Search results for "SHIFT"

showing 10 items of 1226 documents

DYNAMICAL PHENOMENA IN THE ATMOSPHERE OF THE PROTO-PLANETARY NEBULA IRAS 22272+5435

2009

Radial velocity monitoring of the star HD 235858 confirmed regular variations with a peak-to-peak amplitude of about 10 km s–1 and a period of about 131.2 days. The light, color, and velocity variations are typical for RV Tauri stars. Splitting of low-excitation atomic lines was detected. The components are both blue- and redshifted relative to the systemic velocity. Significant variations are observed in the intensity of C2 and CN lines. Variable emission in the Hα profile, splitting of low-excitation atomic absorption lines, appearance of CN emission lines, blue wings of strong lines, and recent reddening give evidence of shocks and mass outflow obviously induced by atmospheric pulsations.

PhysicsAstronomyAstronomy and AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsPlanetary nebulaRedshiftAtmosphereRadial velocityStarsAmplitudeSpace and Planetary ScienceAstrophysics::Solar and Stellar AstrophysicsOutflowEmission spectrumAstrophysics::Galaxy AstrophysicsThe Astrophysical Journal
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Secondary gravitational anisotropies in open universes

1998

The applicability of the potential approximation in the case of open universes is tested. Great Attractor-like structures are considered in the test. Previous estimates of the Cosmic Microwave background anisotropies produced by these structures are analyzed and interpreted. The anisotropies corresponding to inhomogeneous ellipsoidal models are also computed. It is proved that, whatever the spatial symmetry may be, Great Attractor-like objects with extended cores (radius $\sim 10h^{-1}$),located at redshift $z=5.9$ in an open universe with density parameter $\Omega_{0}=0.2$, produce secondary gravitational anisotropies of the order of $10^{-5}$ on angular scales of a few degrees. This aniso…

PhysicsAstrophysics (astro-ph)Cosmic microwave backgroundFOS: Physical sciencesAstronomy and AstrophysicsRadiusAstrophysicsAstrophysicsCurvatureRedshiftGravitationGreat AttractorGravitational potentialSpace and Planetary ScienceAnisotropy
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Recovering the real-space correlation function from photometric redshift surveys

2008

Measurements of clustering in large-scale imaging surveys that make use of photometric redshifts depend on the uncertainties in the redshift determination. We have used light-cone simulations to show how the deprojection method successfully recovers the real space correlation function when applied to mock photometric redshift surveys. We study how the errors in the redshift determination affect the quality of the recovered two-point correlation function. Considering the expected errors associated to the planned photometric redshift surveys, we conclude that this method provides information on the clustering of matter useful for the estimation of cosmological parameters that depend on the la…

PhysicsAstrophysics (astro-ph)FOS: Physical sciencesAstronomy and AstrophysicsScale (descriptive set theory)AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsCorrelation function (astronomy)Space (mathematics)AstrophysicsGalaxyRedshiftDistribution (mathematics)Space and Planetary ScienceCluster analysisPhotometric redshift
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The X-ray Luminosity - Velocity Dispersion relation in the REFLEX Cluster Survey

2003

We present an estimate of the bolometric X-ray luminosity - velocity dispersion L_x - sigma_v relation measured from a new, large and homogeneous sample of 171 low redshift, X-ray selected galaxy clusters. The linear fitting of log(L_x) - log(sigma_v) gives L_x = 10^{32.72 \pm 0.08} sigma^{4.1 \pm 0.3}_v erg s^{-1} h^{-2}_{50}. Furthermore, a study of 54 clusters, for which the X-ray temperature of the intracluster medium T is available, allows us to explore two other scaling relations, L_x -T and sigma_v -T. From this sample we obtain L_x \propto T^{3.1 \pm 0.2} and sigma_v \propto T^{1.00 \pm 0.16}, which are fully consistent with the above result for the L_x-sigma_v. The slopes of L_x -T…

PhysicsAstrophysics (astro-ph)FOS: Physical sciencesSigmaVelocity dispersionAstronomy and AstrophysicsAstrophysicsAstrophysicsRedshiftLuminositySpace and Planetary ScienceIntracluster mediumEnergy sourceScalingGalaxy cluster
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Probing the internal solar magnetic field through g-modes

2006

The observation of g-mode candidates by the SoHO mission opens the possibility of probing the internal structure of the solar radiative zone (RZ) and the solar core more directly than possible via the use of the p-mode helioseismology data. We study the effect of rotation and RZ magnetic fields on g-mode frequencies. Using a self-consistent static MHD magnetic field model we show that a 1% g-mode frequency shift with respect to the Solar Seismic Model (SSeM) prediction, currently hinted in the GOLF data, can be obtained for magnetic fields as low as 300 kG, for current measured modes of radial order n=-20. On the other hand, we also argue that a similar shift for the case of the low order g…

PhysicsAstrophysics (astro-ph)Frequency shiftFOS: Physical sciencesFísicaAstronomy and AstrophysicsAstrophysicsRotationAstrophysicsRadiation zoneMagnetic fieldComputational physicsSolar coreSpace and Planetary ScienceSeismic modelingPhysics::Space PhysicsAstrophysics::Solar and Stellar AstrophysicsHelioseismologyMagnetohydrodynamics
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The exceptionally extended flaring activity in the X-ray afterglow of GRB 050730 observed with Swift and XMM-Newton

