16,307 research outputs found
HST measures of Mass Accretion Rates in the Orion Nebula Cluster
The present observational understanding of the evolution of the mass
accretion rates (Macc) in pre-main sequence stars is limited by the lack of
accurate measurements of Macc over homogeneous and large statistical samples of
young stars. Such observational effort is needed to properly constrain the
theory of star formation and disk evolution. Based on HST/WFPC2 observations,
we present a study of Macc for a sample of \sim 700 sources in the Orion Nebula
Cluster, ranging from the Hydrogen-burning limit to M\ast \sim 2M\odot. We
derive Macc from both the U-band excess and the H{\alpha} luminosity
(LH{\alpha}), after determining empirically both the shape of the typical
accretion spectrum across the Balmer jump and the relation between the
accretion luminosity (Lacc) and LH{\alpha}, that is Lacc/L\odot =
(1.31\pm0.03)\cdotLH{\alpha}/L\odot + (2.63\pm 0.13). Given our large
statistical sample, we are able to accurately investigate relations between
Macc and the parameters of the central star such as mass and age. We clearly
find Macc to increase with stellar mass, and decrease over evolutionary time,
but we also find strong evidence that the decay of Macc with stellar age occurs
over longer timescales for more massive PMS stars. Our best fit relation
between these parameters is given by: log(Macc/M\odot\cdotyr)=(-5.12 \pm 0.86)
-(0.46 \pm 0.13) \cdot log(t/yr) -(5.75 \pm 1.47)\cdot log(M\ast/M\odot) +
(1.17 \pm 0.23)\cdot log(t/yr) \cdot log(M\ast/M\odot). These results also
suggest that the similarity solution model could be revised for sources with
M\ast > 0.5M\odot. Finally, we do not find a clear trend indicating
environmental effects on the accretion properties of the sources.Comment: 17 pages, 15 figures, accepted for publication in Ap
Value of the magnetic resonance image of the lumbar spine with load in the evaluation of stenosis of the lumbar spinal canal
UNIFESPUNIFESPSciEL
Image diagnosis for evaluation of heterotopic ossification
UNIFESP-EPM DDIDiagnósticos da AméricaUNIFESP-EPMHospital São LuizUNIFESP, EPM, DDIUNIFESP, EPMSciEL
A New Method for the Assessment of Age and Age-Spread of Pre-Main Sequence Stars in Young Stellar Associations of the Magellanic Clouds
We present a new method for the evaluation of the age and age-spread among
pre-main-sequence (PMS) stars in star-forming regions in the Magellanic Clouds,
accounting simultaneously for photometric errors, unresolved binarity,
differential extinction, stellar variability, accretion and crowding. The
application of the method is performed with the statistical construction of
synthetic color-magnitude diagrams using PMS evolutionary models. We convert
each isochrone into 2D probability distributions of artificial PMS stars in the
CMD by applying the aforementioned biases that dislocate these stars from their
original CMD positions. A maximum-likelihood technique is then applied to
derive the probability for each observed star to have a certain age, as well as
the best age for the entire cluster. We apply our method to the photometric
catalog of ~2000 PMS stars in the young association LH 95 in the LMC, based on
the deepest HST/ACS imaging ever performed toward this galaxy, with a detection
limit of V~28, corresponding to M~0.2 Msun. Our treatment shows that the age
determination is very sensitive to the considered grid of evolutionary models
and the assumed binary fraction. The age of LH 95 is found to vary from 2.8 Myr
to 4.4 Myr, depending on these factors. Our analysis allows us to disentangle a
real age-spread from the apparent CMD-broadening caused by the physical and
observational biases. We find that LH 95 hosts an age-spread well represented
by a gaussian distribution with a FWHM of the order of 2.8 Myr to 4.2 Myr
depending on the model and binary fraction. We detect a dependence of the
average age of the system with stellar mass. This dependence does not appear to
have any physical meaning, being rather due to imperfections of the PMS
evolutionary models, which tend to predict lower ages for the intermediate
masses, and higher ages for low-mass stars.Comment: 19 pages, 16 figures, accepted for publication by the Astrophysical
Journa
Quantitative Evidence for an Intrinsic Age Spread in the Orion Nebula Cluster
Aims. We present a study of the distribution of stellar ages in the Orion
Nebula Cluster (ONC) based on accurate HST photometry taken from the HST
Treasury Program observations of the ONC utilizing the most recent estimate of
the cluster's distance (Menten et al. 2007). We investigate the presence of an
intrinsic age spread in the region and a possible trend of age with the spatial
distribution. Methods. We estimate the extinction and accretion luminosity
towards each source by performing synthetic photometry on an empirical
calibration of atmospheric models (Da Rio et al. 2010) using the package
Chorizos (Maiz-Apellaniz 2004). The position of the sources in the HR-diagram
is compared with different theoretical isochrones to estimate the mean cluster
age and age dispersion. Through Monte Carlo simulations we quantify the amount
of intrinsic age spread in the region, taking into account uncertainties on the
distance, spectral type, extinction, unresolved binaries, accretion and
photometric variability. Results. According to Siess et al. (2000) evolutionary
models the mean age of the Cluster is 2.2 Myr with a scatter of few Myrs. With
Monte Carlo simulations we find that the observed age spread is inconsistent
with a coeval stellar population, but is in agreement with a star formation
activity between 1.5 and 3.5 Myrs. We also observe light evidence for a trend
of ages with spatial distribution.Comment: 12 pages, 12 figures, Accepted for publication in Astronomy and
Astrophysic
Rapid star formation and global gravitational collapse
