Search results for "dron"

showing 10 items of 4363 documents

Anomalous quartic gauge boson couplings at hadron colliders

2000

We analyze the potential of the Fermilab Tevatron and CERN Large Hadron Collider (LHC) to study anomalous quartic vector--boson interactions (photon photon Z Z) and (photon photon W+ W-). Working in the framework of SU(2)_L X U(1)_Y chiral Lagrangians, we study the production of photons pairs accompanied by (e+e-), (e nu), and jet pairs to impose bounds on these new couplings, taking into account the unitarity constraints. We compare our findings with the indirect limits coming from precision electroweak measurements as well as with presently available direct searches at LEPII. We show that the Tevatron Run II can provide limits on these quartic limits which are of the same order of magnitu…

Weak interactions (Nuclear physics)PhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonLarge Hadron ColliderUnitarityAcceleradors de partículesElectron–positron annihilationElectroweak interactionHadronHigh Energy Physics::PhenomenologyInteraccions febles (Física nuclear)TevatronFOS: Physical sciencesPartícules (Física nuclear)Particle acceleratorsNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentFermilabParticle Physics - PhenomenologyParticles (Nuclear physics)
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Resolution of the ATLAS muon spectrometer monitored drift tubes in LHC Run 2

2019

The momentum measurement capability of the ATLAS muon spectrometer relies fundamentally on the intrinsic single-hit spatial resolution of the monitored drift tube precision tracking chambers. Optimal resolution is achieved with a dedicated calibration program that addresses the specific operating conditions of the 354 000 high-pressure drift tubes in the spectrometer. The calibrations consist of a set of timing offsets and drift time to drift distance transfer relations, and result in chamber resolution functions. This paper describes novel algorithms to obtain precision calibrations from data collected by ATLAS in LHC Run 2 and from a gas monitoring chamber, deployed in a dedicated gas fac…

Wire chambers (MWPCdrift tube13000 GeV-cmsPhysics::Instrumentation and DetectorsmuonsTracking (particle physics)01 natural sciences030218 nuclear medicine & medical imagingHigh Energy Physics - ExperimentSubatomär fysikMWPCHigh Energy Physics - Experiment (hep-ex)Gaseous detectors0302 clinical medicineWire chambersDrift tubesSubatomic Physicsscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]tracking detectorProportional chambersmomentum resolutionInstrumentationImage resolutionMathematical Physicsdrift tubesPhysicsLarge Hadron ColliderDrift chamberstrack data analysisMuon spectrometersResolution (electron density)DetectorSettore FIS/01 - Fisica SperimentaleATLAS:Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]Wire chambers (MWPC Thin-gap chambers drift chambers drift tubes proportional chambers etc)medicine.anatomical_structureCERN LHC Collproportional chambers etc)Gaseous detectors; Muon spectrometers; Particle tracking detectors (gaseous detectors); Wire chambers (MWPC thin-gap chambers drift chambers drift tubes proportional chambers etc)MDT chambersWire chambers (MWPC)LHCcolliding beams [p p]Particle Physics - Experimentp p: scatteringspectrometer [muon]Ciências Naturais::Ciências Físicas530 PhysicsParticle tracking detectors (Gaseous detectors):Ciências Físicas [Ciências Naturais]610FOS: Physical sciencesdrift chamber [muon]gas [monitoring]programming03 medical and health sciencesOpticsAtlas (anatomy)Muon spectrometer0103 physical sciencesCalibrationmedicinemuon: drift chamberGaseous detectorddc:610drift chambersHigh Energy Physicsspatial resolutionMuonScience & Technology010308 nuclear & particles physicsbusiness.industryhep-ex:Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431 [VDP]Thin-gap chamberscalibrationmonitoring: gasExperimental High Energy Physicsbusinessp p: colliding beamsmuon: spectrometerexperimental results
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Metallic subnanometer porous silicon: A theoretical prediction

2021

In the present work, T-Si, a silicon-based counterpart of T-carbon, has been designed with the aid of density functional theory (DFT) calculations. Its stability has been fully confirmed from energetic, mechanical, lattice dynamic, and thermodynamic aspects. Due to the space extrusion, the delocalized electrons on the ${\mathrm{Si}}_{4}$ tetrahedrons are squeezed onto the inter-tetrahedron $\mathrm{Si}\ensuremath{-}\mathrm{Si}$ bonds, which therefore leads T-Si to be metallic. Furthermore, the electronic conductivity of this new material has also been predicted and discussed in this work. This new silicon allotrope with a low density of $0.869\mathrm{g}/{\mathrm{cm}}^{3}$ can even floats on…

Work (thermodynamics)Materials scienceCondensed matter physicsSiliconLattice (group)chemistry.chemical_element02 engineering and technology021001 nanoscience & nanotechnologySpace (mathematics)Porous silicon01 natural sciencesDelocalized electronchemistry0103 physical sciencesTetrahedronDensity functional theory010306 general physics0210 nano-technologyPhysical Review B
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Centrality-dependent forward J/ψ production in high energy proton-nucleus collisions

2016

Forward $J/\psi$ production and suppression in high energy proton-nucleus collisions can be an important probe of gluon saturation. In an earlier work we studied this process in the Color Glass Condensate framework and showed that using the Glauber approach to extrapolate the dipole cross section of a proton to a nucleus leads to results closer to experimental data than previous calculations in this framework. Here we investigate the centrality dependence of the nuclear suppression in this model and show a comparison of our results with recent LHC data.

