2,483 research outputs found
Minimum fuel attitude control of a nonlinear satellite system with bounded control by a method based on linear programming
Optimal control method based on linear programming for satellite fuel consumptio
Minimum time control of a nonlinear system
Time-optimal control problem studied for system representing second-order nonlinear differential equatio
Role of Galaxy Mergers in Cosmic Star Formation History
We present a morphology study of intermediate-redshift (0.2<z<1.2) luminous
infrared galaxies (LIRGs) and general field galaxies in the GOODS fields using
a revised asymmetry measurement method optimized for deep fields. By taking
careful account of the importance of the underlying sky-background structures,
our new method does not suffer from systematic bias and offers small
uncertainties. By redshifting local LIRGs and low-redshift GOODS galaxies to
different higher redshifts, we have found that the redshift dependence of the
galaxy asymmetry due to surface-brightness dimming is a function of the
asymmetry itself, with larger corrections for more asymmetric objects. By
applying redshift-, IR-luminosity- and optical-brightness-dependent asymmetry
corrections, we have found that intermediate-redshift LIRGs generally show
highly asymmetric morphologies, with implied merger fractions ~50% up to z=1.2,
although they are slightly more symmetric than local LIRGs. For general field
galaxies, we find an almost constant relatively high merger fraction (20-30%).
The B-band LFs of galaxy mergers are derived at different redshifts up to z=1.2
and confirm the weak evolution of the merger fraction after breaking the
luminosity-density degeneracy. The IR luminosity functions (LFs) of galaxy
mergers are also derived, indicating a larger merger fraction at higher IR
luminosity. The integral of the merger IR LFs indicates a dramatic evolution of
the merger-induced IR energy density [(1+z)^(5-6)}], and that galaxy mergers
start to dominate the cosmic IR energy density at z>~1.Comment: Accepted for publication in ApJ, 25 pages, 23 figures (2 colors). The
high-resolution pdf is at
http://cztsy.as.arizona.edu/~yong/Research/SHI_MERGER.pd
Quantified HI Morphology V: HI Disks in the Virgo Cluster
We explore the quantified morphology of atomic hydrogen (HI) disks in the
Virgo cluster. These galaxies display a wealth of phenomena in their Hi
morphology, e.g., tails, truncation and warps. These morphological disturbances
are related to the ram-pressure stripping and tidal interaction that galaxies
undergo in this dense cluster environment. To quantify the morphological
transformation of the HI disks, we compute the morphological parameters of CAS,
Gini, and M20 and our own GM for 51 galaxies in 48 HI column density maps from
the VIVA project. Some morphological phenomena can be identified in this space
of relatively low resolution HI data. Truncation of the HI disk can be cleanly
identified via the Concentration parameter (C<1) and Concentration can also be
used to identify HI deficient disks (1<C<5). Tidal interaction is typically
identified using combinations of these morphological parameters, applied to
(optical) images of galaxies. We find that some selection criteria (Gini-M20,
Asymmetry, and a modified Concentration-M20) are still applicable for the
coarse (~15" FWHM) VIVA HI data. The phenomena of tidal tails can be reasonably
well identified using the Gini-M20 criterion (60% of galaxies with tails
identified but with as many contaminants). Ram-pressure does move HI disks into
and out of most of our interaction criteria: the ram-pressure sequence
identified by Vollmer et al. (2009) tracks into and out of some of these
criteria (Asymmetry based and the Gini-M20 selections, but not the
Concentration-M20 or the GM based ones). Therefore, future searches for
interaction using HI morphologies should take ram-pressure into account as a
mechanism to disturb HI disks enough to make them appear as gravitationally
interacting. One mechanism would be to remove all the HI deficient (C<5) disks
from the sample, as these have undergone more than one HI removal mechanism.Comment: 10 pages, 3 figures, accepted by MNRAS, appendixes not include
Quantified HI Morphology III: Merger Visibility Times from HI in Galaxy Simulations
Major mergers of disk galaxies are thought to be a substantial driver in
galaxy evolution. To trace the fraction and the rate galaxies are in mergers
over cosmic times, several observational techniques, including morphological
selection criteria, have been developed over the last decade. We apply this
morphological selection of mergers to 21 cm radio emission line (HI) column
density images of spiral galaxies in nearby surveys. In this paper, we
investigate how long a 1:1 merger is visible in HI from N-body simulations. We
evaluate the merger visibility times for selection criteria based on four
parameters: Concentration, Asymmetry, M20, and the Gini parameter of second
order moment of the flux distribution (GM). Of three selection criteria used in
the literature, one based on Concentration and M20 works well for the HI
perspective with a merger time scale of 0.4 Gyr. Of the three selection
criteria defined in our previous paper, the GM performs well and cleanly
selects mergers for 0.69 Gyr. The other two criteria (A-M20 and C-M20), select
isolated disks as well, but perform best for face-on, gas-rich disks (T(merger)
~ 1 Gyr). The different visibility scales can be combined with the selected
fractions of galaxies in any large HI survey to obtain merger rates in the
nearby Universe. All-sky surveys such as WALLABY with ASKAP and the Medium Deep
Survey with the APETIF instrument on Westerbork are set to revolutionize our
