104 research outputs found
Processing and Transmission of Information
Contains reports on four research projects.National Aeronautics and Space Administration (Grant NGL 22-009-013
Multi-Wavelength Properties of the Type IIb SN 2008ax
We present the UV, optical, X-ray, and radio properties of the Type IIb SN
2008ax discovered in NGC 4490. The observations in the UV are one of the
earliest of a Type IIb supernova (SN). On approximately day four after the
explosion, a dramatic upturn in the u and uvw1 (lambda_c = 2600 Angstroms)
light curves occurred after an initial rapid decline which is attributed to
adiabatic cooling after the initial shock breakout. This rapid decline and
upturn is reminiscent of the Type IIb SN 1993J on day six after the explosion.
Optical/near-IR spectra taken around the peak reveal prominent H-alpha, HeI,
and CaII absorption lines. A fading X-ray source is also located at the
position of SN 2008ax, implying an interaction of the SN shock with the
surrounding circumstellar material and a mass-loss rate of the progenitor of
M_dot = (9+/-3)x10^-6 solar masses per year. The unusual time evolution (14
days) of the 6 cm peak radio luminosity provides further evidence that the
mass-loss rate is low. Combining the UV, optical, X-ray, and radio data with
models of helium exploding stars implies the progenitor of SN 2008ax was an
unmixed star in an interacting-binary. Modeling of the SN light curve suggests
a kinetic energy (E_k) of 0.5x10^51 ergs, an ejecta mass (M_ej) of 2.9 solar
masses, and a nickel mass (M_Ni) of 0.06 solar masses.Comment: Accepted to ApJ Letters, 14 pages, 3 figures, 2 table
The Sparsest Clusters With O Stars
There is much debate on how high-mass star formation varies with environment,
and whether the sparsest star-forming environments are capable of forming
massive stars. To address this issue, we have observed eight apparently
isolated OB stars in the SMC using HST's Advanced Camera for Surveys. Five of
these objects appear as isolated stars, two of which are confirmed to be
runaways. The remaining three objects are found to exist in sparse clusters,
with <10 companion stars revealed, having masses of 1-4 solar mass. Stochastic
effects dominate in these sparse clusters, so we perform Monte Carlo
simulations to explore how our observations fit within the framework of
empirical, galactic cluster properties. We generate clusters using a simplistic
-2 power-law distribution for either the number of stars per cluster (N_*) or
cluster mass (M_cl). These clusters are then populated with stars randomly
chosen from a Kroupa IMF. We find that simulations with cluster lower-mass
limits of M_cl,lo >20 solar mass and N_*,lo >40 match best with observations of
SMC and Galactic OB star populations. We examine the mass ratio of the
second-most massive and most massive stars (m_max,2/m_max), finding that our
observations all exist below the 20th percentile of our simulated clusters.
However, all of our observed clusters lie within the parameter space spanned by
the simulated clusters, although some are in the lowest 5th percentile
frequency. These results suggest that clusters are built stochastically by
randomly sampling stars from a universal IMF with a fixed stellar upper-mass
limit. In particular, we see no evidence to suggest a m_max - M_cl relation.