Work (thermodynamics)Particle physicshigh energyNuclear TheoryProtonQC1-999Nuclear Theory114 Physical sciences01 natural sciences7. Clean energyColor-glass condensateNuclear physics0103 physical sciencesmedicineproton-nucleus collisionsNuclear Experiment010306 general physicsPhysicsLarge Hadron Colliderta114010308 nuclear & particles physicsPhysicsGluonHigh Energy Physics - PhenomenologyDipolemedicine.anatomical_structureJ/ψ productionNucleusGlauberInternational Conference on Physics Opportunities at an Electron-Ion Collider
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Mechanism of aluminium incorporation into C–S–H from ab initio calculations

2014

Blended cements have great potential to reduce the CO2 footprint due to cement production. C(alcium)–S(ilicate)–H(ydrate) in these novel materials is known to incorporate a considerable amount of Al. We have for the first time applied large-scale first principles calculations to address the mechanism of Al incorporation into low C/S ratio C–S–H. In agreement with state-of-the-art NMR information, our calculations show that Al substitutes Si in bridging tetrahedra only, and that substitutions in pairing tetrahedra are strongly disfavoured in a wide range of conditions. In broad terms, the energy penalty for having an Al atom in a pairing position is of about 20 kcal mol−1. Al in bridging tet…

Work (thermodynamics)Range (particle radiation)Materials scienceRenewable Energy Sustainability and the Environmentchemistry.chemical_elementThermodynamicsContext (language use)02 engineering and technologyGeneral Chemistry010402 general chemistry021001 nanoscience & nanotechnology01 natural sciences0104 chemical sciencesCrystallographychemistryAluminiumAb initio quantum chemistry methodsPairingAtomTetrahedronGeneral Materials Science[PHYS.PHYS.PHYS-CHEM-PH]Physics [physics]/Physics [physics]/Chemical Physics [physics.chem-ph]0210 nano-technologyComputingMilieux_MISCELLANEOUS
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Local Environment of Yttrium in Y-Doped Barium Cerate Compounds

2006

The local structure of yttrium in Y-doped BaCeO3 compounds was studied using X-ray absorption spectroscopy (XAS) at the Y K-edge. Data analysis shows that the local environment of Y3+ changes, resulting in a distorted octahedron. The structural distortion found does not depend on the dopant amount at the investigated compositions, but on the level of hydration, as clearly demonstrated by the distortion increase in the BaCe0.9Y0.1O3-ä sample after the treatment in O2/H2O. In situ measurements performed in O2/H2O flux, which show that the distortion is retained at 753 K, are also reported. The observed significative structural changes seem to point out a preferential insertion of the hydroxyl…

X-ray absorption spectroscopyMaterials scienceAbsorption spectroscopyDopantGeneral Chemical EngineeringBarium cerate compoundInorganic chemistryDopingAnalytical chemistryX-ray absorption spectroscopychemistry.chemical_elementBariumGeneral MedicineGeneral ChemistryYttriumDistorted octahedronchemistryOctahedronStructural distortionDistortionMaterials ChemistryChemistry of Materials
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Local structure studies of SrTi16O3and SrTi18O3

2014

In this work we report on the local structure of Ti in SrTi 16 O3 (STO16) and SrTi 18 O3 (STO18) investigated in the low temperature range (6‐300K) by extended x-ray absorption fine structure and x-ray absorption near edge structure (XANES) spectroscopy at Ti K-edge and by optical second harmonic generation (SHG). By comparing XANES of STO16 and STO18 we have identified the isotopic effect which produces at T < 100K a noticeable difference in the measured mean square relative displacements (MSRD) of Ti‐O1 bonds: while STO16 follow the expected Einstein-like behavior, for STO18 we have measured an increase of MSRD values with decreasing temperature. This is an indication of an increasing off…

X-ray spectroscopyMaterials scienceAbsorption spectroscopyOctahedronAnalytical chemistrySecond-harmonic generationAtmospheric temperature rangeCondensed Matter PhysicsSpectroscopyAbsorption (electromagnetic radiation)Mathematical PhysicsAtomic and Molecular Physics and OpticsXANESPhysica Scripta
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"Table 5" of "Determination of $alpha_{s}$ in second order {QCD} from hadronic $Z$ decays"

1992

Difference of the heavy and light jet mass.

Z ProductionAstrophysics::High Energy Astrophysical PhenomenaE+ E- --&gt; HADRONSHigh Energy Physics::Phenomenology91.2E+ E- --&gt; Z0 XJet ProductionDSIG/DMASSInclusiveSingle Differential Cross SectionE+ E- --&gt; JET XE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentNuclear Experiment
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"Table 1" of "Determination of $alpha_{s}$ in second order {QCD} from hadronic $Z$ decays"

1992

Experimental differential Thrust distributions.

Z ProductionComputingMethodologies_SIMULATIONANDMODELINGDSIG/DTHRUSTE+ E- --&gt; HADRONSComputerApplications_COMPUTERSINOTHERSYSTEMS91.2E+ E- --&gt; Z0 XJet ProductionComputerSystemsOrganization_PROCESSORARCHITECTURESInclusiveSingle Differential Cross SectionE+ E- --&gt; JET XE+ E- ScatteringComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATIONComputingMilieux_COMPUTERSANDEDUCATIONExclusive
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"Table 8" of "Determination of $alpha_{s}$ in second order {QCD} from hadronic $Z$ decays"

1992

The differential 2-jet rate D2 as a function of YCUT.

Z ProductionE+ E- --&gt; HADRONSIntegrated Cross Section91.2E+ E- --&gt; 2JET XE+ E- --&gt; Z0 XJet ProductionCross SectionSIGInclusiveDijet ProductionE+ E- ScatteringExclusiveR measurement
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