Search results for "accelerator physics"

showing 10 items of 1294 documents

Central Region Upgrade for the Jyväskylä K130 Cyclotron

2020

The Jyväskylä K130 cyclotron has been in operation for more than 25 years providing beams from H to Au with energies ranging from 1 to 80 MeV/u for nuclear physics research and applications. At the typical energies around 5 MeV/u used for the nuclear physics program the injection voltage used is about 10 kV. The low voltage limits the beam intensity especially from the 18 GHz ECRIS HIISI. To increase the beam intensities the central region of the K130 cyclotron is being upgraded by increasing the injection voltage by a factor of 2. The new central region with spiral inflectors for harmonics 1-3 has been designed. The new central region shows better transmission in simulations than the origi…

ionitsyklotronit04 Operation and UpgradeshiukkaskiihdyttimetAccelerator Physics
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Search for a fermiophobic Higgs boson in the diphoton decay channel with the ATLAS detector

2012

[Excerpt] A search for a fermiophobic Higgs boson using diphoton events produced in proton-proton collisions at a centre-of-mass energy of s√=7 TeV is performed using data corresponding to an integrated luminosity of 4.9 fb−1 collected by the ATLAS experiment at the Large Hadron Collider. A specific benchmark model is considered where all the fermion couplings to the Higgs boson are set to zero and the bosonic couplings are kept at the Standard Model values (fermiophobic Higgs model). The largest excess with respect to the background-only hypothesis is found at 125.5 GeV, with a local significance of 2.9 standard deviations, which reduces to 1.6 standard deviations when taking into account …

Physics and Astronomy (miscellaneous)Atlas detector7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Naturvetenskap[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]HADRON COLLIDERSNuclear ExperimentDetectors de radiacióddc:539PhysicsHIGGS BOSONPhysicsSettore FIS/01 - Fisica SperimentalePHYSICS PARTICLES & FIELDSATLASNuclear & Particles PhysicsTransverse momentumPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs bosonFísica nuclearLHCNatural SciencesParticle Physics - ExperimentParticle physicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]STANDARD MODELFOS: Physical sciencesddc:500.2Partícules (Física nuclear)Nuclear physics0202 Atomic Molecular Nuclear Particle And Plasma Physics0103 physical sciencesddc:530High Energy Physics010306 general physicsEngineering (miscellaneous)0206 Quantum PhysicsScience & Technology010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTRANSVERSE-MOMENTUMCol·lisions (Física nuclear)HADRON-HADRON COLLISIONSExperimental High Energy PhysicsPhysics::Accelerator PhysicsHigh Energy Physics::Experiment
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First demonstration of Doppler-free 2-photon in-source laser spectroscopy at the ISOLDE-RILIS

2020

Abstract Collinear Doppler-free 2-photon resonance ionization has been applied inside a hot cavity laser ion source environment at CERN-ISOLDE. An injection-seeded Ti:sapphire ring laser was used to generate light pulses with a Fourier-limited linewidth for high-resolution spectroscopy. Using a molybdenum foil as a reflective surface positioned at the end of the target transfer line, rubidium was successfully ionized inside the hot cavity. The results are presented alongside previously obtained data from measurements performed at the RISIKO mass separator at Mainz University, where collinear and perpendicular ionization geometries were tested inside an RFQ ion guide. This work is a pre-curs…

Nuclear and High Energy PhysicsMaterials sciencetutkimuslaitteetspektroskopiaPhysics::OpticsRing laser01 natural scienceslaw.invention010309 opticsLaser linewidthsymbols.namesakeOpticslawIonization0103 physical sciencesPhysics::Atomic Physics010306 general physicsSpectroscopyInstrumentationRILISbusiness.industryLaser2-photon spectroscopyIon sourceresonance laser ionizationsymbolsPhysics::Accelerator PhysicsbusinessydinfysiikkaDoppler effectDoppler broadeningNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Medium energy physics with c.w. electron accelerators

2008

Nuclear physicsAccelerator physicsTriple coincidencePhysicsMedium energylawVirtual particleElectronColliderlaw.invention
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TASISpec—A highly efficient multi-coincidence spectrometer for nuclear structure investigations of the heaviest nuclei

2010

TASISpec (TASCA in Small Image mode Spectroscopy) combines composite Ge- and Si-detectors for a new detector setup aimed towards multi-coincidence gamma -ray, X-ray, conversion electron, fission fragment, and a-particle spectroscopy of the heaviest nuclei. It exploits the TASCA separator's unique small image focal mode, i.e. the fact that evaporation residues produced in fusion-evaporation reactions can be focused into an area of less than 3 cm in diameter. This provides the possibility to pack detectors in very close geometry, resulting in an unprecedented detection efficiency of radioactive decays in prompt and delayed coincidence with implanted nuclei. Crown Copyright (C) 2010 Publis…

Recoil separatorsNuclear and High Energy PhysicsalphaFissionElectronandAccelerator Physics and Instrumentationconversion electronNuclear physicsImage modespectroscopy at recoil separatorsgamma-rayNuclear ExperimentSpectroscopyClover Ge detectorInstrumentationSpontaneous fissionPhysicsdetectorSpectrometerDetectorGamma rayDecay tagging spectrometerCluster Ge detectorSi stripAtomic physicsNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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The magnet of the scattering and neutrino detector for the SHiP experiment at CERN

2019

The Search for Hidden Particles (SHiP) experiment proposal at CERN demands a dedicated dipole magnet for its scattering and neutrino detector. This requires a very large volume to be uniformly magnetized at B > 1.2 T, with constraints regarding the inner instrumented volume as well as the external region, where no massive structures are allowed and only an extremely low stray field is admitted. In this paper we report the main technical challenges and the relevant design options providing a comprehensive design for the magnet of the SHiP Scattering and Neutrino Detector.

