Search results for "DISTRIBUTIONS"

showing 10 items of 214 documents

Scaling laws of strategic behavior and size heterogeneity in agent dynamics

2008

The dynamics of many socioeconomic systems is determined by the decision making process of agents. The decision process depends on agent's characteristics, such as preferences, risk aversion, behavioral biases, etc.. In addition, in some systems the size of agents can be highly heterogeneous leading to very different impacts of agents on the system dynamics. The large size of some agents poses challenging problems to agents who want to control their impact, either by forcing the system in a given direction or by hiding their intentionality. Here we consider the financial market as a model system, and we study empirically how agents strategically adjust the properties of large orders in orde…

Physics - Physics and SocietyStatistical Finance (q-fin.ST)Computer scienceORIGINAggregate (data warehouse)Financial marketComplex systemQuantitative Finance - Statistical FinanceFOS: Physical sciencesTime horizonPhysics and Society (physics.soc-ph)FLUCTUATIONSInvestment (macroeconomics)FOS: Economics and businessFINANCIAL MARKETPRICESOrder (exchange)EconometricsDISTRIBUTIONSPreference (economics)Scaling
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Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at √s = 7 TeV with the ATLAS detector

2011

The inclusive and dijet production cross-sections have been measured for jets containing b-hadrons (b-jets) in proton–proton collisions at a centre-of-mass energy of √s =7 TeV, using the ATLAS detector at the LHC. The measurements use data corresponding to an integrated luminosity of 34 pb[superscript −1]. The b-jets are identified using either a lifetime-based method, where secondary decay vertices of b-hadrons in jets are reconstructed using information from the tracking detectors, or a muon-based method where the presence of a muon is used to identify semileptonic decays of b-hadrons inside jets. The inclusive b-jet cross-section is measured as a function of transverse momentum in the ra…

Physics and Astronomy (miscellaneous)01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Invariant massNuclear ExperimentDetectors de radiacióPhysicsQuantum chromodynamicsLarge Hadron ColliderLuminosity (scattering theory)dijet cross-sections; b-jets; pp collisions; ATLAS detectorAcceleradors de partículesSettore FIS/01 - Fisica SperimentaleATLASP(P)Over-Bar Collisionsmedicine.anatomical_structurePhysical SciencesLHCParticle Physics - ExperimentSemileptonic decayParticle physicsCiências Naturais::Ciências FísicasAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Nuclear physicsAtlas (anatomy)0103 physical sciencesmedicineFysikRapidityddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Ciencias ExactasScience & TechnologyMuonBottom-Quark ProductionATLAS detectorParton Distributions010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicab-jetsHigh Energy Physics::Experimentproton-proton collisionsDecays
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Measurement of the jet fragmentation function and transverse profile in proton-proton collisions at a center-of-mass energy of 7 TeV with the ATLAS d…

2011

The jet fragmentation function and transverse profile for jets with 25 GeV<pT jet<500 GeV and |ηjet|<1.2 produced in proton–proton collisions with a center-of-mass energy of 7 TeV are presented. The measurement is performed using data with an integrated luminosity of 36 pb−1. Jets are reconstructed and their momentum measured using calorimetric information. The momenta of the charged particle constituents are measured using the tracking system. The distributions corrected for detector effects are compared with various Monte Carlo event generators and generator tunes. Several of these choices show good agreement with the measured fragmentation function. None of these choices reproduce both t…

Physics and Astronomy (miscellaneous)Atlas detectorMonte Carlo methodKinematics7. Clean energy01 natural sciencesScaling ViolationsHigh Energy Physics - ExperimentScatteringHigh Energy Physics - Experiment (hep-ex)jet fragmentation[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentPhysicsSettore FIS/01 - Fisica SperimentaleDetectorATLASCharged particleTransverse planePhysical SciencesQuarkFísica nuclearDistributionsLHCParticle Physics - ExperimentParticle physics530 PhysicsCiências Naturais::Ciências FísicasAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]jet fragmentation function; proton–proton collisions; ATLAS detectorFOS: Physical sciencesAnnihilationddc:500.2530Nuclear physicsQ2 Dependence0103 physical sciencesFragmentation functionFysikddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Ciencias ExactasHeraScience & TechnologyATLAS detector010308 nuclear & particles physicsFísicaQCDproton-proton collisionsHigh Energy Physics::Experiment
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Measurement of the inclusive jet cross-section in pp collisions at $\sqrt{s}=2.76\ \mbox{TeV}$ and comparison to the inclusive jet cross-section at $…

