216 research outputs found
AT 2023prq: A Classical Nova in the Halo of the Andromeda Galaxy
The classical nova, AT 2023prq, was discovered on 2023 August 15 and is
located at a distance of 46 kpc from the Andromeda Galaxy (M 31). Here we
report photometry and spectroscopy of the nova. The 'very fast'
( d) and low luminosity ()
nature of the transient along with the helium in its spectra would indicate
that AT 2023prq is a 'faint-and-fast' He/N nova. Additionally, at such a large
distance from the centre of M 31, AT 2023prq is a member of the halo nova
population.Comment: 3 pages, 1 figure; Published in Research Notes of the American
Astronomical Societ
Gamma-ray Bursts, Classified Physically
From Galactic binary sources, to extragalactic magnetized neutron stars, to
long-duration GRBs without associated supernovae, the types of sources we now
believe capable of producing bursts of gamma-rays continues to grow apace. With
this emergent diversity comes the recognition that the traditional (and newly
formulated) high-energy observables used for identifying sub-classes does not
provide an adequate one-to-one mapping to progenitors. The popular
classification of some > 100 sec duration GRBs as ``short bursts'' is not only
an unpalatable retronym and syntactically oxymoronic but highlights the
difficultly of using what was once a purely phenomenological classification to
encode our understanding of the physics that gives rise to the events. Here we
propose a physically based classification scheme designed to coexist with the
phenomenological system already in place and argue for its utility and
necessity.Comment: 6 pages, 3 figures. Slightly expanded version of solicited paper to
be published in the Proceedings of ''Gamma Ray Bursts 2007,'' Santa Fe, New
Mexico, November 5-9. Edited by E. E. Fenimore, M. Galassi, D. Palme
Late-time VLA reobservations rule out ULIRG-like host galaxies for most pre-Swift long-duration gamma-ray bursts
We present new Jansky Very Large Array observations of five pre-Swift gamma-ray bursts for which an ultraluminous [star formation rate (SFR) > 100 M⊙; yr-1] dusty host galaxy had previously been inferred from radio or submillimetre observations taken within a few years after the burst. In four of the five cases, we no longer detect any source at the host location to limits much fainter than the original observations, ruling out the existence of an ultraluminous galaxy hosting any of these gamma-ray bursts (GRBs). We continue to detect a source at the position of GRB 980703, but it is much fainter than it was a decade ago and the inferred radio SFR (~80M⊙) is relatively modest. The radio flattening at 200-1000 d observed in the light curve of this GRB may have been caused by a decelerating counterjet oriented 180 deg away from the viewer, although an unjetted wind model can also explain the data. Our results eliminate all well-established ultraluminous infrared galaxies (ULIRGs) among the pre-Swift host population. They also rule out all cases for which an unobscured GRB was found in a galaxy dominated by heavily obscured star formation. When GRBs do occur in ULIRGs, the afterglow is almost always observed to be heavily obscured, consistent with the large dust opacities and high dust covering fractions characteristic of these systems. © 2016 The Authors
Radio Properties of z>4 Optically-Selected Quasars
We report on two programs to address differential evolution between the
radio-loud and radio-quiet quasar populations at high (z>4) redshift. Both
programs entail studying the radio properties of optically-selected quasars.
First, we have observed 32 optically-selected, high-redshift (z>4) quasars with
the VLA at 6 cm (5 GHz). These sources comprise a statistically complete and
well-understood sample. We detect four quasars above our 3-sigma limit of ~0.15
mJy, which is sufficiently sensitive to detect all radio-loud quasars at the
probed redshift range. Second, we have correlated 134 z>4 quasars, comprising
all such sources that we are aware of as of mid-1999, with FIRST and NVSS.
These two recent 1.4 GHz VLA sky surveys reach 3-sigma limits of approximately
0.6 mJy and 1.4 mJy respectively. We identify a total of 15 z>4 quasars, of
which six were not previously known to be radio-loud. The depth of these
surveys does not reach the radio-loud/radio-quiet demarcation luminosity
density (L(1.4 GHz) = 10^32.5 h(50)^(-2) ergs/s/Hz) at the redshift range
considered; this correlation therefore only provides a lower limit to the
radio-loud fraction of quasars at high-redshift. The two programs together
identify eight new radio-loud quasars at z>4, a significant increase over the
seven currently in the published literature. We find no evidence for radio-loud
fraction depending on optical luminosity for -25 > M_B > -28 at z~2, or for
-26>M_B>-28 at z>4. Our results also show no evolution in the radio-loud
fraction between z~2 and z>4 (-26>M_B>-28).Comment: 19 pages, 7 figures; to appear in The Astronomical Journal (April
2000
Late time HST UV and optical observations of AT~2018cow: extracting a cow from its background
The bright, blue, rapidly evolving AT2018cow is a well-studied peculiar
extragalactic transient. Despite an abundance of multi-wavelength data, there
still is no consensus on the nature of the event. We present our analysis of
three epochs of Hubble Space Telescope (HST) observations spanning the period
from 713-1474 days post burst, paying particular attention to uncertainties of
the transient photometry introduced by the complex background in which
AT2018cow resides. Photometric measurements show evident fading in the UV and
more subtle but significant fading in the optical. During the last HST
observation, the transient's optical/UV colours were still bluer than those of
the substantial population of compact, young, star-forming regions in the host
of AT2018cow, suggesting some continued transient contribution to the light.