TechnologyPhysics - Instrumentation and Detectorswigglers and undulators)magnet: designPermanent magnet devicesPhysics::Instrumentation and Detectorsengineering01 natural sciences7. Clean energy09 Engineering030218 nuclear medicine & medical imagingradiation hardened magnetsSubatomär fysik0302 clinical medicineDipole magnetSubatomic PhysicsNeutrino detectorsDetectors and Experimental TechniquesInstruments & InstrumentationInstrumentationphysics.ins-detAcceleration cavities and magnets superconducting (high-temperature superconductor; radiation hardened magnets; normal-conducting; permanent magnet devices; wigglers and undulators)Mathematical PhysicsPhysics02 Physical SciencesLarge Hadron ColliderInstrumentation and Detectors (physics.ins-det)magnet: technologyNuclear & Particles Physicsbending magnetneutrino: detectorNeutrino detectornormal-conductingAcceleration cavities and magnets superconducting (high-temperature superconductorproposed experimentCERN LabRadiation hardened magnetsFOS: Physical sciencesNormal-conductingAccelerator Physics and InstrumentationNuclear physics03 medical and health sciences0103 physical sciencespermanent magnet devices[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Wigglers and undulators)normal-conducting magnetsScience & Technology010308 nuclear & particles physicsScatteringLarge detector systems for particle and astroparticle physicsAcceleratorfysik och instrumenteringLarge detector systems for particle physicsHigh temperature superconductors Neutrons Permanent magnets Ships Superconducting magnets Wigglers Astroparticle physics Comprehensive designs Massive structures Neutrino detectors Normal-conducting Radiation-hardened Ship experiments Technical challenges Particle detectorsVolume (thermodynamics)MagnetAcceleration cavities and magnets superconducting (high-temperature superconductor; Large detector systems for particle and astroparticle physics; Neutrino detectors; Normal-conducting; Permanent magnet devices; Radiation hardened magnets; Wigglers and undulators)High Energy Physics::Experimentneutrino detectors
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Testing electromagnetic proton form factors in the annihilation process p+p¯→π0+e−+e+

2011

We study the annihilation channel in proton antiproton collisions with production of a single neutral pion and an electron-positron pair. It is shown that this reaction allows access to the proton electromagnetic form factors in the ‘unphysical’ region and to the difference between complex phases of the Dirac and Pauli proton form factors. The differential cross section is given in the laboratory frame in an experimental setup where all outgoing particles are fully detected.

PhysicsScattering cross-sectionNuclear and High Energy PhysicsParticle physicsAnnihilationProtonNuclear TheoryDirac (software)Atomic and Molecular Physics and OpticsNuclear physicssymbols.namesakePauli exclusion principlePionAntiprotonsymbolsPhysics::Accelerator PhysicsNuclear ExperimentNuclear Physics B - Proceedings Supplements
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Deceleration of antiprotons from MeV to keV energies

1993

Trapping of antiprotons for high precision measurements at the Low Energy Antiproton Ring (LEAR/CERN) requires the deceleration of the antiproton beam from typically 5.8 MeV energy down to 10 keV for final capture in standard Penning traps. Two methods, the degradation of the beam in thin foils and the deceleration of the beam in an inverse cyclotron are investigated so far. The foil technique was successfully demonstrated with trapping efficiencies up to a few 10−4 and is now routinely used in the high precision measurement of the antiprotonproton mass ratio. The degradation foil method is compared with the deceleration technique using an inverse cyclotron tested also at LEAR.

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderCyclotronTrappingMass ratioCondensed Matter PhysicsAtomic and Molecular Physics and Opticslaw.inventionNuclear physicsAntiproton beamPhysics::Plasma PhysicslawAntiprotonPhysics::Accelerator PhysicsPhysics::Atomic PhysicsPhysical and Theoretical ChemistryAtomic physicsNuclear ExperimentBeam (structure)FOIL methodHyperfine Interactions
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Dijet azimuthal correlations and conditional yields in pp and p+Pb collisions at sNN=5.02TeV with the ATLAS detector

2019

This paper presents a measurement of forward-forward and forward-central dijet azimuthal angular correlations and conditional yields in proton-proton (pp) and proton-lead (p + Pb) collisions as a p ...

PhysicsMapleLarge Hadron Collider010308 nuclear & particles physicsAtlas detectorNuclear Theoryengineering.material01 natural sciences7. Clean energyNuclear physicsAzimuthmedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesmedicineengineeringPhysics::Accelerator PhysicsRapidityNuclear Experiment010306 general physicsNucleonSaturation (chemistry)Physical Review C
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PROTONIUM: The Mainz Cascade Model

1990

Recent experiments at LEAR have studied extensively the properties of antiprotonic hydrogen, often also called protonium.

PhysicsNuclear physicsHydrogenchemistryCascadeProtoniumPrincipal quantum numberPhysics::Accelerator Physicschemistry.chemical_elementHigh Energy Physics::ExperimentPhysics::Atomic PhysicsNuclear Experiment
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