5,136 research outputs found
Evaluating the Effects of a Brief Assertiveness and Help Seeking Skill Intervention
Children in foster care lead their lives at an increased risk for mental health issues that are often complicated by the unstable and unpredictable nature of their living arrangements and interpersonal relationships. As such, there is substantial need to examine brief therapies and interventions for use with children in foster care and children who have experienced similar trauma and instability. Mental health care providers for children in foster care often may not have sufficient periods of time to implement treatment with fidelity. The present study investigated the efficacy of a summer camp based, brief behavioral intervention targeting help-seeking behavior and assertiveness to create meaningful skill improvement in a sample of children in foster care. Three, 30-min group sessions of a targeted assertiveness skill intervention were conducted on a sample of 13 children in foster care between the ages of 6 and 12 and compared to an assessment only control. Measures of general assertiveness, emotions towards seeking help, and assertiveness skill related to asking for help were used in a pretest-posttest format to assess the efficacy of the intervention. Results showed that participants in the intervention condition significantly improved on measures of general assertiveness and assertiveness skill, though not on the measure of emotions towards situations in which they would use these skills. These findings support the use of a brief intervention to teach assertive communication and help-seeking skill. Limitations and future directions are discussed
The evolutionary time scale of Sakurai's object: A test of convection theory?
Sakurai's object (V4334 Sgr) is a born again AGB star following a very late
thermal pulse. So far no stellar evolution models have been able to explain the
extremely fast evolution of this star, which has taken it from the pre-white
dwarf stage to its current appearance as a giant within only a few years. A
very high stellar mass can be ruled out as the cause of the fast evolution.
Instead the evolution time scale is reproduced in stellar models by making the
assumption that the efficiency for element mixing in the He-flash convection
zone during the very late thermal pulse is smaller than predicted by the
mixing-length theory. As a result the main energy generation from fast proton
capture occurs closer to the surface and the expansion to the giant state is
accelerated to a few years. Assuming a mass of V4334 Sgr of 0.604Msun -- which
is consistent with a distance of 4kpc -- a reduction of the mixing length
theory mixing efficiency by a factor of ~ 100 is required to match its
evolutionary time scale. This value decreases if V4334 Sgr has a smaller mass
and accordingly a smaller distance. However, the effect does not disappear for
the smallest possible masses. These findings may present a semi-empirical
constraint on the element mixing in convective zones of the stellar interior.Comment: 16 pages, 3 figures, ApJ Letter, in press; some additional
information as well as modifications as a result of the refereeing process,
improved layout of prev. Fig.1 (now Fig.1 and Fig.2
The Circumstellar Extinction of Planetary Nebulae
We analyze the dependence of circumstellar extinction on core mass for the
brightest planetary nebulae (PNe) in the Magellanic Clouds and M31. We show
that in all three galaxies, a statistically significant correlation exists
between the two quantities, such that high core mass objects have greater
extinction. We model this behavior, and show that the relation is a simple
consequence of the greater mass loss and faster evolution times of high mass
stars. The relation is important because it provides a natural explanation for
the invariance of the [O III] 5007 planetary nebula luminosity function (PNLF)
with population age: bright Population I PNe are extinguished below the cutoff
of the PNLF. It also explains the counter-intuitive observation that
intrinsically luminous Population I PNe often appear fainter than PNe from
older, low-mass progenitors.Comment: 12 pages, 2 figures, accepted for ApJ, April 10, 199
Introduction
The following articles are selected from the papers presented at the International
Congress on the Social History of Alcohol in 1993. In their focus either on drinking
practices or on social responses to drinking, they exemplify the primary concerns
of alcohol history. Approaches are often interdisciplinary, exploiting new types of
sources such as material culture and oral history as well as exploring new uses of
traditional documentary sources. These studies invite comparison among the
experiences with alcohol of various societies and suggest the utility for social
historians of examining international discourses over the use and governance of a
set of substances persistently intertwined in human affairs.Les articles suivants ont été choisis parmi ceux qui ont été présentés à l'occasion
du International Congress on the Social History of Alcohol, en 1993. Ils portent sur
les habitudes de consommation d'alcool ou les réactions de la société face à la
consommation d'alcool et illustrent ainsi les principales préoccupations de l'histoire
de l'alcool. Les auteurs adoptent souvent une démarche pluridisciplinaire et exploitent
de nouvelles sources, telles que la culture matérielle et l'histoire orale, et
examinent de nouvelles façons d'utiliser les sources documentaires traditionnelles.