However, a compact source underlying the transient would substantially modify
the resulting spectral energy distribution, depending on its contribution in
the various bands. In particular, in the optical filters, the complex, diffuse
background poses a problem for precise photometry. An underlying cluster is
expected for a supernova occurring within a young stellar environment or a
tidal-disruption event (TDE) within a dense older one. While many recent works
have focused on the supernova interpretation, we note the substantial
similarity in UV light-curve morphology between AT2018cow and several tidal
disruption events around supermassive black holes. Assuming AT2018cow arises
from a TDE-like event, we fit the late-time emission with a disc model and find
M. Further observations are necessary to
determine the late-time evolution of the transient and its immediate
environment.Comment: 16 pages, 10 figures. Accepted for publication in MNRA
Type II supernova energetics and comparison of light curves to shock-cooling models
During the first few days after explosion, Type II supernovae (SNe) are dominated by relatively simple physics. Theoretical predictions regarding early-time SN light curves in the ultraviolet (UV) and optical bands are thus quite robust. We present, for the first time, a sample of 57 R-band Type II SN light curves that are well monitored during their rise, having > 5 detections during the first 10 days after discovery, and a well-constrained time of explosion to within 1-3 days. We show that
the energy per unit mass (E/M) can be deduced to roughly a factor of five by comparing early-time optical data to the model of Rabinak & Waxman (2011), while the progenitor radius cannot be determined based on R-band data alone. We find that Type II SN explosion energies span a range of
E/M = (0.2-20)x10^(51) erg/(10 M_☉), and have a mean energy per unit mass of 〈E/M〉 = 0.85x10^(51)erg/(10 M_☉), corrected for Malmquist bias. Assuming a small spread in progenitor masses, this indicates a large intrinsic diversity in explosion energy. Moreover, E/M is positively correlated with the amount of ^(56)Ni produced in the explosion, as predicted by some recent models of core-collapse SNe. We further present several empirical correlations. The peak magnitude is correlated with the
decline rate (Δm_(15)), the decline rate is weakly correlated with the rise time, and the rise time is not
significantly correlated with the peak magnitude. Faster declining SNe are more luminous and have longer rise times. This limits the possible power sources for such events
SubmilliJansky Transients in Archival Radio Observations
[ABRIDGED] We report the results of a 944-epoch survey for transient sources
with archival data from the Very Large Array spanning 22 years with a typical
epoch separation of 7 days. Observations were obtained at 5 or 8.4 GHz for a
single field of view with a full-width at half-maximum of 8.6' and 5.1',
respectively, and achieved a typical point-source detection threshold at the
beam center of ~300 microJy per epoch. Ten transient sources were detected with
a significance threshold such that only one false positive would be expected.
Of these transients, eight were detected in only a single epoch. Two transients
were too faint to be detected in individual epochs but were detected in
two-month averages. None of the ten transients was detected in longer-term
averages or associated with persistent emission in the deep image produced from
the combination of all epochs. The cumulative rate for the short timescale
radio transients above 370 microJy at 5 and 8.4 GHz is 0.07 < R < 40 deg^-2
yr^-1, where the uncertainty is due to the unknown duration of the transients,
20 min < t_char < 7 days. A two-epoch survey for transients will detect 1.5 +/-
0.4 transient per square degrees above a flux density of 370 microJy. Two
transients are associated with galaxies at z=0.040 and z=0.249. These may be
similar to the peculiar Type Ib/c radio supernova SN 1998bw associated with GRB
980428. Six transients have no counterparts in the optical or infrared (R=27,
Ks=18). The hosts and progenitors of these transients are unknown.Comment: Accepted for ApJ; full quality figures available at
http://astro.berkeley.edu/~gbower/ps/rt.pd
Keck and ESO-VLT View of the Symmetry of the Ejecta of the XRF/SN 2006aj
Nebular-phase spectra of SN 2006aj, which was discovered in coincidence with
X-ray flash 060218, were obtained with Keck in 2006 July and the Very Large
Telescope in 2006 September. At the latter epoch spectropolarimetry was also
attempted, yielding an upper limit of ~ 2% for the polarization. The spectra
show strong emission lines of [OI] and MgI], as expected from a Type Ic
supernova, but weak CaII lines. The [FeII] lines that were strong in the
spectra of SN 1998bw are much weaker in SN 2006aj, consistent with the lower
luminosity of this SN. The outer velocity of the line-emitting ejecta is ~ 8000
km/s in July and ~ 7400 km/s in September, consistent with the relatively low
kinetic energy of expansion of SN 2006aj. All emission lines have similar
width, and the profiles are symmetric, indicating that no major asymmetries are
present in the ejecta at the velocities sampled by the nebular lines (v < 8000
km/s), except perhaps in the innermost part. The spectra were modelled with a
non-LTE code. The mass of 56Ni required to power the emission spectrum is ~
0.20 Msun, in excellent agreement with the results of early light curve
modelling. The oxygen mass is ~ 1.5 Msun, again much less than in SN 1998bw but
larger by ~ 0.7 Msun than the value derived from the early-time modelling. The
total ejected mass is ~ 2 Msun below 8000 km/s. This confirms that SN 2006aj
was only slightly more massive and energetic than the prototypical Type Ic SN
1994I, but also indicates the presence of a dense inner core, containing ~ 1
Msun of mostly oxygen and carbon. The presence of such a core is inferred for
all broad-lined SNe Ic. This core may have the form of an equatorial
oxygen-dominated region, but it is too deep to affect the early light curve and
too small to affect the late polarization spectrum.Comment: 20 pages, 6 figures. Accepted for publication in the Astrophysical
Journa
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