Search results for "scattering [lepton nucleus]"

showing 10 items of 508 documents

Event reconstruction algorithms for the ATLAS trigger

2007

The ATLAS experiment under construction at CERN is due to begin operation at the end of 2007. The detector will record the results of proton-proton collisions at a centerof- mass energy of 14 TeV. The trigger is a three-tier system designed to identify in real-time potentially interesting events that are then saved for detailed offline analysis. The trigger system will select approximately 200 Hz of potentially interesting events out of the 40 MHz bunch-crossing rate (with 109 interactions per second at the nominal luminosity). Algorithms used in the trigger system to identify different event features of interest will be described, as well as their expected performance in terms of selection…

HistoryATLAS experiment01 natural sciencesEducationAtlas (anatomy)0103 physical sciencesmedicine[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsCiencias ExactasEvent reconstructionPhysicsLarge Hadron ColliderLuminosity (scattering theory)ATLAS detectorAlgoritmos010308 nuclear & particles physicsEvent (computing)ATLAS experimentDetectorFísicaATLASComputer Science ApplicationsTriggermedicine.anatomical_structureLHCAlgorithmEnergy (signal processing)
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Hydrogen influence on the structure and properties of amorphous hydrogenated carbon films deposited by direct ion beam

2008

Abstract The present work provides results for amorphous hydrogenated carbon (a-C:H) films grown by direct ion beam deposition method. Acetylene and its mixtures with hydrogen were used. The films were characterized by Rutherford backscattering spectrometry, elastic recoil detection, Raman spectroscopy, ellipsometry, infrared spectroscopy, and microhardness measurements. These techniques indicated that an admixture of hydrogen yields a lower deposition rate, a higher content of total and bounded hydrogen in the a-C:H films, and a lower film density. The optical and mechanical properties depend on both, hydrogen concentrations in the gas phase and in the films, and show a strong diamond-like…

HydrogenChemistryMetals and AlloysAnalytical chemistrychemistry.chemical_elementSurfaces and InterfacesRutherford backscattering spectrometrySurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsAmorphous solidElastic recoil detectionCondensed Matter::Materials ScienceIon beam depositionCarbon filmAmorphous carbonMaterials ChemistryPhysics::Atomic PhysicsThin filmThin Solid Films
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Selective area vapor-phase epitaxy and structural properties of Hg1 − xCdxTe on sapphire

1997

Selective area (SA) Hg1 − xCdxTesapphire layers have been grown using the recently developed technique of the vapor-phase epitaxy (VPE) of Hg1 − xCdxTe layers on CdTesapphire heteroepitaxial substrates (HS), which we have called “VPE on HS technique” (Sochinskii et al., J. Crystal Growth 149 (1995) 35; 161 (1996) 195). First, planar CdTe (1 1 1) 5–7 μm thick layers were grown on sapphire (0 0 0 1) wafers by metalorganic vapor-phase epitaxy (MOVPE) at 340°C for 1–2.5 h using dimethylcadmium and di-isopropyltellurium as precursors. Second, CdTe/sapphire mesas were formed using standard photolithography in the form of alternating parallel linear arrays consisting of 500 × 70 μm2 elements. Thir…

Inorganic ChemistryScanning electron microscopeChemistryMaterials ChemistryAnalytical chemistrySapphireCrystal growthMetalorganic vapour phase epitaxySubstrate (electronics)Condensed Matter PhysicsEpitaxyRutherford backscattering spectrometryCadmium telluride photovoltaicsJournal of Crystal Growth
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Precision luminosity measurements at LHCb

2014

Measuring cross-sections at the LHC requires the luminosity to be determined accurately at each centre-of-mass energy $\sqrt{s}$. In this paper results are reported from the luminosity calibrations carried out at the LHC interaction point 8 with the LHCb detector for $\sqrt{s}$ = 2.76, 7 and 8 TeV (proton-proton collisions) and for $\sqrt{s_{NN}}$ = 5 TeV (proton-lead collisions). Both the "van der Meer scan" and "beam-gas imaging" luminosity calibration methods were employed. It is observed that the beam density profile cannot always be described by a function that is factorizable in the two transverse coordinates. The introduction of a two-dimensional description of the beams improves sig…