Most young stars in nearby molecular clouds have estimated ages of 1–2 Myr, suggesting that star formation is rapid. However, small numbers of stars in these regions with inferred ages of > rsim 5–10 Myr have been cited to argue that star formation is instead a slow, quasi‐static process. When considering these alternative pictures it is important to recognize that the age spread in a given star‐forming cloud is necessarily an upper limit to the time‐scales of local collapse, as not all spatially distinct regions will start contracting at precisely the same instant. Moreover, star‐forming clouds may dynamically evolve on time‐scales of a few Myr; in particular, global gravitational contraction will tend to yield increasing star formation rates with time due to generally increasing local gas densities. We show that two different numerical simulations of dynamic, flow‐driven molecular cloud formation and evolution (1) predict age spreads for the main stellar population roughly consistent with observations and (2) raise the possibility of forming small numbers of stars early in cloud evolution, before global contraction concentrates the gas and the bulk of the stellar population is produced. In general, the existence of a small number of older stars among a generally much younger population is consistent with the picture of dynamic star formation and may even provide clues to the time evolution of star‐forming clouds.Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/90399/1/j.1365-2966.2011.20131.x.pd
No wide spread of stellar ages in the Orion Nebula Cluster
The wide luminosity dispersion seen for stars at a given effective
temperature in the H-R diagrams of young clusters and star forming regions is
often interpreted as due to significant (~10 Myr) spreads in stellar
contraction age. In the scenario where most stars are born with circumstellar
discs, and that disc signatures decay monotonically (on average) over
timescales of only a few Myr, then any such age spread should lead to clear
differences in the age distributions of stars with and without discs. We have
investigated large samples of stars in the Orion Nebula Cluster (ONC) using
three methods to diagnose disc presence from infrared measurements. We find no
significant difference in the mean ages or age distributions of stars with and
without discs, consistent with expectations for a coeval population. Using a
simple quantitative model we show that any real age spread must be smaller than
the median disc lifetime. For a log-normal age distribution, there is an upper
limit of <0.14 dex (at 99% confidence) to any real age dispersion, compared to
the ~=0.4 dex implied by the H-R diagram. If the mean age of the ONC is 2.5
Myr, this would mean at least 95% of its low-mass stellar population has ages
between 1.3--4.8 Myr. We suggest that the observed luminosity dispersion is
caused by a combination of observational uncertainties and physical mechanisms
that disorder the conventional relationship between luminosity and age for pre
main-sequence stars. This means that individual stellar ages from the H-R
diagram are unreliable and cannot be used to directly infer a star formation
history. Irrespective of what causes the wide luminosity dispersion, the
finding that any real age dispersion is less than the median disc lifetime
argues strongly against star formation scenarios for the ONC lasting longer
than a few Myr.Comment: To appear in MNRAS, 13 page
The double Caldeira-Leggett model: Derivation and solutions of the master equations, reservoir-induced interactions and decoherence
In this paper we analyze the double Caldeira-Leggett model: the path integral
approach to two interacting dissipative harmonic oscillators. Assuming a
general form of the interaction between the oscillators, we consider two
different situations: i) when each oscillator is coupled to its own reservoir,
and ii) when both oscillators are coupled to a common reservoir. After deriving
and solving the master equation for each case, we analyze the decoherence
process of particular entanglements in the positional space of both
oscillators. To analyze the decoherence mechanism we have derived a general
decay function for the off-diagonal peaks of the density matrix, which applies
both to a common and separate reservoirs. We have also identified the expected
interaction between the two dissipative oscillators induced by their common
reservoir. Such reservoir-induced interaction, which gives rise to interesting
collective damping effects, such as the emergence of relaxation- and
decoherence-free subspaces, is shown to be blurred by the high-temperature
regime considered in this study. However, we find that different interactions
between the dissipative oscillators, described by rotating or counter-rotating
terms, result in different decay rates for the interference terms of the
density matrix.Comment: 42 pages, 7 figures, new discussion added, typos adde
Planetary companions around the K giant stars 11 UMi and HD 32518
11 UMi and HD 32518 belong to a sample of 62 K giant stars that has been
observed since February 2004 using the 2m Alfred Jensch telescope of the
Th\"uringer Landessternwarte (TLS) to measure precise radial velocities (RVs).
The aim of this survey is to investigate the dependence of planet formation on
the mass of the host star by searching for planetary companions around
intermediate-mass giants. An iodine absorption cell was used to obtain accurate
RVs for this study. Our measurements reveal that the RVs of 11 UMi show a
periodic variation of 516.22 days. The RV curve of HD 32518 shows sinusoidal
variations with a period of 157.54 days. The HIPPARCOS photometry as well as
our H\alpha core flux measurements reveal no variability with the RV period.
Thus, Keplerian motion is the most likely explanation for the observed RV
variations for both giant stars. An exoplanet with a minimum mass of 10.5
Jupiter masses orbits the K giant 11 UMi. The K1 III giant HD 32518 hosts a
planetary companion with a minimum mass of 3.0 Jupiter masses in a nearly
circular orbit. These are the 4th and 5th planets published from this TLS
survey.Comment: 11 pages, 16 figure
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