Search results for "lider"

showing 10 items of 1757 documents

Effects of shadowing on Drell-Yan dilepton production in high energy nuclear collisions

2001

We compute cross sections for the Drell-Yan process in nuclear collisions at next-to-leading order (NLO) in ��_s. The effects of shadowing on the normalization and on the mass and rapidity dependence of these cross sections are presented. An estimate of higher order corrections is obtained from next-to-next-to-leading order (NNLO) calculation of the rapidity-integrated mass distribution. Variations in these predictions resulting from choices of parton distribution sets are discussed. Numerical results for mass distributions at NLO are presented for RHIC and LHC energies, using appropriate rapidity intervals. The shadowing factors in the dilepton mass range 2 < M < 10 GeV are predicted…

Normalization (statistics)PhysicsNuclear and High Energy PhysicsParticle physicsHigh energyLarge Hadron ColliderMass distributionHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and AstronomyPartonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)RapidityHigh Energy Physics::ExperimentNuclear Experiment
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The importance of kinematic twists and genuine saturation effects in dijet production at the Electron-Ion Collider

2021

We compute the differential yield for quark anti-quark dijet production in high-energy electron-proton and electron-nucleus collisions at small $x$ as a function of the relative momentum $\boldsymbol{P}_\perp$ and momentum imbalance $\boldsymbol{k}_\perp$ of the dijet system for different photon virtualities $Q^2$, and study the elliptic and quadrangular anisotropies in the relative angle between $\boldsymbol{P}_\perp$ and $\boldsymbol{k}_\perp$. We review and extend the analysis in [1], which compared the results of the Color Glass Condensate (CGC) with those obtained using the transverse momentum dependent (TMD) framework. In particular, we include in our comparison the improved TMD (ITMD…

Nuclear Theoryquark antiquarkQC770-798hiukkasfysiikkaPROTONtransverse momentum dependence01 natural scienceslaw.inventionColor-glass condensateGLUON DISTRIBUTION-FUNCTIONSHigh Energy Physics - Phenomenology (hep-ph)lawEQUATIONSaturation (graph theory)Wave functionPhysicselectron nucleon: colliding beamsQUARK PAIR PRODUCTIONFLUCTUATIONSQCD PhenomenologyQCD phenomenologyHigh Energy Physics - PhenomenologykinematicstwistPhysics::Space PhysicsProduction (computer science)Quarkdijet: productionCOLLISIONSNuclear and High Energy PhysicsParticle physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciencesanisotropy114 Physical sciencesdihadron: angular correlationdeep inelastic scattering (phenomenology)AZIMUTHAL CORRELATIONSMomentumelectron p: scatteringNuclear Theory (nucl-th)Nuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesWAVE-FUNCTIONS010306 general physicsColliderDeep Inelastic Scattering (Phenomenology)010308 nuclear & particles physicselectron nucleus: scatteringHigh Energy Physics::PhenomenologyEVOLUTIONGluon[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]gluon: saturationcolor glass condensateHigh Energy Physics::ExperimentkvanttiväridynamiikkaJournal of High Energy Physics
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Dielectron production in proton-proton and proton-lead collisions at √sNN=5.02TeV

2020

The first measurements of dielectron production at midrapidity (|ηe| < 0.8) in proton–proton and proton–lead collisions at √sNN = 5.02 TeV at the LHC are presented. The dielectron cross section is measured with the ALICE detector as a function of the invariant mass mee and the pair transverse momentum pT, ee in the ranges mee < 3.5 GeV/c2 and pT, ee < 8 GeV/c, in both collision systems. In proton–proton collisions, the charm and beauty cross sections are determined at midrapidity from a fit to the data with two different event generators. This complements the existing dielectron measurements performed at √s = 7 and 13 TeV. The slope of the √s dependence of the three measurements is…

Nuclear and High Energy Physics:Kjerne- og elementærpartikkelfysikk: 431 [VDP]ProtonHadronNuclear Theorydielectrondielectron production01 natural sciences7. Clean energyNuclear physicshadron-ion interactionshadron-hadron collisions; dielectron production;Ionic Collisionsdielectron cross sectiondielectron nuclear modification factor0103 physical sciencesInvariant massDielectronCharm (quantum number)Dielectron; hadron-hadron interactions; hadron-ion interactionsPhysics::Atomic PhysicsIonic Collisions; Relativistic Heavy-ion Collisions; Quark-Gluon Plasma010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsLarge Hadron Collider010308 nuclear & particles physicsPhysicsVDP::Kjerne- og elementærpartikkelfysikk: 431hadron-hadron interactionNuclear matterhadron-hadron collisionsNATURAL SCIENCES. Physics.ALICE LHC proton-lead collisions proton-proton collisionsPRIRODNE ZNANOSTI. Fizika.:Nuclear and elementary particle physics: 431 [VDP]VDP::Nuclear and elementary particle physics: 431dielectron ; LHC ; dielectron cross section ; dielectron nuclear modification factorQuark–gluon plasmaQuark-Gluon PlasmaHigh Energy Physics::ExperimentLHChadron-hadron interactionsRelativistic Heavy-ion Collisions
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Neutron capture cross section measurements for nuclear astrophyisics at CERN n_TOF

