Search results for "Physics::Space Physics"

showing 10 items of 357 documents

Filter approach to the stochastic analysis of MDOF wind-excited structures

1999

Abstract In this paper, an approach useful for stochastic analysis of the Gaussian and non-Gaussian behavior of the response of multi-degree-of-freedom (MDOF) wind-excited structures is presented. This approach is based on a particular model of the multivariate stochastic wind field based upon a particular diagonalization of the power spectral density (PSD) matrix of the fluctuating part of wind velocity. This diagonalization is performed in the space of eigenvectors and eigenvalues that are called here wind-eigenvalues and wind-eigenvectors, respectively. From the examination of these quantities it can be recognized that the wind-eigenvectors change slowly with frequency while the first wi…

Astrophysics::High Energy Astrophysical PhenomenaGaussianAerospace EngineeringGeometryOcean EngineeringCondensed Matter PhysicWind speedMatrix (mathematics)symbols.namesakePhysics::Atmospheric and Oceanic PhysicsEigenvalues and eigenvectorsMathematicsCivil and Structural EngineeringStochastic processMechanical EngineeringMathematical analysisSpectral densityStatistical and Nonlinear PhysicsFilter (signal processing)White noiseCondensed Matter PhysicsMultivariate stochastic analysis; Filter equations; Wind-excited structuresNuclear Energy and EngineeringPhysics::Space PhysicssymbolsStatistical and Nonlinear Physic
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SphinX soft X-ray spectrophotometer: Science objectives, design and performance

2011

The goals and construction details of a new design Polish-led X-ray spectrophotometer are described. The instrument is aimed to observe emission from entire solar corona and is placed as a separate block within the Russian TESIS X- and EUV complex aboard the CORONAS-PHOTON solar orbiting observatory. SphinX uses silicon PIN diode detectors for high time resolution measurements of the solar spectra in the range 0.8–15 keV. Its spectral resolution allows for discerning more than hundred separate energy bands in this range. The instrument dynamic range extends two orders of magnitude below and above these representative for GOES. The relative and absolute accuracy of spectral measurements is e…

Astrophysics::High Energy Astrophysical PhenomenaInstrumentationExtreme ultraviolet lithographyspectrumlaw.inventionX-raySettore FIS/05 - Astronomia E AstrofisicaOpticssolar corona; spectrum; X-ray; abundances; instrumentation; SphinXObservatorylawAstrophysics::Solar and Stellar AstrophysicsSpectral resolutioninstrumentationPhysicsabundanceDynamic rangebusiness.industrysolar coronaSphinXDetectorPIN diodeAstronomy and AstrophysicsSpace and Planetary SciencePhysics::Space PhysicsbusinessOrder of magnitudeSolar System Research
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Polarimetric VLBI observations of 0735+178

2001

We present a new centimeter polarimetric VLBI image of the BL Lac object 0735+178. This source exhibits one of the most pronounced curvatures observed in jets of AGNs, with two sharp apparent bends of 90 degrees within the inner 2 milliarcseconds from the core. Through the analysis of the data gathered over the past decades we study whether this curvature is produced by precession of the jet with ejection of ballistic components, or a precession in such a way that components' velocity vector are always parallel to the jet axis. These possibilities are also studied by comparison with 3D hydrodynamic relativistic simulations of precessing jets.

Astrophysics::High Energy Astrophysical PhenomenaPhysics::Space PhysicsAstrophysics (astro-ph)FOS: Physical sciencesAstrophysics
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Observation of the Cosmic Ray Moon shadowing effect with ARGO-YBJ

2011

Cosmic rays are hampered by the Moon and a deficit in its direction is expected (the so-called \emph{Moon shadow}). The Moon shadow is an important tool to determine the performance of an air shower array. Indeed, the westward displacement of the shadow center, due to the bending effect of the geomagnetic field on the propagation of cosmic rays, allows the setting of the absolute rigidity scale of the primary particles inducing the showers recorded by the detector. In addition, the shape of the shadow permits to determine the detector point spread function, while the position of the deficit at high energies allows the evaluation of its absolute pointing accuracy. In this paper we present th…

Astrophysics::High Energy Astrophysical PhenomenaPhysics::Space PhysicsAstrophysics - High Energy Astrophysical PhenomenaHigh Energy Physics - Experiment
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"Table 12" of "Search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

2018

Selection efficiency for reconstructed photons originating from the decay $a\rightarrow 2\gamma$ with $m_a$ = 2 GeV.

Astrophysics::High Energy Astrophysical PhenomenaPhysics::Space PhysicsHigh Energy Physics::PhenomenologySelection efficiencyHigh Energy Physics::Experiment$pp\rightarrow X \rightarrow aa \rightarrow 4\gamma$Nuclear Experiment13000Photon-jet
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"Table 9" of "Search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

2018

Selection efficiency for reconstructed photons originating from the decay $a\rightarrow 2\gamma$ with $m_a$ = 0.5 GeV.

Astrophysics::High Energy Astrophysical PhenomenaPhysics::Space PhysicsHigh Energy Physics::PhenomenologySelection efficiencyHigh Energy Physics::Experiment$pp\rightarrow X \rightarrow aa \rightarrow 4\gamma$Nuclear Experiment13000Photon-jet
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"Table 11" of "Search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

2018

Selection efficiency for reconstructed photons originating from the decay $a\rightarrow 2\gamma$ with $m_a$ = 1 GeV.

Astrophysics::High Energy Astrophysical PhenomenaPhysics::Space PhysicsHigh Energy Physics::PhenomenologySelection efficiencyHigh Energy Physics::Experiment$pp\rightarrow X \rightarrow aa \rightarrow 4\gamma$Nuclear Experiment13000Photon-jet
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"Table 10" of "Search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

2018

Selection efficiency for reconstructed photons originating from the decay $a\rightarrow 2\gamma$ with $m_a$ = 0.7 GeV.

Astrophysics::High Energy Astrophysical PhenomenaPhysics::Space PhysicsHigh Energy Physics::PhenomenologySelection efficiencyHigh Energy Physics::Experiment$pp\rightarrow X \rightarrow aa \rightarrow 4\gamma$Nuclear Experiment13000Photon-jet
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"Table 8" of "Search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

2018

Selection efficiency for reconstructed photons originating from the decay $a\rightarrow 2\gamma$ with $m_a$ = 0.1 GeV.

Astrophysics::High Energy Astrophysical PhenomenaPhysics::Space PhysicsHigh Energy Physics::PhenomenologySelection efficiencyHigh Energy Physics::Experiment$pp\rightarrow X \rightarrow aa \rightarrow 4\gamma$Nuclear Experiment13000Photon-jet
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"Table 14" of "Search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

2018

Selection efficiency for reconstructed photons originating from the decay $a\rightarrow 2\gamma$ with $m_a$ = 10 GeV.

Astrophysics::High Energy Astrophysical PhenomenaPhysics::Space PhysicsHigh Energy Physics::PhenomenologySelection efficiencyHigh Energy Physics::Experiment$pp\rightarrow X \rightarrow aa \rightarrow 4\gamma$Nuclear Experiment13000Photon-jet
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