Search results for "nuclear physics"

showing 10 items of 5307 documents

First operation of the superconducting Darmstadt linear electron accelerator as an energy recovery linac

2020

The superconducting Darmstadt linear electron accelerator (S-DALINAC) has been operated as an energy recovery linac (ERL) for the first time. The S-DALINAC is a recirculating superconducting radio-frequency (SRF) accelerator and had been upgraded with an additional recirculation beamline. It features a path length adjustment system that provides a freedom of choice of 360\ifmmode^\circ\else\textdegree\fi{} for the rf phase difference between the electron bunches recirculated through the new beamline and the phase of the accelerating ${\mathrm{TM}}_{010}$ mode of the oscillating electromagnetic field in the SRF cavities of the accelerator. A choice of around 180\ifmmode^\circ\else\textdegree…

Electromagnetic fieldSuperconductivityPhysicsNuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)Phase (waves)Particle acceleratorSurfaces and InterfacesKinetic energylaw.inventionNuclear physicsBeamlinelawlcsh:QC770-798Physics::Accelerator Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityEnergy (signal processing)Beam (structure)Physical Review Accelerators and Beams
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Towards saturation of the electron-capture delayed fission probability: The new isotopes $^{240}Es$ and $^{236}Bk$

2016

Abstract The new neutron-deficient nuclei 240 Es and 236 Bk were synthesised at the gas-filled recoil separator RITU. They were identified by their radioactive decay chains starting from 240 Es produced in the fusion–evaporation reaction 209 Bi( 34 S,3n) 240 Es. Half-lives of 6 ( 2 ) s and 22 − 6 + 13 s were obtained for 240 Es and 236 Bk, respectively. Two groups of α particles with energies E α = 8.19 ( 3 ) MeV and 8.09 ( 3 ) MeV were unambiguously assigned to 240 Es. Electron-capture delayed fission branches with probabilities of 0.16 ( 6 ) and 0.04 ( 2 ) were measured for 240 Es and 236 Bk, respectively. These new data show a continuation of the exponential increase of ECDF probabilitie…

Electron-capture delayed fissionNuclear and High Energy PhysicsElectron captureFissionFusion–evaporation reaction236[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]236 Bk01 natural sciences7. Clean energyRecoil separatorNuclear physicsfusion-evaporation reactionsE236Bk240Es240 Es0103 physical sciencesddc:530010306 general physicsα decayisotopesPhysics240Isotopeta114Isotopes with mass 236–240010308 nuclear & particles physicslcsh:QC1-999Exponential functionBkmassAtomic physicsSaturation (chemistry)Fusion–evaporation reactionsα particleslcsh:PhysicsRadioactive decay
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Mechanical construction and installation of the ATLAS tile calorimeter

2013

This paper summarises the mechanical construction andinstallation of the Tile Calorimeter for the ATLASexperiment at the Large Hadron Collider in CERN, Switzerland. The TileCalorimeter is a sampling calorimeter using scintillator as the sensitivedetector and steel as the absorber and covers the central region of the ATLASexperiment up to pseudorapidities ±1.7. The mechanical construction ofthe Tile Calorimeter occurred over a periodof about 10 years beginning in 1995 with the completionof the Technical Design Report and ending in 2006 with the installationof the final module in the ATLAS cavern. Duringthis period approximately 2600 metric tons of steel were transformedinto a laminated struc…

EngineeringLarge Hadron ColliderAtlas (topology)business.industryPhysics::Instrumentation and DetectorsNuclear engineeringATLAS experimentCalorimeters; Detector design and construction technologies and materialsNuclear physicsTile calorimeterCalorimetersPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentDetectors and Experimental TechniquesMechanical constructionDetector design and construction technologies and materialsNuclear ExperimentbusinessInstrumentationMathematical Physics
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The measurement programme at the neutron time-of-flight facility n_TOF at CERN

2016

Neutron-induced reaction cross sections are important for a wide variety of research fields ranging from the study of nuclear level densities, nucleosynthesis to applications of nuclear technology like design, and criticality and safety assessment of existing and future nuclear reactors, radiation dosimetry, medical applications, nuclear waste transmutation, accelerator-driven systems and fuel cycle investigations. Simulations and calculations of nuclear technology applications largely rely on evaluated nuclear data libraries. The evaluations in these libraries are based both on experimental data and theoretical models. CERN’s neutron time-of-flight facility n TOF has produced a considerabl…

