covers the range
of black hole mass 10^6<M_BH/M_Sun<10^9.5 and luminosity in Eddington units
10^-3 < L/L_Edd < 1. We combine ROSAT, GALEX and 2MASS observations to form the
SED from 2.2 mic to 2 keV. We find the following: 1. The distribution of the
H-alpha FWHM values is independent of luminosity. 2. The observed mean
optical-UV SED is well matched by a fixed shape SED of luminous quasars, which
scales linearly with L_bHa, and a host galaxy contribution. 3. The host galaxy
r-band (fibre) luminosity function follows well the luminosity function of
inactive non-emission line galaxies (NEG), consistent with a fixed fraction of
~3% of NEG hosting an AGN, regardless of the host luminosity. 4. The hosts of
lower luminosity AGN have a mean z band luminosity and u-z colour which are
identical to NEG with the same redshift distribution. With increasing L_bHa the
AGN hosts become bluer and less luminous than NEG. The implied increasing star
formation rate with L_bHa is consistent with the relation for SDSS type 2 AGN
of similar bolometric luminosity. 5. The optical-UV SED of the more luminous
AGN shows a small dispersion, consistent with dust reddening of a blue SED, as
expected for thermal thin accretion disc emission. 6. There is a rather tight
relation of nuL_nu(2 keV) and L_bHa, which provides a useful probe for
unobscured (true) type 2 AGN. 7. The primary parameter which drives the X-ray
to UV emission ratio is the luminosity, rather than M_BH or L/L_Edd.Comment: 33 pages, 23 figures; accepted for publication in MNRAS; complete
versions of tables 1 and B1 can be found at
http://physics.technion.ac.il/~stern/PaperData/Type1AGN1
Mapping the Association of Global Executive Functioning Onto Diverse Measures of Psychopathic Traits
Psychopathic individuals display a callous-coldhearted approach to interpersonal and affective situations and engage in impulsive and antisocial behaviors. Despite early conceptualizations suggesting that psychopathy is related to enhanced cognitive functioning, research examining executive functioning (EF) in psychopathy has yielded few such findings. It is possible that some psychopathic trait dimensions are more related to EF than others. Research using a 2-factor or 4-facet model of psychopathy highlights some dimension-specific differences in EF, but this research is limited in scope. Another complicating factor in teasing apart the EF–psychopathy relationship is the tendency to use different psychopathy assessments for incarcerated versus community samples. In this study, an EF battery and multiple measures of psychopathic dimensions were administered to a sample of male prisoners (N
Minor Review: An Overview of a Synthetic Nanophase Bone Substitute
Material is reviewed that consists of reconstituted collagen fibril gel mineralized in a manner that produces biomimetically sized nanoapatites intimately associated with the fibrils. This gel is formed into usable shapes with a modulus and strength that allow it to be surgically press fitted into bony defects. The design paradigm for the material is that the nanoapatites will dissolve into soluble Ca2+ as the collagen is degraded into RGD-containing peptide fragments due to osteoclastic action. This is intended to signal to the osteoclasts to continue removing the material in a biomimetic fashion similar to bony remodeling. Preliminary experiments in a subcutaneous rat model show that the material is biocompatible with respect to inflammatory and immunogenic responses, and that it supports cellular invasion. Preliminary experiments in a critical-sized mandibular defect in rats show that the material is resorbable and functions well as a bone morphogenetic 2 (BMP-2) carrier. We have produced a range of mechanical and biological responses by varying mechanical and chemical processing of the material
- …