2005

A series of neutron capture cross section measurements of interest to nuclear astrophysics have been recently performed at n_TOF, the neutron spallation source operating at CERN. The low repetition frequency of the proton beam driver, the extremely high instantaneous neutron flux, and the low background conditions in the experimental area are optimal for capture cross section measurements on low-mass or radioactive samples. An overview of the measurements performed during the two experimental campaigns in 2002 and 2003 is presented with special emphasis on the measurement of the capture cross sections of the Os isotopes relevant for the cosmochronology based on the Re/Os clock. http://www.s…

Nuclear and High Energy PhysicsAstrofísica nuclearNeutron cross sectionsProtonAstrophysics::High Energy Astrophysical PhenomenaNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNeutrons -- SeccionsNuclear physicsCross section (physics)Neutron flux0103 physical sciencesNeutron cross sectionNuclear astrophysicsSpallationNeutron010306 general physicsNuclear ExperimentPhysicsNeutronsLarge Hadron Collider:Física [Àrees temàtiques de la UPC]010308 nuclear & particles physicsRadioactivityPhysics::Accelerator PhysicsNuclear astrophysicsFísica nuclear
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Neutron measurements for advanced nuclear systems: The n_TOF project at CERN

2012

A few years ago, the neutron time-of-flight facility n_TOF was built at CERN to address some of the urgent needs of high-accuracy nuclear data for Accelerator Driven Systems and other advanced nuclear energy systems, as well as for nuclear astrophysics and fundamental nuclear physics. Thanks to the characteristics of the neutron beam, and to state-of-the-art detection and acquisition systems, high quality neutron cross-section data have been obtained for a variety of isotopes, many of which radioactive. Following an important upgrade of the spallation target and of the experimental area, a new measurement campaign has started last year. After a brief review of the most important results obt…

Nuclear and High Energy PhysicsAstrofísica nuclearNuclear engineeringNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyNuclear physics0103 physical sciencesNuclear astrophysicsSpallationNeutron010306 general physicsNuclear ExperimentInstrumentationPhysics:Energies::Energia nuclear [Àrees temàtiques de la UPC]NeutronsLarge Hadron Collider:Física [Àrees temàtiques de la UPC]010308 nuclear & particles physicsNuclear fissionNuclear dataNeutron radiationNuclear technologyEnergia nuclearPhysics::Accelerator PhysicsFísica nuclearSpallation Neutron Source
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Measurement of cross sections of the interactions e+e−→ ϕϕω and e+e−→ ϕϕϕ at center-of-mass energies from 4.008 to 4.600 GeV

2017

Abstract Using data samples collected with the BESIII detector at the BEPCII collider at six center-of-mass energies between 4.008 and 4.600 GeV, we observe the processes e + e − → ϕ ϕ ω and e + e − → ϕ ϕ ϕ . The Born cross sections are measured and the ratio of the cross sections σ ( e + e − → ϕ ϕ ω ) / σ ( e + e − → ϕ ϕ ϕ ) is estimated to be 1.75 ± 0.22 ± 0.19 averaged over six energy points, where the first uncertainty is statistical and the second is systematic. The results represent first measurements of these interactions.

Nuclear and High Energy PhysicsBESIII детекторe+e- annihilationElectron–positron annihilation01 natural sciencesNOlaw.inventionNuclear physicsCross section (physics)law0103 physical sciencesCross section; e+e−annihilation; Triple quarkonia; Nuclear and High Energy Physics010306 general physicsColliderTriple quarkoniaPhysicsAnnihilationCross section010308 nuclear & particles physicse+e−annihilatione+e− annihilationlcsh:QC1-999BEPCII коллайдерe+e? annihilationCenter of massCross section; e+e- annihilation; Triple quarkonia; Nuclear and High Energy Physicslcsh:Physics
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Laser resonance ionization spectroscopy on lutetium for the MEDICIS project

2017

The MEDICIS-PROMED Innovative Training Network under the Horizon 2020 EU program aims to establish a network of early stage researchers, involving scientific exchange and active cooperation between leading European research institutions, universities, hospitals, and industry. Primary scientific goal is the purpose of providing and testing novel radioisotopes for nuclear medical imaging and radionuclide therapy. Within a closely linked project at CERN, a dedicated electromagnetic mass separator system is presently under installation for production of innovative radiopharmaceutical isotopes at the new CERN-MEDICIS laboratory, directly adjacent to the existing CERN-ISOLDE radioactive ion beam …