perspective on neutral hydrogen and will provide an accurate measure of the
merger fraction and rate of the present epoch.Comment: 12 pages, 6 figures, 4 tables, accepted by MNRAS, appendix not
include
Quantified HI Morphology I: Multi-Wavelengths Analysis of the THINGS Galaxies
Galaxy evolution is driven to a large extent by interactions and mergers with
other galaxies and the gas in galaxies is extremely sensitive to the
interactions. One method to measure such interactions uses the quantified
morphology of galaxy images. Well-established parameters are Concentration,
Asymmetry, Smoothness, Gini, and M20 of a galaxy image. Thus far, the
application of this technique has mostly been restricted to restframe
ultra-violet and optical images. However, with the new radio observatories
being commissioned (MeerKAT, ASKAP, EVLA, WSRT/APERTIF, and ultimately SKA), a
new window on the neutral atomic hydrogen gas (HI) morphology of a large
numbers of galaxies will open up. The quantified morphology of gas disks of
spirals can be an alternative indicator of the level and frequency of
interaction. The HI in galaxies is typically spatially more extended and more
sensitive to low-mass or weak interactions. In this paper, we explore six
morphological parameters calculated over the extent of the stellar (optical)
disk and the extent of the gas disk for a range of wavelengths spanning UV,
Optical, Near- and Far-Infrared and 21 cm (HI) of 28 galaxies from The HI
Nearby Galaxy Survey (THINGS). Though the THINGS sample is small and contains
only a single ongoing interaction, it spans both non-interacting and
post-interacting galaxies with a wealth of multi-wavelength data. We find that
the choice of area for the computation of the morphological parameters is less
of an issue than the wavelength at which they are measured. The signal of
interaction is as good in the HI as in any of the other wavelengths in which
morphology has been used to trace the interaction rate to date, mostly
star-formation dominated ones (near- and far-ultraviolet). The Asymmetry and
M20 parameters are the ones which show the most promise as tracers of
interaction in 21 cm line observations.Comment: 16 pages, 11 figure, table 1, accepted by MNRAS, appendix not
include
The Colors of Dwarf Elliptical Galaxy Globular Cluster Systems, Nuclei and Stellar Halos
We present the results of a Hubble Space Telescope WFPC2 F555W and F814W
survey of 69 dwarf elliptical galaxies (dEs) in the Virgo and Fornax Clusters
and Leo Group. The colors of the dE globular clusters, nuclei, and
underlying field star populations are used to trace the dE star-formation
histories. We find that the dE globular cluster candidates are as blue as the
metal-poor globular clusters of the Milky Way. The observed correlation of the
dE globular cluster systems' color with the luminosity of the host dE is
strong evidence that the globular clusters were formed within the the halos of
dEs and do not have a pre-galactic origin. Assuming the majority of dE clusters
are old, the mean globular cluster color- host galaxy luminosity correlation
implies a cluster metallicity galaxy luminosity relation of , which is significantly shallower than the field star
metallicity - host galaxy luminosity relationship observed in Local Group
dwarfs (). The dE stellar envelopes are
magnitudes redder in than their globular clusters and nuclei. This color
offset implies separate star-formation episodes within the dEs for the clusters
and field stars, while the very blue colors of two dE nuclei trace a third
star-formation event in those dEs less than a Gyr ago.Comment: 39 pages, including 5 tables and 10 figures; accepted by the
Astrophysical Journa
Investigating evidence for different black hole accretion modes since redshift z~1
Chandra data in the COSMOS, AEGIS-XD and 4Ms CDFS are combined with
optical/near-IR photometry to determine the rest-frame U-V vs V-J colours of
X-ray AGN hosts at mean redshifts 0.40 and 0.85. This combination of colours
(UVJ) provides an efficient means of separating quiescent from star-forming,
including dust reddened, galaxies. Morphological information emphasises
differences between AGN split by their UVJ colours. AGN in quiescent galaxies
are dominated by spheroids, while star-forming hosts are split between bulges
and disks. The UVJ diagram of AGN hosts is then used to set limits on the
accretion density associated with evolved and star-forming systems. Most of the
black hole growth since z~1 is associated with star-forming hosts.
Nevertheless, ~15-20% of the X-ray luminosity density since z~1, is taking
place in the quiescent region of the UVJ diagram. For the z~0.40 subsample,
there is tentative evidence (2sigma significance), that AGN split by their UVJ
colours differ in Eddington ratio. AGN in star-forming hosts dominate at high
Eddington ratios, while AGN in quiescent hosts become increasingly important as
a fraction of the total population toward low Eddington ratios. At higher
redshift, z~0.8, such differences are significant at the 2sigma level only at
Eddington ratios >1e-3. These findings are consistent with scenarios in which
diverse accretion modes are responsible for the build-up of SMBHs at the
centres of galaxies. We compare our results with the GALFORM semi-analytic
model, which postulates two black hole fuelling modes, the first linked to
star-formation and the second occuring in passive galaxies. GALFORM predicts a
larger fraction of black hole growth in quiescent galaxies at z<1, compared to
the data. Relaxing the strong assumption of the model that passive AGN hosts
have zero star-formation rate could reconcile this disagreement.Comment: MNRAS accepte
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