Ces études incitent à comparer les expériences vécues par diverses sociétés au
chapitre de l'alcool et démontrent l'utilité pour l'historien social d'étudier les
traités internationaux sur la consommation et la gestion de substances qui ont
toujours été intimement liées à la vie des hommes
A Possible Hidden Population of Spherical Planetary Nebulae
We argue that relative to non-spherical planetary nebulae (PNs), spherical
PNs are about an order of magnitude less likely to be detected, at distances of
several kiloparsecs. Noting the structure similarity of halos around
non-spherical PNs to that of observed spherical PNs, we assume that most
unobserved spherical PNs are also similar in structure to the spherical halos
around non-spherical PNs. The fraction of non-spherical PNs with detected
spherical halos around them, taken from a recent study, leads us to the claim
of a large (relative to that of non-spherical PNs) hidden population of
spherical PNs in the visible band. Building a toy model for the luminosity
evolution of PNs, we show that the claimed detection fraction of spherical PNs
based on halos around non-spherical PNs, is compatible with observational
sensitivities. We use this result to update earlier studies on the different PN
shaping routes in the binary model. We estimate that ~30% of all PNs are
spherical, namely, their progenitors did not interact with any binary
companion. This fraction is to be compared with the ~3% fraction of observed
spherical PNs among all observed PNs. From all PNs, ~15% owe their moderate
elliptical shape to the interaction of their progenitors with planets, while
\~55% of all PNs owe their elliptical or bipolar shapes to the interaction of
their progenitors with stellar companions.Comment: AJ, in pres
On the Luminosities and Temperatures of Extended X-ray Emission from Planetary Nebulae
We examine mechanisms that may explain the luminosities and relatively low
temperatures of extended X-ray emission in planetary nebulae. By building a
simple flow structure for the wind from the central star during the proto, and
early, planetary nebulae phase, we estimate the temperature of the X-ray
emitting gas and its total X-ray luminosity. We conclude that in order to
account for the X-ray temperature and luminosity, both the evolution of the
wind from the central star and the adiabatic cooling of the post-shocked wind's
material must be considered. The X-ray emitting gas results mainly from shocked
wind segments that were expelled during the early planetary nebulae phase, when
the wind speed was moderate. Alternatively, the X-ray emitting gas may result
from a collimated fast wind blown by a companion to the central star. Heat
conduction and mixing between hot and cool regions are likely to occur in some
cases and may determine the detailed X-ray morphology of a nebula, but are not
required to explain the basic properties of the X-ray emitting gas.Comment: ApJ, submitted; 16 page
Andrew Wiese — Places of Their Own: African American Suburbanization in the Twentieth Century
Chemical Abundances of Planetary Nebulae in the Sagittarius Dwarf Elliptical Galaxy
Spectrophotometry and imaging of the two planetary nebulae He2-436 and
Wray16-423, recently discovered to be in the Sagittarius dwarf elliptical
galaxy, are presented. Wray16-423 is a high excitation planetary nebula (PN)
with a hot central star. In contrast He2-436 is a high density PN with a cooler
central star and evidence of local dust, the extinction exceeding that for
Wray16-423 by E(B-V)=0.28. The extinction to Wray16-423, (E(B-V)=0.14), is
consistent with the extinction to the Sagittarius (Sgr) Dwarf. Both PN show
Wolf-Rayet features in their spectra, although the lines are weak in
Wray16-423. Images in [O III] and H-alpha+[N II], although affected by poor
seeing, yield a diameter of 1.2'' for Wray16-423 after deconvolution; He~2-436
was unresolved. He2-436 has a luminosity about twice that of Wray16-423 and its
size and high density suggest a younger PN. In order to reconcile the differing
luminosity and nebular properties of the two PN with similar age progenitor
stars, it is suggested that they are on He burning tracks
The abundance pattern is very similar in both nebulae and shows an oxygen
depletion of -0.4 dex with respect to the mean O abundance of Galactic PN and
[O/H] = -0.6. The Sgr PN progenitor stars are representative of the higher
metallicity tail of the Sgr population. The pattern of abundance depletion is
similar to that in the only other PN in a dwarf galaxy companion of the Milky
Way, that in Fornax, for which new spectra are presented. However the
abundances are larger than for Galactic halo PN suggesting a later formation
age. The O abundance of the Sgr galaxy deduced from its PN, shows similarities
with that of dwarf ellipticals around M31, suggesting that this galaxy was a
dwarf elliptical before its interaction with the Milky Way.Comment: 24 pages, Latex (aas2pp4.sty) including 5 postscript figures. To
appear in Ap
Exploring Halo Substructure with Giant Stars. VI. Extended Distributions of Giant Stars Around the Carina Dwarf Spheroidal Galaxy -- How Reliable Are They?
The question of the existence of active tidal disruption around various dSph
galaxies remains controversial. That debate often centers on the nature (bound
vs. unbound) of extended populations of stars. However, the more fundamental
issue of the very existence of the extended populations is still contentious.
We present an evaluation of the debate centering on one particular dSph,
Carina, for which claims both for and against the existence of stars beyond the
King radius have been made. Our review includes an examination of all previous
studies bearing on the Carina radial profile and shows that the survey method
which achieves the highest detected dSph signal-to-background in the outer
parts of the galaxy is the Washington M, T2 + DDO51 (MTD) filter approach from
Paper II in this series. We then address statistical methods used to evaluate
the reliability of MTD surveys in the presence of photometric errors and for
which a new, a posteriori statistical analysis methodology is provided.
Finally, these statistical methods are tested by new spectroscopy of stars in
the MTD-selected Carina candidate sample. Of 74 candidate giants with follow-up
spectroscopy, the MTD technique identified 61 new Carina members, including 8
stars outside the King radius. From a sample of 29 stars not initially
identified as candidate Carina giants but that lie just outside of our
selection criteria, 12 have radial velocities consistent with membership,
including 5 extratidal stars. Carina is shown to have an extended population of
giant stars extending to a major axis radius of 40' (1.44x the nominal King
radius).Comment: 56 pages, 10 figures. Submitted to the Astronomical Journal, 2004 Sep
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