Nuclear and High Energy PhysicsCERN-MEDICISIon beamNuclear engineeringchemistry.chemical_element02 engineering and technology01 natural sciencesLASER IONIZATION SPECTROSCOPYIsotope separationlaw.invention010309 opticslawIonizationLUTETIUM0103 physical sciencesDetectors and Experimental TechniquesPhysical and Theoretical ChemistryLarge Hadron ColliderChemistry021001 nanoscience & nanotechnologyCondensed Matter PhysicsLaserAtomic and Molecular Physics and OpticsIon sourceLutetiumRadionuclide therapyISOTOPE SEPARATIONAtomic physics0210 nano-technologyHyperfine Interactions
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Latest predictions from the EbyE NLO EKRT model

2019

We present the latest results from the NLO pQCD + saturation + viscous hydrodynamics (EbyE NLO EKRT) model. The parameters in the EKRT saturation model are fixed by the charged hadron multiplicity in the 0-5 \% 2.76 TeV Pb+Pb collisions. The $\sqrt{s}$, $A$ and centrality dependence of the initial particle production follows then from the QCD dynamics of the model. This allows us to predict the $\sqrt{s}$ and $A$ dependence of the particle production. We show that our results are in an excellent agreement with the low-$p_T$ data from 2.76 TeV and 5.02 TeV Pb+Pb collisions at the LHC as well as with the data from the 200 GeV Au+Au collisions at RHIC. In particular, we study the centrality de…

Nuclear and High Energy PhysicsCOLLISIONSMULTIPLICITIESNuclear TheoryHadronFOS: Physical scienceshiukkasfysiikka7. Clean energy01 natural sciences114 Physical sciencesdissipative fluid dynamicNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsTRANSVERSE ENERGIESNuclear ExperimentNuclear theoryMass numberQuantum chromodynamicsPhysicsLarge Hadron Colliderta114010308 nuclear & particles physicssaturationHigh Energy Physics::PhenomenologyMultiplicity (mathematics)heavy-ion collisionsCharged particleHigh Energy Physics - PhenomenologyHigh Energy Physics::Experimentperturbative QCD calculationsydinfysiikka
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The experience of building and operating COMPASS RICH-1

2010

COMPASS RICH-1 is a large size gaseous Imaging Cherenkov Detector providing hadron identification in the range from 3 to 55 GeV/c, in the wide acceptance spectrometer of the COMPASS Experiment at CERN SPS. It uses a 3 m long C(4)F(10) radiator, a 21 m(2) large VUV mirror surface and two kinds of photon detectors: MAPMTs and MWPCs with CsI photocathodes, covering a total of 5.5 m(2). It is in operation since 2002 and its performance has increased in time thanks to progressive optimization and mostly to a major upgrade which was implemented in 2006. The main characteristics of COMPASS RICH-1 components are described and some specific aspects related to the radiator gas system, the mirror alig…

Nuclear and High Energy PhysicsCherenkov detectorPhysics::Instrumentation and Detectors[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]COMPASS01 natural sciencesParticle identificationParticle identificationlaw.inventionNuclear physicsCOMPASS; CsI; MAPMT; Photon detection; PID; RICH; Instrumentation; Nuclear and High Energy PhysicsOpticslawCompass0103 physical sciencesCOMPASS experimentCsI photoconverter010306 general physicsRICHInstrumentationEvent reconstructionPhysicsLarge Hadron ColliderSpectrometer010308 nuclear & particles physicsbusiness.industryPIDUpgradePhoton detectionMAPMTCsIParticle identification; COMPASS; RICH; MAPMT; CsI photoconverterHigh Energy Physics::Experimentbusiness
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The DAMPE silicon–tungsten tracker

2016

Abstract The DArk Matter Particle Explorer (DAMPE) is a spaceborne astroparticle physics experiment, launched on 17 December 2015. DAMPE will identify possible dark matter signatures by detecting electrons and photons in the 5 GeV–10 TeV energy range. It will also measure the flux of nuclei up to 100 TeV, for the study of the high energy cosmic ray origin and propagation mechanisms. DAMPE is composed of four sub-detectors: a plastic strip scintillator, a silicon–tungsten tracker–converter (STK), a BGO imaging calorimeter and a neutron detector. The STK is composed of six tracking planes of 2 orthogonal layers of single-sided micro-strip detectors, for a total detector surface of ca. 7 m2. T…

Nuclear and High Energy PhysicsCosmic rays; Dark matter; Silicon tracker; Spaceborne experiment; Nuclear and High Energy Physics; InstrumentationPhysics::Instrumentation and DetectorsCosmic rayParticle detectorsTracking (particle physics)01 natural sciencesParticle detectorOpticscosmic rays0103 physical sciencesDark matterNeutron detection010303 astronomy & astrophysicsInstrumentationAstroparticle physicsPhysicsLarge Hadron ColliderCalorimeter (particle physics)010308 nuclear & particles physicsbusiness.industryDetectorSettore FIS/01 - Fisica SperimentaleParticle detectors cosmic raysSpaceborne experimentSilicon trackerHigh Energy Physics::Experimentbusiness
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