Search results for "scattering [electron hadron]"

showing 10 items of 654 documents

Yangian Symmetry for Fishnet Feynman Graphs

2017

Various classes of fishnet Feynman graphs are shown to feature a Yangian symmetry over the conformal algebra. We explicitly discuss scalar graphs in three, four and six spacetime dimensions as well as the inclusion of fermions in four dimensions. The Yangian symmetry results in novel differential equations for these families of largely unsolved Feynman integrals. Notably, the considered fishnet graphs in three and four dimensions dominate the correlation functions and scattering amplitudes in specific double scaling limits of planar, gamma-twisted N=4 super Yang-Mills or ABJM theory. Consequently, the study of fishnet graphs allows us to get deep insights into the integrability of the plana…

High Energy Physics - Theorydimension: 4Feynman graphScalar (mathematics)[PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph]FOS: Physical sciencesConformal mapintegrability01 natural sciencesalgebra: conformal[ PHYS.HTHE ] Physics [physics]/High Energy Physics - Theory [hep-th]symbols.namesake0103 physical sciencesFeynman diagramcorrelation function010306 general physicsABJM modelMathematical PhysicsMathematical physicsPhysicsfield theory: conformalSpacetimeAdS/CFT correspondence010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]Mathematical analysisscattering amplitudescalingdifferential equationsMathematical Physics (math-ph)FermionScattering amplitudespace-time: dimension: 6AdS/CFT correspondenceHigh Energy Physics - Theory (hep-th)symmetry: Yangiansupersymmetry: 4symbols[ PHYS.MPHY ] Physics [physics]/Mathematical Physics [math-ph]Yangian
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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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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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Calibrating the effective scattering albedo in the SMOS algorithm: some first results

2016

International audience; This study focuses on the calibration of the effective scattering albedo (ω) of vegetation in the soil moisture (SM) retrieval at L-Band. Currently, in the SMOS Level 2 and 3 algorithms, the value of ω is set to 0 for low vegetation and ∼ 0.06 – 0.08 for forests. Different parameterizations of vegetation (in terms of ω values) were tested in this study. The possibility of combining soil roughness and vegetation contributions as a single parameter (“combined” method) leads to an important simplification in the algorithm and was also evaluated here. Following these assumptions, retrieved values of SMOS SM were compared with SM data measured over many in situ sites worl…

L band010504 meteorology & atmospheric sciencesPixelScattering0211 other engineering and technologies[SDU.STU]Sciences of the Universe [physics]/Earth SciencesSingle parameter02 engineering and technologyVegetationSMAP15. Life on landAlbedo01 natural sciencesscattering albedoCalibrationEnvironmental sciencesoil moistureL-MEB modelAlgorithmWater content[SPI.SIGNAL]Engineering Sciences [physics]/Signal and Image processing021101 geological & geomatics engineering0105 earth and related environmental sciencesRemote sensingSMOS
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Incidence Angle Diversity on L-Band Microwave Radiometry and Its Impact on Consistent Soil Moisture Retrievals

2021

Incidence angle diversity of space-borne L-band radiometers needs to be taken into account for a consistent estimation of surface soil moisture (SM). In this study, the Land Parameter Retrieval Model (LPRM) is applied to SMOS brightness temperatures to calibrate the effective scattering albedo (w) and the soil roughness (h 1 ) parameter against ERA5-land SM. The analysis is carried out for SMOS data at three different incidence angles ( 32.5±5∘, 42.5±5∘ and 52.5±5∘ ) focusing in 2016 on the three main land cover types of the Iberian Peninsula according to the Climate Change Initiative (agricultural, forest and grassland). The parameterization shows an increasing trend of w and h 1 with rise…

L bandBrightnessmicrowaveincidence angleScattering albedoradiometryLand coverAtmospheric sciencesMicroonesmulti-angularMicrowavesWater contentRadiometerScattering:Enginyeria de la telecomunicació [Àrees temàtiques de la UPC]AlbedoL-bandSatèl·lits artificials en teledeteccióEnvironmental scienceSoil moistureRoughness and incidence angle diversitysoil moistureMicrowave radiometryLPRMArtificial satellites in remote sensingSMOS
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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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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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Time-variations of zeroth-order vegetation absorption and scattering at L-band

2021

Abstract Surface soil moisture and vegetation optical depth (VOD), as an indicator of vegetation wet biomass, from passive microwave remote sensing have been increasingly applied in global ecology and climate research. Both soil moisture and VOD are retrieved from satellite brightness temperature measurements assuming a zeroth order radiative transfer model, commonly known as the tau-omega model. In this model the emission of a vegetated surface is dependent on soil moisture, vegetation absorption and vegetation scattering. Vegetation scattering is normally represented by the single scattering albedo, ω, and is commonly assumed to be a time-invariant calibration parameter to achieve high ac…

LidarScatteringSingle-scattering albedoAttenuationeffective scattering albedoSoil ScienceGeologySoil scienceContext (language use)SMAPradiometryVegetationvegetation optical depthICESat-2L-bandAtmospheric radiative transfer codesBrightness temperaturerelative canopy scatteringEnvironmental scienceComputers in Earth SciencesAbsorption (electromagnetic radiation)relative canopy absorptionRemote sensingRemote Sensing of Environment
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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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