388 research outputs found
Evolution of stars with suppressed core convection
Stellar evolution on the upper main sequence was computed for models of stars with cores assumed to be in radiative equilibrium, up to the point of central helium ignition. The role of the Schonberg-Chandrasekhar limit for an isothermal core is found to be critical for the evolutionary tracks. Observational data are used to rule out the hypothesis of evolution with radiative cores (in upper main-sequence stars) and, by implication, of magnetic fields that are sufficiently strong to have suppressed the core convention
Flood basalt eruptions, comet showers, and mass extinction events
A chronology of initiation dates of the major continental flood basalt episodes has been established from compilation of published K-Ar and Ar-Ar ages of basaltic flows and related basic intrusions. The dating is therefore independent of the biostratigraphic and paleomagnetic time scales, and the estimated errors of the inititation dates are approximately + or - 4 pct. There are 11 distinct episodes of continental flood basalts known during the past 250 Myr. The data show that flood basalt episodes are generally relatively brief geologic events, with intermittent eruptions during peak output periods lasting ony 2 to 3 Myr or less. Statistical analyses suggest that these episodes may have occurred quasi-periodically with a mean cycle time of 32 + or - 1 Myr. The initiation dates of the flood basalts are close to the estimated dates of marine mass extinctions and impact-crater clusters. Although a purely internal forcing might be argued for the flood basalt volcanism, quasi-periodic comet impacts may be the trigger for both the flood basalts and the extinctions. Impact cratering models suggest that large-body impactors lead to deep initial cratering, and therefore may cause mantle disturbances and initiate mantle plume activity. The flood basalt episodes commonly mark the initiation or jump of a mantle hotspot, and are often followed by continental rifting and separation. Evidence from dynamical studies of impacts, occurrences of craters and hotspots, and the geochemistry of boundary layers is synthesized to provide a possible model of impact-generated volcanism. Flood basalt eruptions may themselves have severe effects on climate, and possibly on life. Impacts might, as a result, have led to mass extinctions through direct atmospheric disturbances, and/or indirectly through prolonged flood basalt volcanism
Forehead Skin Blood Flow in Normal Neonates during Active and Quiet Sleep, Measured with a Diode Laser Doppler Instrument
Changes in forehead skin blood flow during active and quiet sleep were determined in 16 healthy neonates using a recently developed semi-conductor laser Doppler flow meter without light conducting fibres. Measurements were carried out at a postnatal age varying from 5 hours to 7 days. The two sleep states could be distinguished in 17 recordings. The mean skin blood flow values during active sleep were significantly higher (p<0.01) than those during quiet sleep, the mean increase being 28.1%. The variability of the flow signal, expressed as the coefficient of variation, changed significantly from 23.1% during active sleep to 18.2% during quiet sleep
Pulsational instability of yellow hypergiants
Instability of population I (X=0.7, Y=0.02) massive stars against radial
oscillations during the post-main sequence gravitational contraction of the
helium core is investigated. Initial stellar masses are in the range from
65M_\odot to 90M_\odot. In hydrodynamic computations of self-exciting stellar
oscillations we assumed that energy transfer in the envelope of the pulsating
star is due to radiative heat conduction and convection. The convective heat
transfer was treated in the framework of the theory of time-dependent turbulent
convection. During evolutionary expansion of outer layers after hydrogen
exhaustion in the stellar core the star is shown to be unstable against radial
oscillations while its effective temperature is Teff > 6700K for
Mzams=65M_\odot and Teff > 7200K for mzams=90M_\odot. Pulsational instability
is due to the \kappa-mechanism in helium ionization zones and at lower
effective temperature oscillations decay because of significantly increasing
convection. The upper limit of the period of radial pulsations on this stage of
evolution does not exceed 200 day. Radial oscillations of the hypergiant resume
during evolutionary contraction of outer layers when the effective temperature
is Teff > 7300K for Mzams=65M_\odot and Teff > 7600K for Mzams=90M_\odot.