Instrumentation for particle accelerators and storage rings - high energy (linear acceleratorsHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)cluster finding[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment06.20.fbInstrumentationMathematical PhysicsQCPhysicsLuminosity (scattering theory)Large Hadron ColliderPattern recognition cluster finding calibration and fitting methodssynchrotrons)DetectorPattern recognition cluster finding calibration and fitting methodsComputer interfacecalibration and fitting methodsFísica nuclearTracking and position-sensitive detectorLHCParticle Physics - ExperimentParticle physics29.40.GxPattern recognition cluster finding calibration and fitting methods; Instrumentation for particle accelerators and storage rings - high energy (linear accelerators synchrotrons)Astrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsLHCb - Abteilung HofmannPattern recognition cluster finding calibration and fitting methodInstrumentation for particle accelerators and storage rings - high energy (linear accelerators synchrotrons)NOConsistency (statistics)Pattern recognitionCalibrationSDG 7 - Affordable and Clean EnergyInstrumentation for particle accelerators and storage rings - high energy (linear accelerators synchrotrons)/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyInteraction pointStandards and calibrationFunction (mathematics)29.50.+vLHCbInstrumentation for particle accelerators and storage rings - high energy (linear accelerators synchrotrons); Pattern recognition cluster finding calibration and fitting methods; Instrumentation; Mathematical PhysicsTEVPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentInstrumentation for particle accelerators and storage rings - high energy (linear accelerators synchrotrons); Pattern recognition cluster finding calibration and fitting methodsEnergy (signal processing)
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Prospects for quarkonium studies at the high-luminosity LHC

2020

Prospects for quarkonium-production studies accessible during the upcoming high-luminosity phases of the CERN Large Hadron Collider operation after 2021 are reviewed. Current experimental and theoretical open issues in the field are assessed together with the potential for future studies in quarkonium-related physics. This will be possible through the exploitation of the huge data samples to be collected in proton-proton, proton-nucleus and nucleus-nucleus collisions, both in the collider and fixed-target modes. Such investigations include, among others, those of: (i) J/psi and Upsilon produced in association with other hard particles; (ii) chi(c,b) and eta(c,b) down to small transverse mom…

J/psi(3100)heavy ion: scatteringgeneralized parton distributionNuclear TheoryProtonNuclear Theorynucleus nucleusparton: distribution functionPartoneta/c(3590)nucl-extransverse momentum dependenceLarge Hadron Collider (LHC)7. Clean energy01 natural sciencesHigh Energy Physics - Experimentlaw.inventionSivers functionHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)lawHigh Luminosity[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]partonNuclear Experiment (nucl-ex)Quarkonium productionNuclear ExperimentNuclear Experimentquark gluon: plasmaPhysicsLarge Hadron ColliderLuminosity (scattering theory)hep-phhighnucleus nucleus: scatteringQuarkoniumheavy ionHigh Energy Physics - PhenomenologyCERN LHC CollNuclear Physics - Theoryluminosity: higheta/c(2980)Particle Physics - ExperimentquarkoniumHigh Luminosity; Large Hadron Collider (LHC); Quarkonium productionNuclear and High Energy PhysicsParticle physicsp p: scatteringsmall-xCERN Labnucl-th[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]collectiveFOS: Physical sciencestransverse momentum[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Theory (nucl-th)0103 physical sciencesNuclear Physics - Experimentluminosity010306 general physicsColliderp nucleus: scatteringquark gluonplasmaParticle Physics - Phenomenology010308 nuclear & particles physicshep-exHigh Energy Physics::PhenomenologyscatteringnucleusgluonGluon[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Quark–gluon plasmaHigh Energy Physics::Experimentp nucleusproduction
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Measuring the differential scattering cross-section of gold nanoparticles - art. no. 70321E

2008

International audience; In this paper we present an experimental apparatus capable of measuring the differential scattering cross sections of individual nanoparticles and arrangement of nanoparticles. We show that the mapping a partial differential scattering cross section, qualitative information about the electromagnetic local density of states dominated by evanescent modes scattered by the structure can be obtained.