2007

We present the results of a detailed spectral and temporal analysis of Swift and XMM-Newton observations of the high redshift (z=3.969) GRB 050730. The X-ray afterglow of GRB 050730 was found to decline with time with superimposed intense flaring activity that extended over more than two orders of magnitude in time. Seven distinct re-brightening events starting from 236 s up to 41.2 ks after the burst were observed. The underlying decay of the afterglow was well described by a double broken power-law model with breaks at t_1= 237 +/- 20 s and t_2 = 10.1 (-2.2) (+4.6) ks. The temporal decay slopes before, between and after these breaks were alpha_1 = 2.1 +/- 0.3, alpha_2 = 0.44 (-0.08) (+0.1…

PhysicsAstrophysics (astro-ph)X-rayFOS: Physical sciencesAstronomy and AstrophysicsAstrophysicsAstrophysicsRedshiftGalaxylaw.inventionAfterglowSpectral evolutionSpace and Planetary SciencelawGamma-ray burstOrder of magnitudeFlare
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Gravitational lensing on the Cosmic Microwave Background by gravity waves

1997

We study the effect of a stochastic background of gravitational waves on the gravitational lensing of the Cosmic Microwave Background (CMB) radiation. It has been shown that matter density inhomogeneities produce a smoothing of the acoustic peaks in the angular power spectrum of the CMB anisotropies. A gravitational wave background gives rise to an additional smoothing of the spectrum. For the most simple case of a gravitational wave background arising during a period of inflation, the effect results to be three to four orders of magnitude smaller than its scalar counterpart, and is thus undetectable. It could play a more relevant role in models where a larger background of gravitational wa…

PhysicsAstrophysics and AstronomyNuclear and High Energy PhysicsGravitational-wave observatoryGravitational waveGravitational lensing formalismStrong gravitational lensingAstrophysics (astro-ph)AstronomyFOS: Physical sciencesAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsGravitational energyGravitational wave backgroundGeneral Relativity and Quantum CosmologyWeak gravitational lensingGravitational redshift
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Redshifts of southern clusters. II

1991

New redshifts are given for 21 clusters of galaxies from the Abell, Corwin, and Olowin Rich Cluster Catalogue. The redshift of the brightest cluster galaxy - where the brightest member is brighter than 15.5 - is employed as an indicator of the mean cluster redshift. The redshifts of first-, second-, and third-ranked galaxies are shown to agree, confirming the value of the survey procedure, although some clusters require more information than simply the redshift of the brightest cluster. 7 refs.

PhysicsAstrophysics::High Energy Astrophysical PhenomenaAstronomyAstronomy and AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsRedshiftGalaxyRadial velocityGalaxy groups and clustersAbell 2744Space and Planetary ScienceCluster (physics)Brightest cluster galaxyAstrophysics::Galaxy AstrophysicsGalaxy clusterThe Astronomical Journal
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XMM-Newton and VLT observations of the afterglow of GRB040827

2005

The field of the Gamma-Ray Burst GRB 040827 was observed with XMM-Newton and with the ESO/VLT starting ~6 and ~12 hours after the burst, respectively. A fading X-ray afterglow is clearly detected with the XMM-Newton/EPIC instrument, with a time decay t^(-delta), with delta=1.41+/-0.10. Its spectrum is well described by a power law (photon index Gamma=2.3+/-0.1) affected by an absorption largely exceeding (by a factor ~5) the expected Galactic one, requiring the contribution of an intrinsic, redshifted absorber. In the optical/NIR range, the afterglow emission was observed in the Ks band, as a weak source superimposed to the host galaxy, with magnitude Ks=19.44+/-0.13 (12 hours after the GRB…

PhysicsAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)FOS: Physical sciencesFluxAstronomy and AstrophysicsAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsGalaxyRedshiftAfterglowPhotometry (astronomy)Space and Planetary ScienceMagnitude (astronomy)Astrophysics::Earth and Planetary AstrophysicsGamma-ray burstAbsorption (electromagnetic radiation)Astrophysics::Galaxy Astrophysics
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The Redshift Distribution of Flat-Spectrum Radio Sources

2003

The redshift distribution of flat-spectrum radio sources with 5 GHz flux densities S>5 mJy is a key component in using current radio lens surveys to probe the cosmological model. We have constructed the first flat-spectrum radio sample in the flux density range 3-20 mJy. Our new sample has 33 sources; we have determined the redshifts of 14 of these (42% complete). The low mean redshift, ~0.75, of our faintest sample needs to be confirmed by further observations to improve the sample completeness. We also increased the redshift completeness of several surveys of brighter flat-spectrum sources. While the mean redshift, ~1.1 of flat-spectrum samples fainter than 1 Jy is nearly constant, the fr…

PhysicsAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)FluxFOS: Physical sciencesAstronomy and AstrophysicsQuasarAstrophysicsCosmological modelAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsSample (graphics)RedshiftDistribution (mathematics)Space and Planetary ScienceRange (statistics)Astrophysics::Galaxy Astrophysics
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