Initially radial oscillations are due to instability of the first overtone and
transition to fundamental mode pulsations takes place at higher effective
temperatures (Teff > 7700K for Mzams=65M_\odot and Teff > 8200K for
Mzams=90M_\odot). The upper limit of the period of radial oscillations of
evolving blueward yellow hypergiants does not exceed 130 day. Thus, yellow
hypergiants are stable against radial stellar pulsations during the major part
of their evolutionary stage.Comment: 20 pages, 7 gigures. Accepted for publication in Astronomy Letter
The light-curve modulation of XY And and UZ Vir - Two Blazhko RR Lyrae stars with additional frequencies
A thorough analysis of multicolour CCD observations of two modulated
RRab-type variables, XY And and UZ Vir is presented. These Blazhko stars show
relatively simple light-curve modulation with the usual multiplet structures in
their Fourier spectra. One additional, independent frequency with
linear-combination terms of the pulsation frequency is also detected in the
residual spectrum of each of the two stars. The amplitude and phase relations
of the triplet components are studied in detail. Most of the epoch-independent
phase differences show a slight, systematic colour dependence, however, these
trends have the opposite sign in the two stars. The mean values of the global
physical parameters and their changes with Blazhko phase are determined
utilizing the Inverse Photometric Method (IPM). The modulation properties and
the IPM results are compared for the two variables. The pulsation period of XY
And is the shortest when its pulsation amplitude is the highest, while UZ Vir
has the longest pulsation period at this phase of the modulation. Despite this
opposite behaviour, the phase relations of their mean-physical-parameter
variations are similar. These results are not in accord with the predictions of
the Blazhko model of Stothers (2006, ApJ, 652, 643).Comment: Accepted for publication in MNRAS. The paper contains 7 figures and
12 tables. Tables 5, 6 and A1-A5 will be published in full online only. See
electronic data on http://konkoly.hu/24/publications/ als
The Period-Luminosity Relation of Red Supergiant Stars in the Small Magellanic Cloud
The characteristics of light variation of RSGs in SMC are analyzed based on
the nearly 8-10 year long data collected by the ASAS and MACHO projects. The
identified 126 RSGs are classified into five categories accordingly: 20 with
poor photometry, 55 with no reliable period, 6 with semi-regular variation, 15
with Long Secondary Period (LSP) and distinguishable short period and 30 with
only LSP. For the semi-regular variables and the LSP variables with
distinguishable short period, the Ks band period-luminosity (P-L) relation is
analyzed and compared with that of the Galaxy, LMC and M33. It is found that
the RSGs in these galaxies obey similar P-L relation except the Galaxy. In
addition, the P-L relations in the infrared bands, namely the 2MASS JHKs,
Spitzer/IRAC and Spitzer/MIPS 24 {\mu}m bands, are derived with high
reliability. The best P-L relation occurs in the Spitzer/IRAC [3.6] and [4.5]
bands. Based on the comparison with the theoretical calculation of the P-L
relation, the mode of pulsation of RSGs in SMC is suggested to be the first
overtone radial mode.Comment: 82 pages, 31 figures, 6 tables, accepted for publication in Ap
Intermediate mass stars: updated models
A new set of stellar models in the mass range 1.2 to 9 is
presented. The adopted chemical compositions cover the typical galactic values,
namely and . A comparison among
the most recent compilations of similar stellar models is also discussed. The
main conclusion is that the differencies among the various evolutionary results
are still rather large. For example, we found that the H-burning evolutionary
time may differ up to 20 %. An even larger disagreement is found for the
He-burning phase (up to 40-50 %). Since the connection between the various
input physics and the numerical algorithms could amplify or counterbalance the
effect of a single ingredient on the resulting stellar model, the origin of
this discrepancies is not evident. However most of these discrepancies, which
are clearly found in the evolutionary tracks, are reduced on the isochrones. By
means of our updated models we show that the ages inferred by the theory of
stellar evolution is in excellent agreement with those obtained by using other
independent methods applied to the nearby Open Clusters. Finally, the
theoretical initial/final mass relation is revised.Comment: 35 pages, 24 figures, 4 tables, accepted for publication in the
Astrophisycal Journa
Red Supergiant Stars in the Large Magellanic Cloud: I. The Period-Luminosity Relation
From previous samples of Red Supergiants (RSGs) by various groups, 191
objects are assembled to compose a large sample of RSG candidates in LMC. For
189 of them, the identity as a RSG is verified by their brightness and color
indexes in several near- and mid-infrared bands related to the 2MASS JHKs bands
and the Spitzer/IRAC and Spitzer/MIPS bands. From the visual time-series
photometric observations by the ASAS and MACHO projects which cover nearly 8-10
years, the period and amplitude of light variation are analyzed carefully using
both the PDM and Period04 methods. According to the properties of light
variation, these objects are classified into five categories: (1) 20 objects
are saturated in photometry or located in crowded stellar field with poor
photometric results, (2) 35 objects with too complex variation to have any
certain period, (3) 23 objects with irregular variation, (4) 16 objects with
semi-regular variation, and (5) 95 objects with Long Secondary Period (LSP)
among which 31 have distinguishable short period, and 51 have a long period
shorter than 3000 days that can be determined with reasonable accuracy. For the
semi-regular variables and the LSP variables with distinguishable short period,
the period-luminosity relation is analyzed in the visual, near-infrared and
mid-infrared bands. It is found that the P-L relation is tight in the infrared
bands such as the 2MASS JHKs bands and the Spitzer/IRAC bands, in particular in
the Spitzer/IRAC [3.6] and [4.5] bands; meanwhile, the P-L relation is
relatively sparse in the V band which may be caused by the inhomogeneous
interstellar extinction. The results are compared with others' P-L
relationships for RSGs and the P-L sequences of red giants in LMC.Comment: 41 pages, 14 figures, 4 tables, accepted by Ap
Fitting Blazhko light curves
The correct amplitude and phase modulation formalism of the Blazhko
modulation is given. The harmonic order dependent amplitude and phase
modulation form is equivalent with the Fourier decomposition of multiplets. The
amplitude and phase modulation formalism used in electronic transmission
technique as introduced by Benk\H{o}, Szab\'o and Papar\'o (2011, MNRAS 417,
974) for Blazhko stars oversimplifies the amplitude and phase modulation
functions thus it does not describe the light variation in full detail.
The results of the different formalisms are compared and documented by
fitting the light curve of a real Blazhko star, CM UMa.Comment: 8 pages, 5 figures. Accepted for publication in MNRA
Long-term photometric behaviour of XZ Dra Binarity or magnetic cycle of a Blazhko type RRab star
The extended photometry available for XZ Dra, a Blazhko type RR Lyrae star,
makes it possible to study its long-term behavior. It is shown that its
pulsation period exhibit cyclic, but not strictly regular variations with
approx. 7200 d period. The Blazhko period (approx. 76 d) seems to follow the
observed period changes of the fundamental mode pulsation with dP_B/dP_0=7.7 x
10^4 gradient. Binary model cannot explain this order of period change of the
Blazhko modulation, nevertheless it can be brought into agreement with the O-C
data of the pulsation. The possibility of occurrence of magnetic cycle is
raised.Comment: 13 pages, 11 figures (submitted to A&A
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