2013

The inclusive jet cross-section has been measured in proton-proton collisions at sqrt(s)=2.76 TeV in a dataset corresponding to an integrated luminosity of 0.20pb-1 collected with the ATLAS detector at the Large Hadron Collider in 2011. Jets are identified using the anti-kt algorithm with two radius parameters of 0.4 and 0.6. The inclusive jet double-differential cross-section is presented as a function of the jet transverse momentum pT and jet rapidity y, covering a range of 20 &lt;= pT &lt; 430 GeV and |y| &lt; 4.4. The ratio of the cross-section to the inclusive jet cross-section measurement at sqrt(s)=7 TeV, published by the ATLAS Collaboration, is calculated as a function of both trans…

Physics and Astronomy (miscellaneous)Cern Pbarp ColliderCiencias FísicasMonte Carlo methodParton01 natural sciences7. Clean energyHigh Energy Physics - ExperimentEp Scattering//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)PhysicsLarge Hadron ColliderSettore FIS/01 - Fisica SperimentalePerturbative QCDATLASPerturbation-TheoryINCLUSIVE JET CROSS SECTIONPhysical SciencesLHCCIENCIAS NATURALES Y EXACTASParticle Physics - ExperimentParticle physicsShowersCiências Naturais::Ciências Físicas530 PhysicsAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesFísica de Partículas y CamposNuclear physicsDeep-Inelastic ScatteringFragmentation0103 physical sciencesFysikRapidityddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Science & Technology010308 nuclear & particles physicsParton DistributionsFísica//purl.org/becyt/ford/1.3 [https]Deep inelastic scatteringDistribution function(P)over-Bar-P CollisionsHADRON-HADRON COLLISIONSExperimental High Energy PhysicsHigh Energy Physics::ExperimentDimensionless quantityModelThe European Physical Journal C
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Measurement of the flavour composition of dijet events in pp collisions at √s = 7 TeV with the ATLAS detector

2013

This paper describes a measurement of the flavour composition of dijet events produced in pp collisions at s√=7~TeVs=7~TeV using the ATLAS detector. The measurement uses the full 2010 data sample, corresponding to an integrated luminosity of 39 pb−1. Six possible combinations of light, charm and bottom jets are identified in the dijet events, where the jet flavour is defined by the presence of bottom, charm or solely light flavour hadrons in the jet. Kinematic variables, based on the properties of displaced decay vertices and optimised for jet flavour identification, are used in a multidimensional template fit to measure the fractions of these dijet flavour states as functions of the leadin…

Physics and Astronomy (miscellaneous)Ciencias FísicasHadronFlavourNuclear physics01 natural sciencesHigh Energy Physics - ExperimentLuminosity (scattering theory)//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)Ciencias Naturales y ExactasNaturvetenskap[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Charm (quantum number)Nuclear ExperimentQCPhysicsJet (fluid)Luminosity (scattering theory)PhysicsSettore FIS/01 - Fisica SperimentaleParticle physicsCross-SectionATLASmedicine.anatomical_structureComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCNatural SciencesParticle Physics - ExperimentParticle physics530 PhysicsCiências Naturais::Ciências FísicasAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2Física de Partículas y Campos530GluonNuclear physicsAtlas (anatomy)Jet (fluid)0103 physical sciencesmedicineCharm (quantum number)Rapidityddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)Hadron-Hadron ScatteringScience & Technology010308 nuclear & particles physicsParton DistributionsHigh Energy Physics::PhenomenologyFísica//purl.org/becyt/ford/1.3 [https]GluonJETHADRON-HADRON COLLISIONSHadronExperimental High Energy PhysicsFlavourRapidityHigh Energy Physics::ExperimentFLAVORColliderEuropean Physical Journal C
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Spin distribution measurement for 64Ni + 100Mo at near and above barrier energies

