Search results for "Physics::Geophysics"

showing 10 items of 261 documents

Optimization of image parameters using a hyperspectral library application to soil identification and moisture estimation

2009

The growing number of sensors raises questions about the image parameters required for the application, soil identification and moisture estimation. Hyperspectral images are also known to contain highly redundant information. Hence not all the spectral bands are needed for the satisfactory classification of the soil types. Hence, the work was aimed at obtaining these optimal spectral bands for identifying the soil types and to use these spectral bands to estimate the moisture content of the soils using the method proposed by Whiting et.al.

Identification (information)MoistureSoil waterEnvironmental scienceHyperspectral imagingFeature selectionSoil classificationSpectral bandsWater contentPhysics::GeophysicsRemote sensing2009 IEEE International Geoscience and Remote Sensing Symposium
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The weak mixing angle from low energy neutrino measurements: A global update

2016

Taking into account recent theoretical and experimental inputs on reactor fluxes we reconsider the determination of the weak mixing angle from low energy experiments. We perform a global analysis to all available neutrino-electron scattering data from reactor antineutrino experiments, obtaining sin^2(theta_W) = 0.252 \pm 0.030. We discuss the impact of the new theoretical prediction for the neutrino spectrum, the new measurement of the reactor antineutrino spectrum by the Daya Bay collaboration, as well as the effect of radiative corrections. We also reanalyze the measurements of the nu_e-e cross section at accelerator experiments including radiative corrections. By combining reactor and ac…

ImaginationNuclear and High Energy Physicsmedia_common.quotation_subjectFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentPhysics::GeophysicsNuclear physicsHigh Energy Physics - Experiment (hep-ex)Cross section (physics)High Energy Physics - Phenomenology (hep-ph)Low energy0103 physical sciencesRadiative transfer010306 general physicsMixing (physics)media_commonPhysics010308 nuclear & particles physicsScatteringWeinberg anglelcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNeutrinolcsh:PhysicsPhysics Letters B
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Feasibility study for a nanosatellite-based instrument for in-situ measurements of radio noise

2015

The radio environment on the earth is heavily affected by manmade sources such as radio transmissions, radars, and the like. The effect is particularly strong at MF frequencies and below, since the signals can propagate large distances via ionospheric bounce. Terrestrial magnetometer measurements have long been used to predict the Kp index, which is related to radio transmission at these ranges. Space weather measurements and models can also predict propagation of MF signals on the ground.

In situRadio transmissionMeteorologyMagnetometerlawPhysics::Space PhysicsEnvironmental scienceSpace weatherIonospherePhysics::GeophysicsRadio waveRemote sensinglaw.invention2015 1st URSI Atlantic Radio Science Conference (URSI AT-RASC)
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"Table 26" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Difference of the Hemisphere Broadening, BDIFF. Corrected to final state particles.

InclusiveDN/DBDIFFE+ E- --> NEUTRAL XE+ E- ScatteringE+ E- --> CHARGED XDN/DDBDIFF91.2Astrophysics::Earth and Planetary AstrophysicsSingle Differential DistributionPhysics::Atmospheric and Oceanic PhysicsPhysics::Geophysics
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"Table 23" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Wide Hemisphere Broadening, BMAX. Corrected to final state particles.

InclusiveDN/DBMAXE+ E- --> NEUTRAL XE+ E- ScatteringDN/DDBMAXE+ E- --> CHARGED X91.2Astrophysics::Earth and Planetary AstrophysicsSingle Differential DistributionPhysics::Atmospheric and Oceanic PhysicsPhysics::Geophysics
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"Table 20" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Heavy-Hemisphere-Mass distribution. Corrected to final state particles.

InclusiveDN/DHEAVY-HEMISPHERE-MASSE+ E- --> NEUTRAL XE+ E- ScatteringHigh Energy Physics::PhenomenologyE+ E- --> CHARGED X91.2Astrophysics::Earth and Planetary AstrophysicsSingle Differential DistributionNuclear ExperimentPhysics::Atmospheric and Oceanic PhysicsPhysics::Geophysics
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"Table 22" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Difference in Hemisphere Masses. Corrected to final state particles.

InclusiveE+ E- --> NEUTRAL XE+ E- ScatteringE+ E- --> CHARGED X91.2Astrophysics::Earth and Planetary AstrophysicsSingle Differential DistributionPhysics::Atmospheric and Oceanic PhysicsPhysics::GeophysicsDN/DM**2/ELVIS**2
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"Table 25" of "Tuning and test of fragmentation models based on identified particles and precision event shape data."

1996

Total Hemisphere Broadening, BSUM. Corrected to final state particles.

InclusiveE+ E- --> NEUTRAL XE+ E- ScatteringE+ E- --> CHARGED XDN/DBSUM91.2Astrophysics::Earth and Planetary AstrophysicsSingle Differential DistributionDN/DDBSUMPhysics::Atmospheric and Oceanic PhysicsPhysics::Geophysics
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A comparison of numerical surface topography calculations in geodynamic modelling: an evaluation of the ‘sticky air’ method

2012

SUMMARY Calculating surface topography in geodynamic models is a common numerical problem. Besides other approaches, the so-called ‘sticky air’ approach has gained interest as a free-surface proxy at the top boundary. The often used free slip condition is thereby vertically extended by introducing a low density, low viscosityfluid layer. This allows the air/crust interface to behave in a similar manner to a true free surface. We present here a theoretical analysis that provides the physical conditions under which the sticky air approach is a valid approximation of a true free surface. Two cases are evaluated that characterize the evolution of topography on different timescales: (1) isostati…

Length scale010504 meteorology & atmospheric sciencesFinite differenceEulerian pathGeophysicsSlip (materials science)Mechanics010502 geochemistry & geophysics01 natural sciencesFinite element methodPhysics::GeophysicsPlumesymbols.namesakeGeophysicsGeochemistry and PetrologyFree surfacesymbolsAnisotropyPhysics::Atmospheric and Oceanic PhysicsGeology0105 earth and related environmental sciencesGeophysical Journal International
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Method to find the Minimum 1D Linear Gradient Model for Seismic Tomography

2016

The changes in the state of a geophysical medium before a strong earthquake can be found by studying of 3D seismic velocity images constructed for consecutive time windows. A preliminary step is to see changes with time in a minimum 1D model. In this paper we develop a method that finds the parameters of the minimum linear gradient model by applying a two-dimensional Taylor series of the observed data for the seismic ray and by performing least-square minimization for all seismic rays. This allows us to obtain the mean value of the discrete observed variable, close to zero value.

Local earthquake tomography02 engineering and technology010502 geochemistry & geophysics01 natural sciencesTheoretical Computer SciencePhysics::Geophysicssymbols.namesakeTime windowsLinear gradient of velocity0202 electrical engineering electronic engineering information engineeringTaylor series0105 earth and related environmental sciencesAlgebra and Number TheoryZero (complex analysis)State (functional analysis)GeodesyLinear gradientVariable (computer science)Computational Theory and MathematicsLíkönSeismic tomographysymbols020201 artificial intelligence & image processingMinificationJarðskjálftarMinimum 1D modelGeologyJarðskjálftamælingarInformation Systems
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