Our results may be more consistent with core accretion models of star formation
than with competitive accretion models, and they are inconsistent with the
proposed steepening of the integrated galaxy IMF (IGIMF).Comment: 19 pages, 12 figures, accepted for publication in Ap
Implications of a non-universal IMF from C, N, and O abundances in very metal-poor Galactic stars and damped Lyman-alpha absorbers
Recently revealed C, N, and O abundances in the most metal-poor damped
Lyman-alpha (DLA) absorbers are compared with those of extremely metal-poor
stars in the Galactic halo, as well as extragalactic H II regions, to decipher
nucleosynthesis and chemical enrichment in the early Universe. These
comparisons surprisingly identify a relatively high C/O ratio and a low N/O
ratio in DLA systems, which is hard to explain theoretically. We propose that
if these features are confirmed by future studies, this effect occurs because
the initial mass function in metal-poor DLA systems has a cut-off at the upper
mass end at around 20-25 Msun, thus lacks the massive stars that provide the
nucleosynthesis products leading to the low C/O and high N/O ratios. This
finding is a reasonable explanation of the nature of DLA systems in which a
sufficient amount of cold H I gas remains intact because of the suppression of
ionization by massive stars. In addition, our claim strongly supports a high
production rate of N in very massive stars, which might be acceptable in light
of the recent nucleosynthesis calculations with fast rotation models. The
updates of both abundance data and nucleosynthesis results will strengthen our
novel proposition that the C/O and N/O abundances are a powerful tool for
inferring the form of the initial mass function.Comment: 9 pages including 5 figures, accepted for publication in A&
UV+IR Star Formation Rates: Hickson Compact Groups with Swift and Spitzer
We present Swift UVOT (1600-3000A) 3-band photometry for 41 galaxies in 11
nearby (<4500km/s) Hickson Compact Groups (HCGs) of galaxies. We use the
uvw2-band (2000A) to estimate the dust-unobscured component, SFR_UV, of the
total star-formation rate, SFR_T. We use Spitzer MIPS 24-micron photometry to
estimate SFR_IR, the dust-obscured component of SFR_T. We obtain
SFR_T=SFR_UV+SFR_IR. Using 2MASS K_s band based stellar mass, M*, estimates, we
calculate specific SFRs, SSFR=SFR_T/M*. SSFR values show a clear and
significant bimodality, with a gap between low (<~3.2x10^-11 / yr) and high
SSFR (>~1.2x10^-10 / yr) systems. All galaxies with MIR activity index a_IRAC
0) are in the high- (low-) SSFR locus, as expected if high levels of
star-formation power MIR emission from polycyclic aromatic hydrocarbon
molecules and a hot dust continuum. All elliptical/S0 galaxies are in the
low-SSFR locus, while 22 out of 24 spirals/irregulars are in the high-SSFR
locus, with two borderline cases. We divide our sample into three subsamples
(I, II and III) according to decreasing HI-richness of the parent galaxy group
to which a galaxy belongs. Consistent with the SSFR and a_IRAC bimodality, 12
out of 15 type-I (11 out of 12 type-III) galaxies are in the high- (low-) SSFR
locus, while type II galaxies span almost the full range of SSFR values. Unlike
HCG galaxies, galaxies in a comparison quiescent SINGS sub-sample are
continuously distributed both in SSFR and a_IRAC. Any uncertainties can only
further enhance the SSFR bimodality. These results suggest that an environment
characterized by high galaxy number-densities and low galaxy
velocity-dispersions, such as the one found in compact groups, plays a key role
in accelerating galaxy evolution by enhancing star-formation processes in
galaxies and favoring a fast transition to quiescence.(abridged)Comment: Accepted by ApJ. [8 Tables, 16 Figures. Color figures have reduced
size for ArXiv - emulateapj v. 2/16/10
Paper II: Calibration of the Swift ultraviolet/optical telescope
The Ultraviolet/Optical Telescope (UVOT) is one of three instruments onboard
the Swift observatory. The photometric calibration has been published, and this
paper follows up with details on other aspects of the calibration including a
measurement of the point spread function with an assessment of the orbital
variation and the effect on photometry. A correction for large scale variations
in sensitivity over the field of view is described, as well as a model of the
coincidence loss which is used to assess the coincidence correction in extended
regions. We have provided a correction for the detector distortion and measured
the resulting internal astrometric accuracy of the UVOT, also giving the
absolute accuracy with respect to the International Celestial Reference System.
We have compiled statistics on the background count rates, and discuss the
sources of the background, including instrumental scattered light. In each case
we describe any impact on UVOT measurements, whether any correction is applied
in the standard pipeline data processing or whether further steps are
recommended.Comment: Accepted for publication in MNRAS. 15 pages, 21 figures, 4 table
Two years of monitoring Supergiant Fast X-ray Transients with Swift
We present two years of intense Swift monitoring of three SFXTs, IGR
J16479-4514, XTE J1739-302, and IGR J17544-2619 (since October 2007).