LDOS[SPI.OPTI] Engineering Sciences [physics]/Optics / Photonic[SPI.NANO] Engineering Sciences [physics]/Micro and nanotechnologies/MicroelectronicsSurface plasmon[SPI.OPTI]Engineering Sciences [physics]/Optics / PhotonicPhysics::OpticsMetal nanoparticles[ SPI.NANO ] Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics[ SPI.OPTI ] Engineering Sciences [physics]/Optics / Photonic[SPI.NANO]Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronicsdifferential scattering cross section
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Performance of ATLAS tracking detector

2012

The track and vertex reconstruction algorithms of the ATLAS Inner Detector have demonstrated excellent performance in the early data from the LHC. However, the rapidly increas- ing number of interactions per bunch crossing introduces new challenges both in computational aspects and physics performance. The combination of both silicon and gas based detectors provides high precision impact parameter and momentum measurement of charged particles, with high efficiency and small fake rate. Vertex reconstruction is used to identify with high efficiency the hard scattering process and to measure the amount of pile-up interactions, both aspects are cru- cial for many physics analyses. The performan…

Large Hadron ColliderAtlas (topology)Computer scienceDetectorScattering processImpact parameterDetectors and Experimental TechniquesImage resolutionCharged particleComputational science
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Upgrade of ALICE forward detectors

2019

ALICE will upgrade its subsystems in 2019−2020 to fully benefit from the increased collision rate and luminosity of the LHC at CERN. Two new forward detectors will be installed at the core of ALICE: the Fast Interaction Trigger (FIT) and the Muon Forward Tracker (MFT). Additionally, during the shutdown between Run 3 and Run 4, there will be an opportunity to install the Forward Calorimeter (FoCal). This paper describes these new forward detectors, their physics justification and goals, selected design features along with performance of detector prototypes and simulated performance figures. peerReviewed

Large Hadron ColliderLuminosity (scattering theory)Calorimeter (particle physics)Physics::Instrumentation and DetectorsComputer sciencebusiness.industrydesign features simulated performancetutkimuslaitteetDetectorElectrical engineeringhiukkasfysiikkaUpgradePhysics::Accelerator PhysicsHigh Energy Physics::Experimentcollision rateDetectors and Experimental TechniquesALICE (propellant)businessCollision rateProceedings of The 39th International Conference on High Energy Physics — PoS(ICHEP2018)
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Structure and characteristics of laser crystallized thin amorphous Si films

2011

Abstract Pure amorphous Si thin films deposited on oxidized crystalline Si surface (111) were crystallized by picosecond UV laser pulses. The Raman scattering spectra show that pulse energy of 330 mJ/cm2 is enough to fully crystallize Si film and further increase of the energy does not improve crystallinity. A large grained polycrystalline Si was obtained as revealed by surface analysis. A significant increase in carrier mobility was observed after laser crystallization.

Laser crystallizationElectron mobilityMaterials scienceAnalytical chemistryPhysics::OpticsP-SiLasereye diseasesAmorphous solidlaw.inventionCondensed Matter::Materials ScienceCrystallinityCrystallographyEnergy(all)lawCondensed Matter::SuperconductivityPicosecondsense organsCrystalliteA-SiAFMThin filmEnergy (signal processing)Raman scattering spectraEnergy Procedia
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Dependence of two-proton radioactivity on nuclear pairing models

2017

Sensitivity of two-proton emitting decay to nuclear pairing correlation is discussed within a time-dependent three-body model. We focus on the $^6$Be nucleus assuming $\alpha + p + p$ configuration, and its decay process is described as a time-evolution of the three-body resonance state. For a proton-proton subsystem, a schematic density-dependent contact (SDDC) pairing model is employed. From the time-dependent calculation, we observed the exponential decay rule of a two-proton emission. It is shown that the density dependence does not play a major role in determining the decay width, which can be controlled only by the asymptotic strength of the pairing interaction. This asymptotic pairin…

Light nucleusNuclear TheoryNuclear TheoryFOS: Physical sciences01 natural sciences114 Physical sciencesDECAYSNuclear Theory (nucl-th)symbols.namesakeENERGY-LEVELSLIMITS0103 physical sciencesmedicineExponential decayNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysicsta114010308 nuclear & particles physicsQUASI-STATIONARY STATEproton emissionTime evolutionwidthsnuclear forcesScattering lengthDRIP-LINEmedicine.anatomical_structureLIGHT-NUCLEIDensity distributionPairing3-BODY SYSTEMfew-body systemssymbolslifetimesAtomic physicsHamiltonian (quantum mechanics)Nucleus
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