2015

Spin distribution measurements were performed for the reaction 64 Ni + 100 Mo at three beam energies ranging from 230 to 260 MeV. Compound nucleus (CN) spin distributions were obtained channel selective for each evaporation residue populated by the de-excitation cascade. A comparison of the spin distribution at different beam energies indicates that its slope becomes steeper and steeper with increasing beam energy. This change in slope of the spin distribution is mainly due to the onset of fission competition with particle evaporation at higher beam energies.

PhysicsFissionPhysicsQC1-999fusion reactions ; spin distributionsEvaporation7. Clean energyDistribution (mathematics)CascadeParticlePhysics::Accelerator PhysicsCondensed Matter::Strongly Correlated ElectronsAtomic physicsBeam energyBeam (structure)Spin-½EPJ Web of Conferences
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Invariant mass spectrum and α-n correlation function studied in the fragmentation of 6He on a carbon target

1998

13 pags, 5 figures.-- PACS nrs.: 24.60.−t; 25.70.Ef; 27.20.+n.

PhysicsNuclear and High Energy PhysicsReaction mechanismMomentum distributionsBreakupSpectral lineIon[PACS] Reactions induced by unstable nucleiBreakup reactions6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Fragmentation (mass spectrometry)Halo nucleiFragmentation mechanism[PACS] ResonancesSecondary radioactive beamsInvariant massNeutronHe-5He-6Invariant mass spectra[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Atomic physicsGround stateExotic nucleiNuclear Physics A
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Searching for the 5H resonance in the t+n+n system

2003

19 pages, 7 figures, 2 tables, 2 appendices.-- PACS nrs.: 27.10.+h; 25.60.Gc.-- Printed version published Jul 28, 2003.

PhysicsNuclear reactionNuclear and High Energy PhysicsComparisons with previous resultsMeasured triton and neutron relative energy spectra energy and angular correlationsHyperspherical harmonic expansion analysisResonance[PACS] Properties of specific nuclei listed by mass ranges: A ≤ 5Nuclear Reactions C(6Hent) (6He2nt) E=240 MeV/nucleonNuclear physicsNuclear magnetic resonanceA ≤ 5 [[PACS] Properties of specific nuclei listed by mass ranges]45H deduced resonance features[PACS] Breakup and momentum distributionsNuclear Physics A
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Quark model predictions for the SU(6)-breaking ratio of the proton momentum distributions

2003

The ratio between the anomalous magnetic moments of proton and neutron has been recently parametrized by the ratio of proton momentum fractions $M_{2}^{q_{val}}$. This ratio is evaluated using different constituent quark models, starting from the CQM density distributions and calculating the next-to leading order distributions. We show that this momentum fractions $M_{2}^{q_{val}}$ ratio is a sensitive test for SU(6)-breaking effects and therefore it is useful to distinguish among different CQMs. We investigate also the possibility of getting constraints on the formulation of quark structure models.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsNuclear TheoryProtonMagnetic momentParton distributionsNuclear TheoryQuark modelFOS: Physical sciencesConstituent quarkOrder (ring theory)Constituent quark modelsHadronsNuclear Theory (nucl-th)MomentumSU(6)PartonsPhysics Letters B
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Partially time invariant panel data regression

2023

When dealing with panel data, considering the variation over time of the variable of interest allows to get rid of potential individual effects. Even though the outcome variable has a continuous distribution, its variation over time can be equal to zero with a strictly positive probability and thus its distribution is a mixture of a mass at zero and a continuous distribution. We introduce a parametric statistical model based on conditional mixtures, build estimators for the parameters related to the conditional probability of no variation and to the conditional expectation related to the continuous part of the distribution and derive their asymptotic consistency and normality under a specif…

Policy EvaluationZero InflationMixture of DistributionsPanel DataBootstrapHeterogeneous Treatment Effects[STAT] Statistics [stat]
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