Out-of-outburst intensity-based X-ray (0.3-10keV) spectroscopy yields absorbed
power laws with by hard photon indices (G~1-2). Their outburst broad-band
(0.3-150 keV) spectra can be fit well with models typically used to describe
the X-ray emission from accreting NSs in HMXBs. We assess how long each source
spends in each state using a systematic monitoring with a sensitive instrument.
These sources spend 3-5% of the total in bright outbursts. The most probable
flux is 1-2E-11 erg cm^{-2} s^{-1} (2-10 keV, unabsorbed), corresponding to
luminosities in the order of a few 10^{33} to 10^{34} erg s^{-1} (two orders of
magnitude lower than the bright outbursts). The duty-cycle of inactivity is 19,
39, 55%, for IGR J16479-4514, XTE J1739-302, and IGR J17544-2619, respectively.
We present a complete list of BAT on-board detections further confirming the
continued activity of these sources. This demonstrates that true quiescence is
a rare state, and that these transients accrete matter throughout their life at
different rates. X-ray variability is observed at all timescales and
intensities we can probe. Superimposed on the day-to-day variability is
intra-day flaring which involves variations up to one order of magnitude that
can occur down to timescales as short as ~1ks, and whichcan be explained by the
accretion of single clumps composing the donor wind with masses
M_cl~0.3-2x10^{19} g. (Abridged)Comment: Accepted for publication in MNRAS. 17 pages, 11 figures, 8 table
The origin of the early time optical emission of Swift GRB 080310
We present broadband multi-wavelength observations of GRB 080310 at redshift
z = 2.43. This burst was bright and long-lived, and unusual in having extensive
optical and near IR follow-up during the prompt phase. Using these data we
attempt to simultaneously model the gamma-ray, X-ray, optical and IR emission
using a series of prompt pulses and an afterglow component. Initial attempts to
extrapolate the high energy model directly to lower energies for each pulse
reveal that a spectral break is required between the optical regime and 0.3 keV
to avoid over predicting the optical flux. We demonstrate that afterglow
emission alone is insufficient to describe all morphology seen in the optical
and IR data. Allowing the prompt component to dominate the early-time optical
and IR and permitting each pulse to have an independent low energy spectral
indices we produce an alternative scenario which better describes the optical
light curve. This, however, does not describe the spectral shape of GRB 080310
at early times. The fit statistics for the prompt and afterglow dominated
models are nearly identical making it difficult to favour either. However one
enduring result is that both models require a low energy spectral index
consistent with self absorption for at least some of the pulses identified in
the high energy emission model.Comment: 24 pages, 12 figures, 12 tables. Accepted to MNRA
Antideuteron yield at the AGS and coalescence implications
We present Experiment 864's measurement of invariant antideuteron yields in
11.5A GeV/c Au + Pt collisions. The analysis includes 250 million triggers
representing 14 billion 10% central interactions sampled for events with high
mass candidates. We find (1/2 pi pt) d^(2)N/dydpt = 3.5 +/- 1.5 (stat.)
+0.9,-0.5 (sys.) x 10^(-8) GeV^(-2)c^(2) for 1.8=0.35 GeV/c
(y(cm)=1.6) and 3.7 +/- 2.7 (stat.) +1.4,-1.5 (sys.) x 10^(-8) GeV^(-2)c^(2)
for 1.4=0.26 GeV/c, and a coalescence parameter B2-bar of 4.1 +/-
2.9 (stat.) +2.3,-2.4 (sys.) x 10^(-3) GeV^(2)c^(-3). Implications for the
coalescence model and antimatter annihilation are discussed.Comment: 8 pages, 4 figures, Latex, submitted to Phys. Rev. Let
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