Search results for "Collider"

showing 10 items of 1690 documents

Measurement of the 241Am neutron capture cross section at the n-TOF facility at CERN

2016

New neutron cross section measurements of minor actinides have been performed recently in order to reduce the uncertainties in the evaluated data, which is important for the design of advanced nuclear reactors and, in particular, for determining their performance in the transmutation of nuclear waste. We have measured the 241 Am(n,γ) cross section at the n TOF facility between 0.2 eV and 10 keV with a BaF2 Total Absorption Calorimeter, and the analysis of the measurement has been recently concluded. Our results are in reasonable agreement below 20 eV with the ones published by C. Lampoudis et al. in 2013, who reported a 22% larger capture cross section up to 110 eV compared to experimental …

Nuclear reactionNuclear transmutationnTOFQC1-999Neutron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyNuclear physicsPhysics and Astronomy (all)Cross section (physics)Nuclear reactorsReactors nuclears0103 physical sciencesCERNNeutron cross sectionNuclear Physics - Experimentddc:530Neutron010306 general physicsAbsorption (electromagnetic radiation)PhysicsNeutrons:Energies::Energia nuclear [Àrees temàtiques de la UPC]Large Hadron ColliderCross section:Física [Àrees temàtiques de la UPC]010308 nuclear & particles physicsPhysicsNuclear reactionCalorimeter
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Large-angle production of charged pions by 3 GeV/c - 12.9 GeV/c protons on beryllium, aluminium and lead targets

2008

Measurements of the double-differential pi(+/-) production cross-section in the range of momentum 100 MeV/c <= p < 800 MeV/c and angle 0.35 rad <= theta < 2.15 rad in proton-beryllium, proton-aluminium and proton-lead collisions are presented. The data were taken with the HARP detector in the T9 beam line of the CERN PS. The pions were produced by proton beams in a momentum range from 3 GeV/c to 12.9 GeV/c hitting a target with a thickness of 5% of a nuclear interaction length. The tracking and identification of the produced particles was performed using a small-radius cylindrical time projection chamber (TPC) placed inside a solenoidal magnet. Incident particles were identified by an elabo…

Nuclear reactionParticle physicsMesonProtonPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsHadronNuclear TheoryFOS: Physical sciencesddc:500.201 natural sciences7. Clean energyHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Pion0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear interaction length010306 general physicsNuclear ExperimentEngineering (miscellaneous)PhysicsTime projection chamberLarge Hadron Collider010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleFísicaSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Physics::Accelerator PhysicsHigh Energy Physics::ExperimentParticle Physics - Experiment
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Large-angle production of charged pions by 3 GeV/c-12 GeV/c protons on carbon, copper and tin targets

2008

A measurement of the double-differential pi(+/-) production cross-section in proton-carbon, proton-copper and proton-tin collisions in the range of pion momentum 100 MeV/c <= p <800 MeV/c and angle 0.35 rad <= theta < 2.15 rad is presented. The data were taken with the HARP detector in the T9 beam line of the CERN PS. The pions were produced by proton beams in a momentum range from 3 GeV/c to 12 GeV/c hitting a target with a thickness of 5% of a nuclear interaction length. The tracking and identification of the produced particles was done using a small-radius cylindrical time projection chamber (TPC) placed in a solenoidal magnet. An elaborate system of detectors in the beam line ensured th…

Nuclear reactionParticle physicsPhysics and Astronomy (miscellaneous)ProtonMesonPhysics::Instrumentation and DetectorsHadronNuclear TheoryFOS: Physical sciencesddc:500.201 natural sciences7. Clean energyHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Pion0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear interaction length010306 general physicsNuclear ExperimentEngineering (miscellaneous)PhysicsTime projection chamberLarge Hadron Collidercross section010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleFísicaSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Physics::Accelerator PhysicsHigh Energy Physics::ExperimentParticle Physics - ExperimentEUROPEAN PHYSICAL JOURNAL C
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Measurement of Z 0 -boson production at large rapidities in Pb–Pb collisions at

