601 research outputs found
Space Station Freedom altitude strategy
The Space Station Freedom (SSF) altitude strategy provides guidelines and assumptions to determine an altitude profile for Freedom. The process for determining an altitude profile incorporates several factors such as where the Space Shuttle will rendezvous with the SSF, when reboosts must occur, and what atmospheric conditions exist causing decay. The altitude strategy has an influence on all areas of SSF development and mission planning. The altitude strategy directly affects the micro-gravity environment for experiments, propulsion and control system sizing, and Space Shuttle delivery manifests. Indirectly the altitude strategy influences almost every system and operation within the Space Station Program. Evolution of the SSF altitude strategy has been a very dynamic process over the past few years. Each altitude strategy in turn has emphasized a different consideration. Examples include a constant Space Shuttle rendezvous altitude for mission planning simplicity, or constant micro-gravity levels with its inherent emphasis on payloads, or lifetime altitudes to provide a safety buffer to loss of control conditions. Currently a new altitude strategy is in development. This altitude strategy will emphasize Space Shuttle delivery optimization. Since propellant is counted against Space Shuttle payload-to-orbit capacity, lowering the rendezvous altitude will not always increase the net payload-to-orbit, since more propellant would be required for reboost. This altitude strategy will also consider altitude biases to account for Space Shuttle launch slips and an unexpected worsening of atmospheric conditions. Safety concerns will define a lower operational altitude limit, while radiation levels will define upper altitude constraints. The evolution of past and current SSF altitude strategies and the development of a new altitude strategy which focuses on operational issues as opposed to design are discussed
The Distribution of Lya-Emitting Galaxies at z=2.3
We present the detection of 34 Ly-alpha emission-line galaxy candidates in a
80x80x60 co-moving Mpc region surrounding the known z=2.38 galaxy cluster
J2143-4423. The space density of Ly-alpha emitters is comparable to that found
by Steidel et al. when targeting a cluster at redshift 3.09, but is a factor of
5.8 +/- 2.5 greater than that found by field samples at similar redshifts. The
distribution of these galaxy candidates contains several 5-10 Mpc scale voids.
We compare our observations with mock catalogs derived from the VIRGO
consortium Lambda-CDM n-body simulations. Fewer than 1% of the mock catalogues
contain voids as large as we observe. Our observations thus tentatively suggest
that the galaxy distribution at redshift 2.38 contains larger voids than
predicted by current models. Three of the candidate galaxies and one previously
discovered galaxy have the large luminosities and extended morphologies of
"Ly-alpha blobs".Comment: 10 pages, 8 figures, emulateapj5, Accepted for publication in Ap
Mystery of the Lyα Blobs
We present Spitzer Space Telescope observations of the extended Lyman α blobs associated with the z=2.38 over-density J2143-4423, the largest known structure (110 Mpc) above z=2. We detect all 4 of the Lyα blobs in all four IRAC channels and we also detect 3 out of 4 of the blobs with MIPS 24μm. Conversion from rest-wavelength 7μm to total far-infrared luminosity using locally derived correlations suggests all the detected sources are in the class of ULIRGs or even Hyper-LIRGs. We find a weak correlation between Lyα and mid-infrared emission for the Lyα blobs (L_(Lyα)/L_(bol) = 0.05-0.2%). Nearly all Lyα blobs show some evidence for interaction, either in HST imaging, or the proximity of multiple MIPS sources within the Lyα cloud. This suggests that interaction or even mergers may be related to the production of Lyα blobs. Optical through infrared SEDs of the Lyα blobs do not show a clear 1.6μm bump, but rather are indicative of a composite of star formation and AGN energy sources
Ultraviolet-Bright, High-Redshift ULIRGS
We present Spitzer Space Telescope observations of the z=2.38 lya-emitter
over-density associated with galaxy cluster J2143-4423, the largest known
structure (110 Mpc) above z=2. We imaged 22 of the 37 known lya-emitters within
the filament-like structure, using the MIPS 24um band. We detected 6 of the
lya-emitters, including 3 of the 4 clouds of extended (>50 kpc) lyman alpha
emission, also known as Lya Blobs. Conversion from rest-wavelength 7um to total
far-infrared luminosity using locally derived correlations suggests all the
detected sources are in the class of ULIRGs, with some reaching Hyper-LIRG
energies. Lya blobs frequently show evidence for interaction, either in HST
imaging, or the proximity of multiple MIPS sources within the Lya cloud. This
connection suggests that interaction or even mergers may be related to the
production of Lya blobs. A connection to mergers does not in itself help
explain the origin of the Lya blobs, as most of the suggested mechanisms for
creating Lya blobs (starbursts, AGN, cooling flows) could also be associated
with galaxy interactions.Comment: 12 pages, 3 figures, accepted by ApJ Letter
Polycyclic Aromatic Hydrocarbon Emission within Lyα Blobs
