Search results for "shift"

showing 10 items of 1226 documents

The structure of cosmic voids in a LCDM Universe

2013

Eulerian cosmological codes are especially suited to properly describe the low density regions. This property makes this class of codes excellent tools to study the formation and evolution of cosmic voids. Following such ideas, we present the results of an Eulerian adaptive mesh refinement (AMR) hydrodynamical and N-body simulation, that contrary to the common practice, has been designed to refine the computational grid in the underdense regions of the simulated volume. Thus, the void regions are better described due to the combined effect of the Eulerian character of the numerical technique and the use of high numerical resolution from the AMR approach. To analyse the outcome of this simul…

PhysicsVoid (astronomy)COSMIC cancer databaseCosmology and Nongalactic Astrophysics (astro-ph.CO)Density gradient010308 nuclear & particles physicsAdaptive mesh refinementDark matterFOS: Physical sciencesAstronomy and AstrophysicsEulerian pathAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesRedshiftComputational physicssymbols.namesakeTheoretical physicsSpace and Planetary Science0103 physical sciencessymbolsDensity contrast010303 astronomy & astrophysicsAstrophysics - Cosmology and Nongalactic Astrophysics
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On the microwave background anisotropy produced by big voids in open universes

1996

The Tolman-Bondi solution of the Einstein equations is used in order to model the time evolution of the void observed in Bo\"otes. The present density contrast of the central region ($\sim -0.75$) and its radius ($\sim 30h^{-1} \ Mpc$) are fixed, while the density parameter of the Universe, the amplitude of the density contrast inside the void wall, the width of this wall and the distance from the void centre to the Local Group are appropriately varied. The microwave background anisotropy produced by Bo\"otes-like voids is estimated for a significant set of locations. All the voids are placed far from the last scattering surface. It is shown that the anisotropy generated by these voids stro…

PhysicsVoid (astronomy)Condensed matter physicsScatteringAstrophysics (astro-ph)Cosmic microwave backgroundFOS: Physical sciencesAstronomy and AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsRedshiftDipoleAmplitudeSpace and Planetary ScienceQuantum mechanicsDensity contrastAnisotropyMonthly Notices of the Royal Astronomical Society
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Confined Pt-1(1+) Water Clusters in a MOF Catalyze the Low-Temperature Water-Gas Shift Reaction with both CO2 Oxygen Atoms Coming from Water

2018

[EN] The synthesis and reactivity of single metal atoms in a low-valence state bound to just water, rather than to organic ligands or surfaces, is a major experimental challenge. Herein, we show a gram-scale wet synthesis of Pt-1(1+) stabilized in a confined space by a crystallographically well-defined first water sphere, and with a second coordination sphere linked to a metal-organic framework (MOF) through electrostatic and H-bonding interactions. The role of the water cluster is not only isolating and stabilizing the Pt atoms, but also regulating the charge of the metal and the adsorption of reactants. This is shown for the low-temperature water-gas shift reaction (WGSR: CO + H2O CO2 + H…

PhysicsWater–gas shift reactionQuímica Inorgánicabiology010405 organic chemistryWater-gas shift reactionSingle atom catalystGeneral MedicineGeneral ChemistryMetal-organic frameworks010402 general chemistrybiology.organism_classification01 natural sciencesCatalysisWater-gas shift reactionSingle-atom catalyst0104 chemical sciencesOxygen atomWater clustersPhysical chemistryValenciaMetal-organic frameworks (MOFs)Platinum
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CSRZ-ASK and DPSK 40 Gb/s All-Raman WDM Transmission Based on UltraWave Fiber

2006

In this paper, we report a complete experimental and numerical analysis of 40 Gb/s WDM ultra long-haul (ULH) transmission using CSRZ-DPSK and CSRZ-ASK modulation formats on UltraWavetrade fiber spans. Experimental results compare well with full numerical simulations

PhysicsWdm transmissionbusiness.industryAmplitude-shift keyingsymbols.namesakeOpticsTransmission (telecommunications)ModulationAsk priceWavelength-division multiplexingsymbolsOptoelectronicsFiberbusinessRaman spectroscopyLEOS 2006 - 19th Annual Meeting of the IEEE Lasers and Electro-Optics Society
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A Preliminary Analysis of a New Chandra Observation (ObsID 6148) of Cir X-1

2008

We present the preliminary spectral analysis of a 25 ks long Chandra observation of the peculiar source Cir X–1 near the periastron passage. We estimate more precise coordinates of the source compatible with the optical and radio counterpart coordinates. We detect emission lines associated to Mg XII, Si XIII, Si XIV, S XV, S XVI Ar XVII, Ar XVIII, Ca XIX, Ca XX, Fe XXV, Fe XXVI showing a redshift of 470 km s−1. The more intense emission features at 6.6 keV show a double‐peaked shape that can be modelled with two or three Gaussian lines.