2018

The production of Z0 bosons at large rapidities in Pb–Pb collisions at √sNN=5.02TeV is reported. Z0 candidates are reconstructed in the dimuon decay channel (Z0→μ+μ−), based on muons selected with pseudo-rapidity −4.0 20GeV/c. The invariant yield and the nuclear modification factor, RAA, are presented as a function of rapidity and collision centrality. The value of RAA for the 0–20% central Pb–Pb collisions is 0.67±0.11(stat.)±0.03(syst.)±0.06(corr. syst.), exhibiting a deviation of 2.6σ from unity. The results are well-described by calculations that include nuclear modifications of the parton distribution functions, while the predictions using vacuum PDFs deviate from data by 2.3σ in the 0…

Nuclear reactionPhysicsNuclear and High Energy PhysicsLarge Hadron ColliderMuon010308 nuclear & particles physicsParton01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesRapidityImpact parameter010306 general physicsColliderBoson
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Shape dynamics in neutron-rich Kr isotopes: Coulomb excitation of 92Kr, 94Kr and 96Kr

2013

We report on the study of excited states in 92,94,96Kr populated via projectile Coulomb excitation at safe energies. The radioactive ion beams at energies of 2.85 MeV/u were delivered by the REX-ISOLDE facility at CERN and impinged on self-supporting 194,196Pt targets. The emitted γ -rays were detected by the Miniball detector-array. A detailed description of the experimental techniques used for extracting diagonal and transitional matrix elements and of the theoretical framework is given. The present experiment reveals the moderate evolution of the collective structure in the considered neutron-rich Kr isotopic chain, which is supported by the interacting boson model combined with the self…

Nuclear reactionPhysicsNuclear and High Energy PhysicsLarge Hadron Colliderta114[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsProjectileCoulomb excitation01 natural sciences7. Clean energyNuclear physicsMatrix (mathematics)Excited state0103 physical sciencesPhysics::Accelerator PhysicsNeutronInteracting boson modelAtomic physicsNuclear Experiment010306 general physics
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Pathlength dependence of energy loss within in-medium showers

2010

Studying the pathlength dependence of high P_T hadron suppression in heavy-ion collisions by measuring the dependence of hard hadron production on the angle phi with the reaction plane in non-central collisions has so far been one of the most successful tools in constraining the microscopical picture of leading parton energy loss. With the imminent start of the LHC heavy-ion program and the possibility of full jet reconstruction, the focus has shifted to models which are capable of simulating full in-medium parton showers rather than tracing the leading parton only. Yet, on the level of single inclusive hadron observables, such shower models need to reproduce the findings of leading parton …

Nuclear reactionPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Colliderta114010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsMonte Carlo methodHadronHigh Energy Physics::PhenomenologyFOS: Physical sciencesPartonObservableElementary particle01 natural sciencesNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesProduction (computer science)High Energy Physics::Experiment010306 general physicsNuclear ExperimentPhysical Review C
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The Pion Single-Event Effect Resonance and its Impact in an Accelerator Environment

2020

International audience; The pion resonance in the nuclear reaction cross section is seen to have a direct impact on the single-event effect (SEE) cross section of modern electronic devices. This was experimentally observed for single-event upsets and single-event latchup. Rectangular parallelepiped (RPP) models built to fit proton data confirm the existence of the pion SEE cross-section resonance. The impact on current radiation hardness assurance (RHA) soft error rate (SER) predictions is, however, minimal for the accelerator environment since this is dominated by high neutron fluxes. The resonance is not seen to have a major impact on the high-energy hadron equivalence approximation estab…

Nuclear reactionProtonNuclear Theoryresonance: effectSingle event upsets01 natural sciences7. Clean energyResonance (particle physics)nuclear reactionelektroniikkakomponentitradiation hardness assurance (RHA)Detectors and Experimental TechniquesNuclear Experimentradiation: damagePhysicsLarge Hadron Colliderprotonscross sectionMesonsneutronitRandom access memorySEELarge Hadron Colliderpionsn: fluxNuclear and High Energy PhysicsprotonitMesonaccelerator[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]RHAsoft error ratesoft error rate (SER)hiukkaskiihdyttimetNuclear physicsFLUKACross section (physics)hiukkasetPion0103 physical sciencesNeutron[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Electrical and Electronic Engineeringpi: interactionsingle-event effect (SEE)Neutrons010308 nuclear & particles physicsneutronsAccelerators and Storage RingsParticle beamsNuclear Energy and EngineeringsäteilyfysiikkahadronIEEE Transactions on Nuclear Science
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Nuclear data activities at the n_TOF facility at CERN