We present Spitzer observations of Lyα blobs (LABs) at z = 2.38-3.09. The mid-infrared ratios (4.5 μm/8 μm and 8 μm/24 μm) indicate that ~60% of LAB infrared counterparts are cool, consistent with their infrared output being dominated by star formation and not active galactic nuclei (AGNs). The rest have a substantial hot dust component that one would expect from an AGN or an extreme starburst. Comparing the mid-infrared to submillimeter fluxes (~850 μm or rest-frame far-infrared) also indicates that a large percentage (~2/3) of the LAB counterparts have total bolometric energy output dominated by star formation, although the number of sources with submillimeter detections or meaningful upper limits remains small (~10). We obtained Infrared Spectrograph (IRS) spectra of six infrared-bright sources associated with LABs. Four of these sources have measurable polycyclic aromatic hydrocarbon (PAH) emission features, indicative of significant star formation, while the remaining two show a featureless continuum, indicative of infrared energy output completely dominated by an AGN. Two of the counterparts with PAHs are mixed sources, with PAH line-to-continuum ratios and PAH equivalent widths indicative of large energy contributions from both star formation and AGN. Most of the LAB infrared counterparts have large stellar masses, around 10^(11) M_⊙. There is a weak trend of mass upper limit with the Lyα luminosity of the host blob, particularly after the most likely AGN contaminants are removed. The range in likely energy sources for the LABs found in this and previous studies suggests that there is no single source of power that is producing all the known LABs
PAH Emission Within Lyman Alpha Blobs
We present Spitzer observations of Lya Blobs (LAB) at z=2.38-3.09. The
mid-infrared ratios (4.5/8um and 8/24um) indicate that ~60% of LAB infrared
counterparts are cool, consistent with their infrared output being dominated by
star formation and not active galactic nuclei (AGN). The rest have a
substantial hot dust component that one would expect from an AGN or an extreme
starburst. Comparing the mid-infrared to submillimeter fluxes (~850um or rest
frame far infrared) also indicates a large percentage (~2/3) of the LAB
counterparts have total bolometric energy output dominated by star formation,
although the number of sources with sub-mm detections or meaningful upper
limits remains small (~10). We obtained Infrared Spectrograph (IRS) spectra of
6 infrared-bright sources associated with LABs. Four of these sources have
measurable polycyclic aromatic hydrocarbon (PAH) emission features, indicative
of significant star formation, while the remaining two show a featureless
continuum, indicative of infrared energy output completely dominated by an AGN.
Two of the counterparts with PAHs are mixed sources, with PAH line-to-continuum
ratios and PAH equivalent widths indicative of large energy contributions from
both star formation and AGN. Most of the LAB infrared counterparts have large
stellar masses, around 10^11 Mo. There is a weak trend of mass upper limit with
the Lya luminosity of the host blob, particularly after the most likely AGN
contaminants are removed. The range in likely energy sources for the LABs found
in this and previous studies suggests that there is no single source of power
that is producing all the known LABs.Comment: 34 pages, 5 figures, accepted by Ap
Galaxy Morphology from NICMOS Parallel Imaging
We present high resolution NICMOS images of random fields obtained in
parallel to other HST observations. We present galaxy number counts reaching
H=24. The H-band galaxy counts show good agreement with the deepest I- and
K-band counts obtained from ground-based data. We present the distribution of
galaxies with morphological type to H<23. We find relatively fewer irregular
galaxies compared to an I-band sample from the Hubble Deep Field, which we
attribute to their blue color, rather than to morphological K-corrections. We
conclude that the irregulars are intrinsically faint blue galaxies at z<1.Comment: 13 pages, including 4 figures. Accepted for publication in ApJ
Letter
Competition Between Gravitational and Scalar Field Radiation
Recent astrophysical observations have provided strong evidence that the
present expansion of the universe is accelerating, powered by the energy
density associated with a cosmological term. Assuming the latter to be not
simply a constant term but a "quintessence" field, we study the radiation of
quanta of such a "quintessence" field ("quintons") by binary systems of
different types and compare intensities to those of standard tensor
gravitational wave emission. We consider both the case in which the
quintessence field varies only over cosmological distances and the case in
which it is modified spatially by (strong) gravitational fields, a condition
that results in bounds on the gradient of the scalar field. We show that, in
both the first case and, because of a bound we derive from the Hulse-Taylor
pulsar, in the second, there is not sufficient quinton radiation to affect
expected LISA and LIGO gravity wave signals from binary systems. We show that,
in the second case, the Large Hadron Collider is capable of setting a bound
similar to that from the binary pulsar.Comment: 12 pages aastex, accepted for publication in the Astrophysical
Journal. Minor typographical errors and reference list correcte
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