EngineeringNuclear transmutationQC1-999Nuclear engineering[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesNuclear physicsPhysics and Astronomy (all)0103 physical sciences:Física::Electromagnetisme [Àrees temàtiques de la UPC]ddc:530Nuclear Physics - ExperimentNeutron010306 general physicsNeutrons:Energies::Energia nuclear [Àrees temàtiques de la UPC]Large Hadron Collider010308 nuclear & particles physicsbusiness.industryPhysicsNuclear dataRadioactive wasteNuclear technologyBeamlineCriticalitybusinessEPJ Web of Conferences
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Mock-up testing facilities and qualification strategy for EU ITER TBMs

2010

European test blanket modules (TBM) for both European blanket concepts, namely the Helium Cooled Lithium Lead (HCLL) and the Helium Cooled Pebble Bed (HCPB), and their auxiliary systems have been designed in the last years. This paper presents the experimental facilities available in Europe for the qualification tests of European TBMs. In particular, devices designed to analyze specific technological issues, for example corrosion under strong magnetic fields or tritium management and extraction, as well as large scale facility to perform integral tests are described. A preliminary overview on the qualification strategy is presented and discussed.

EngineeringTest facilityTokamakbusiness.industryMechanical EngineeringNuclear engineeringChamp magnetiqueFusion powerBlanketlaw.inventionNuclear physicsNuclear Energy and EngineeringMockuplawQualification testingGeneral Materials SciencebusinessCivil and Structural EngineeringFusion Engineering and Design
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First Observation of an Attractive Interaction between a Proton and a Cascade Baryon

2019

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. This Letter presents the first experimental observation of the attractive strong interaction between a proton and a multistrange baryon (hyperon) Ξ−. The result is extracted from two-particle correlations of combined p−Ξ−⊕¯p−¯Ξ+ pairs measured in p−Pb collisions at √sNN=5.02  TeV at the LHC with ALICE. The measured correlation function is compared with the prediction obtained assuming only an attractive Coulomb interaction and a stand…

Equation of state:Kjerne- og elementærpartikkelfysikk: 431 [VDP]HadronGeneral Physics and Astronomyinteraction: Coulombhyperon01 natural sciencesdensity [saturation]hyperon productionALICEBound state[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Coulombn: matterBOUND-STATE; COLLISIONScorrelation functionHeavy IonNuclear Experimentneutron starhadron-hadron scatteringlatticePhysicsPhysicsstrong interactionVDP::Kjerne- og elementærpartikkelfysikk: 431ddc::Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]quark gluon plasmaPRIRODNE ZNANOSTI. Fizika.:Nuclear and elementary particle physics: 431 [VDP]CERN LHC CollVDP::Nuclear and elementary particle physics: 431saturation: densitycorrelation: two-particleCOLLISIONSeducationStrong interactionPhysics and Astronomy(all)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]BOUND-STATE114 Physical sciencesmatter [n]Nuclear physicsinteraction: Coulomb ; correlation: two-particle ; saturation: density ; n: matter ; strong interaction ; lattice ; hyperon ; correlation function ; equation of state ; CERN LHC Coll ; neutron star ; ALICE ; experimental results ; 5020 GeV-cms/nucleon0103 physical sciencesddc:530Neutron5020 GeV-cms/nucleon010306 general physicstwo-particle [correlation]equation of stateCoulomb [interaction]Heavy Ion Physics:Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431 [VDP]HyperonALICE experimenthyperon production hadron-hadron scattering ALICE experimentNATURAL SCIENCES. Physics.BaryonElementary Particles and FieldsHigh Energy Physics::Experimentexperimental results
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Probing Compositeness with the CMS eejj & eej Data

2016

Quark-lepton compositeness is a well-known beyond the Standard Model (SM) scenario with heavy exotic particles like leptoquarks (LQs) and leptogluons (LGs) etc. These particles can couple to leptons and jets simultaneously. In this letter, we use the recent CMS scalar LQ search data in the $eejj$ and $eej$ channels to probe this scenario. We recast the data in terms of a color octet partner of the SM electron (or a first generation spin-1/2 LG) that couples to an electron and a gluon via a dimension five operator suppressed by the quark-lepton compositeness scale ($\Lambda$). By combining different production processes of the color octet electron ($e_8$) at the LHC, we use the CMS 8TeV data…