2016

International audience; Nuclear data in general, and neutron-induced reaction cross sections in particular, are important for a wide variety of research fields. They play a key role in the safety and criticality assessment of nuclear technology, not only for existing power reactors but also for radiation dosimetry, medical applications, the transmutation of nuclear waste, accelerator-driven systems, fuel cycle investigations and future reactor systems as in Generation IV. Applications of nuclear data are also related to research fields as the study of nuclear level densities and stellar nucleosynthesis. Simulations and calculations of nuclear technology applications largely rely on evaluate…

Nuclear reactionU-235Nuclear transmutationnTOFCAPTURE CROSS-SECTIONNuclear dataTOTAL ABSORPTION CALORIMETERGeneral Physics and Astronomy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]COLLABORATION7. Clean energy01 natural sciences3100PHYSICSNuclear physicsPhysics and Astronomy (all)neutronDESIGNRadiation dosimetry0103 physical sciencesCERNn_TOFNuclear Physics - ExperimentNeutron010306 general physicsnuclear data n_TOF CERNPhysics:Energies::Energia nuclear [Àrees temàtiques de la UPC]NeutronsFRAGMENT ANGULAR-DISTRIBUTIONLarge Hadron Colliderntof:Física [Àrees temàtiques de la UPC]Cross section010308 nuclear & particles physicscernExperimental dataRadioactive wasteNuclear datanuclear dataNATURAL SCIENCES. Physics.Radiació--DosimetriaPRIRODNE ZNANOSTI. Fizika.Nuclear technologyCAPTURE CROSS-SECTION TOTAL ABSORPTION CALORIMETER FRAGMENT ANGULAR-DISTRIBUTION NEUTRON TH-232 U-235 C6D6 COLLABORATION PHYSICS DESIGN.NEUTRONTH-232C6D6
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The 33S(n,α)30Si cross section measurement at n TOF-EAR2 (CERN): From 0.01 eV to the resonance region

2017

The 33S(n,α)30Si cross section measurement, using 10B(n,α) as reference, at the n TOF Experimental Area 2 (EAR2) facility at CERN is presented. Data from 0.01 eV to 100 keV are provided and, for the first time, the cross section is measured in the range from 0.01 eV to 10 keV. These data may be used for a future evaluation of the cross section because present evaluations exhibit large discrepancies. The 33S(n,α)30Si reaction is of interest in medical physics because of its possible use as a cooperative target to boron in Neutron Capture Therapy (NCT).

Nuclear reactionnTOFNeutron therapyQC1-999chemistry.chemical_elementNeutron01 natural sciencesResonance (particle physics)Nuclear physicsCross section (physics)Physics and Astronomy (all)0103 physical sciencesCERNNeutronddc:530010306 general physicsBoronPhysicsNeutrons:Energies::Energia nuclear [Àrees temàtiques de la UPC]Range (particle radiation)Large Hadron Collidercross sectionReaccions nuclears:Física [Àrees temàtiques de la UPC]010308 nuclear & particles physicsPhysicsNuclear reactionNeutron capturechemistryNuclear reactions
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High precision measurement of the radiative capture cross section of 238U at the n_TOF CERN facility

2016

The importance of improving the accuracy on the capture cross-section of 238U has been addressed by the Nuclear Energy Agency, since its uncertainty significantly affects the uncertainties of key design parameters for both fast and thermal nuclear reactors. Within the 7th framework programme ANDES of the European Commission three different measurements have been carried out with the aim of providing the 238U(n,γ) cross-section with an accuracy which varies from 1 to 5%, depending on the energy range. Hereby the final results of the measurement performed at the n-TOF CERN facility in a wide energy range from 1 eV to 700 keV will be presented. © The Authors, published by EDP Sciences, 2017.

Nuclear reactionnTOFQC1-999Neutron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyNuclear physicsCross section (physics)Physics and Astronomy (all)Nuclear reactorsReactors nuclears0103 physical sciencesThermalCERNNeutronddc:530Nuclear Physics - Experiment010306 general physicsPhysics:Energies::Energia nuclear [Àrees temàtiques de la UPC]NeutronsRange (particle radiation)Large Hadron Collider:Física [Àrees temàtiques de la UPC]Cross section010308 nuclear & particles physicsPhysicsRadiative captureNuclear energyNuclear reactionEnergia nuclearEnergy (signal processing)
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