PhysicsX-ray binaries Accretion and accretion disks Neutron stars Distances redshifts radial velocities; spatial distribution of galaxies Black holesX-ray binaries Accretion and accretion disks Neutron stars Distances redshifts radial velocitieGaussianX-ray binaryAstronomyAstrophysicsRedshiftPreliminary analysisRed shiftNeutron starsymbols.namesakeSettore FIS/05 - Astronomia E AstrofisicasymbolsSpectral analysisEmission spectrumspatial distribution of galaxies Black holes
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The XMM-Newton survey of the ELAIS-S1 field

2006

We have surveyed with XMM-Newton the central ~0.6 deg2 region of the ELAIS-S1 field down to flux limits of ~5.5X10-16 cgs (0.5-2 keV, S band), ~2X10-15 cgs (2-10 keV, H band), and ~4X10-15 cgs (5-10 keV, HH band). We detect a total of 478 sources, 395 and 205 of which detected in the S and H bands respectively. We identified 7 clearly extended sources and estimated their redshift through X-ray spectral fits with thermal models. In four cases the redshift is consistent with z=0.4. We have computed the angular correlation function of the sources in the S and H bands, finding best fit correlation angles theta_0=5.2+/-3.8 arcsec and theta_0=12.8+/-7.8 arcsec respectively. A rough estimate of th…

PhysicsX-rays : galaxieField (physics)galaxies : activeAstrophysics (astro-ph)FOS: Physical sciencesFluxAstronomy and AstrophysicsAstrophysicsH bandAstrophysicsRedshiftDistribution (mathematics)Space and Planetary ScienceRange (statistics)Relative densitylarge-scale structure of UniverseS bandAstronomy & Astrophysics
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Precise determination of the ground state hyperfine structure splitting of43Ca II

1994

We have performed a laser microwave double resonance experiment on43Ca+ ions stored in a Paul ion trap. The ground state hfs splitting has been determined to Δν=3 225 608 286. 4(3) Hz. The value is corrected for small Zeeman, Stark and second order Doppler shifts as well as for light shift effects caused by the laserfields. The uncertainty is mainly determined by the errors of these corrections.

PhysicsZeeman effectResonanceAtomic and Molecular Physics and OpticsIonsymbols.namesakeLight ShiftsymbolsPhysics::Atomic PhysicsIon trapAtomic physicsGround stateDoppler effectHyperfine structureZeitschrift f�r Physik D Atoms, Molecules and Clusters
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Detecting filamentary pattern in the cosmic web : a catalogue of filaments for the SDSS

2014

The main feature of the spatial large-scale galaxy distribution is its intricate network of galaxy filaments. This network is spanned by the galaxy locations that can be interpreted as a three-dimensional point distribution. The global properties of the point process can be measured by different statistical methods, which, however, do not describe directly the structure elements. The morphology of the large scale structure, on the other hand, is an important property of the galaxy distribution. Here we apply an object point process with interactions (the Bisous model) to trace and extract the filamentary network in the presently largest galaxy redshift survey, the Sloan Digital Sky Survey (…

Physics[PHYS]Physics [physics]Cosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsFOS: Physical sciencesAstronomyAstronomy and AstrophysicsAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsRedshift survey01 natural sciencesGalaxySpace and Planetary ScienceSupercluster[SDU]Sciences of the Universe [physics]0103 physical sciencesSatellite galaxyBrightest cluster galaxyInteracting galaxyIrregular galaxy[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]010303 astronomy & astrophysicsLenticular galaxyAstrophysics::Galaxy AstrophysicsAstrophysics - Cosmology and Nongalactic Astrophysics
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Pressure Shift and Gravitational Red Shift of Balmer Lines in White Dwarfs. Rediscussion

2015

The Stark-induced shift and asymmetry, the so-called pressure shift (PS) of $H_\alpha$ and $H_\beta$ Balmer lines in spectra of DA white dwarfs (WDs), as masking effects in measurements of the gravitational red shift in WDs, have been examined in detail. The results are compared with our earlier ones from before a quarter of a century (Grabowski et al. 1987, hereafter ApJ'87; Madej and Grabowski 1990). In these earlier papers, as a dominant constituent of the Balmer-line-profiles, the standard, symmetrical Stark line profiles, shifted as the whole by PS-effect, were applied to all spectrally active layers of the WD atmosphere. At present, in each of the WD layers, the Stark-line-profiles (e…

Physicsatomic processes; line: formation; line: profiles; plasmas; white dwarfsmedia_common.quotation_subjectFOS: Physical sciencesBalmer seriesWhite dwarfAstronomy and AstrophysicsAstrophysicsPlasmaAsymmetrySpectral linesymbols.namesakeStarsAstrophysics - Solar and Stellar AstrophysicsSpace and Planetary SciencesymbolsSolar and Stellar Astrophysics (astro-ph.SR)Line (formation)media_commonGravitational redshift
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Operation conditions and stability of a degenerate two-photon laser

1993

Abstract The presence of a far off-resonant intermediate level in a degenerate three-level two-photon laser model manifests through a steady pump-dependent and a dynamic frequency shift on the laser equations. The steady shift strongly affects the pump threshold necessary for emission, preventing it in certain cases. The dynamic shift makes the frequency pulling/pushing to be intensity-dependent and substantially modify the domains of existence and stability of the lasing solution permitting stable operation for large cavity losses in certain cases.

Physicsbusiness.industryDegenerate energy levelsPhysics::OpticsFrequency shiftIntermediate levelLaserStability (probability)Atomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialslaw.inventionOpticsTwo-photon excitation microscopylawElectrical and Electronic EngineeringPhysical and Theoretical ChemistrybusinessLasing thresholdOptics Communications
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