Exclusion limitsParticle physicsNuclear and High Energy PhysicsLeptogluonPhysics beyond the Standard ModelLHC; Compositeness scale; Leptogluon; Exclusion limitsFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsSubatomär fysikHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesSubatomic PhysicsLeptoquark010306 general physicsPhysicsLarge Hadron Collider010308 nuclear & particles physicsCompositeness scaleHigh Energy Physics::Phenomenologylcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics::ExperimentLHClcsh:PhysicsLepton
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Observation of e + e − → ηψ(2S) at center-of-mass energies from 4.236 to 4.600 GeV

2021

Journal of high energy physics 2021(10), 177 (2021). doi:10.1007/JHEP10(2021)177

ExoticsNuclear and High Energy Physicsmeasured [channel cross section]e+-e− ExperimentsQuarkoniumannihilation [electron positron]QC770-798electron positron: annihilationetaParticle and resonance productionMeasure (mathematics)530Standard deviationNONuclear physicsSubatomär fysikCross section (physics)e+-e��� Experimentsenergy dependence: measured [cross section]Astronomi astrofysik och kosmologiNuclear and particle physics. Atomic energy. RadioactivitySubatomic PhysicsAstronomy Astrophysics and Cosmologyddc:530e+-e− Experiments Exotics Particle and resonance production Quarkoniumpsi(3685)PhysicsBESe(+)-e(-) ExperimentsDetectorstatistical [error]electron positron --> eta psi(3685)e +-e − Experimentselectron positron: colliding beamsBeijing Stor4.236-4.600 GeV-cmsCollisionerror: statisticalYield (chemistry)e-e Experimentselectron positron --> eta psi(3685)colliding beams [electron positron]High Energy Physics::ExperimentCenter of masscross section: energy dependence: measuredchannel cross section: measuredStorage ringexperimental results
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Search for new phenomena in final states with large jet multiplicities and missing transverse momentum at s√=8 TeV proton-proton collisions using the…

2013

A search is presented for new particles decaying to large numbers (7 or more) of jets, with missing transverse momentum and no isolated electrons or muons. This analysis uses 20.3 fb[superscript −1] of pp collision data at s√ = 8 TeV collected by the ATLAS experiment at the Large Hadron Collider. The sensitivity of the search is enhanced by considering the number of b-tagged jets and the scalar sum of masses of large-radius jets in an event. No evidence is found for physics beyond the Standard Model. The results are interpreted in the context of various simplified supersymmetry-inspired models where gluinos are pair produced, as well as an mSUGRA/CMSSM model.

ExoticsPhysics::Instrumentation and DetectorsCiencias FísicasPhysics beyond the Standard ModelElectron01 natural sciences7. Clean energyHigh Energy Physics - Experiment//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)Jets[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]QChadron-hadron scatteringPhysicsGluinoLarge Hadron ColliderSettore FIS/01 - Fisica SperimentaleATLAS experimentSupersymmetryATLASJet physicsPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGLHCParticle Physics - ExperimentCIENCIAS NATURALES Y EXACTASNuclear and High Energy PhysicsParticle physicsHadron-Hadron Scattering; Jet physics; Supersymmetry ExoticsCiências Naturais::Ciências Físicas530 Physics:Ciências Físicas [Ciências Naturais]Scalar (mathematics)FOS: Physical sciencesHadron-hadron scattering530Nuclear physics0103 physical sciencesFysikddc:530High Energy Physics010306 general physicsScience & TechnologyMuon010308 nuclear & particles physicssupersymmetry; hadron-hadron scattering; jet physics; exoticsHigh Energy Physics::PhenomenologyexoticsFísica//purl.org/becyt/ford/1.3 [https]Hadron scatteringAstronomíaHADRON-HADRON COLLISIONSExperimental High Energy PhysicsHigh Energy Physics::ExperimentSupersymmetrysupersymmetry
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Alpha-decay studies of the francium isotopes 198Fr and 199Fr nuclei

2013

Very neutron deficient francium isotopes have been produced in fusion evaporation reactions using 60Ni ions on 141Pr targets. The gas-filled recoil separator RITU was employed to collect the fusion products and to separate them from the scattered beam. The activities were implanted into a position sensitive silicon detector after passing through a gas-counter system. The isotopes were identified using spatial and time correlations between the implants and the decays. Two α-particle activities, with Eα = 7613(15) keV and T1/2 = (15+12 −5 ) ms and Eα = 7684(15) keV and T1/2 = (16+13 −5 ) ms were identified in the new isotope 198Fr. In addition, the half-life and α-particle energy of 199Fr wer…

Experimental Nuclear Physics
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