Search results for "PARTICLE PHYSICS"

showing 10 items of 6826 documents

Effect of double frequency heating on the lead afterglow beam currents of an electron cyclotron resonance ion source

2017

International audience; The effect of double frequency heating on the performance of the CERN GTS-LHC 14.5 GHz ElectronCyclotron Resonance (ECR) ion source in afterglow mode is reported. The source of the secondary microwave frequency was operated both in pulsed and continuous wave (CW) modes within the range of 12–18 GHz. The results demonstrate that the addition of the secondary frequency can significantly impact the extracted beam currents and the temporal stability of the beam during the afterglow discharge. For example, up to a factor of 2.6 increase was achieved for 208Pb35+ and a factor of 3.1 for 208Pb37+ compared to single frequency afterglow currents. It is shown that these effect…

Nuclear and High Energy PhysicsMaterials scienceCERN LabPhysics and Astronomy (miscellaneous)Ion beam[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Cyclotron resonancecyclotron: resonanceheating01 natural sciencesElectron cyclotron resonance010305 fluids & plasmasmicrowaves: frequencyplasma production0103 physical scienceslead: ionlcsh:Nuclear and particle physics. Atomic energy. Radioactivityparticle source010302 applied physicsta114beam: stabilityResonanceSurfaces and InterfacesAccelerators and Storage RingsIon sourceheavy ionAfterglowlcsh:QC770-798Atomic physicsMicrowaveIon cyclotron resonanceperformancePhysical Review Accelerators and Beams
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Hybrid density functional calculations of hyperfine coupling tensor for hole-type defects in MgAl2O4

2020

This work has been performed within the framework of the EUROfusion Enabling Research project: ENR-MFE19.ISSP-UL-02 “Advanced experimental and theoretical analysis of defect evolution and structural disordering in optical and dielectric materials for fusion application”. The views and opinions expressed herein do not necessarily reflect those of the European Commission.

Nuclear and High Energy PhysicsMaterials scienceMgAl2O4 (spinel)02 engineering and technologyType (model theory)engineering.material010402 general chemistry01 natural sciencesMolecular physicsResonance (particle physics)Spectral linelaw.inventionParamagnetismlaw:NATURAL SCIENCES:Physics [Research Subject Categories]TensorElectron paramagnetic resonanceInstrumentationHole-type defects (V-centres)Relaxation (NMR)Spinel021001 nanoscience & nanotechnology3. Good health0104 chemical sciencesHybrid DFT calculations (B3LYP)engineering0210 nano-technologyNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Tracking with heavily irradiated silicon detectors operated at cryogenic temperatures

1998

In this work we show that a heavily irradiated double-sided silicon microstrip detector recovers its performance when operated at cryogenic temperatures. A DELPHI microstrip detector, irradiated to a fluence of /spl sim/4/spl times/10/sup 14/ p/cm/sup 2/, no longer operational at room temperature, cannot be distinguished from a non-irradiated one when operated at T<120 K. Besides confirming the previously observed 'Lazarus effect' in single diodes, these results establish, for the first time, the possibility of using standard silicon detectors for tracking applications in extremely demanding radiation environments.

Nuclear and High Energy PhysicsMaterials sciencePassivationSiliconbusiness.industryDetectorchemistry.chemical_elementRadiationTracking (particle physics)FluenceNuclear Energy and EngineeringchemistryOptoelectronicsIrradiationDetectors and Experimental TechniquesElectrical and Electronic EngineeringbusinessDiodeIEEE Transactions on Nuclear Science
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Vacuum electrical breakdown conditioning study in a parallel plate electrode pulsed dc system

2019

Conditioning of a metal structure in a high-voltage system is the progressive development of resistance to vacuum arcing over the operational life of the system. This is, for instance, seen during the initial operation of radio frequency (rf) cavities in particle accelerators. It is a relevant topic for any technology where breakdown limits performance and where conditioning continues for a significant duration of system run time. Projected future linear accelerators require structures with accelerating gradients of up to 100  MV/m. Currently, this performance level is achievable only after a multimonth conditioning period. In this work, a pulsed dc system applying voltage pulses over paral…

Nuclear and High Energy PhysicsMaterials sciencePhysics and Astronomy (miscellaneous)Electrical breakdownFOS: Physical sciencesApplied Physics (physics.app-ph)01 natural sciences114 Physical scienceslaw.inventionElectric arclaw0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physics010308 nuclear & particles physicsbusiness.industryPulsed DCParticle acceleratorPhysics - Applied PhysicsSurfaces and InterfacesElectrodeOptoelectronicslcsh:QC770-798Radio frequencybusinessphysics.app-phOrder of magnitudeVoltagePhysical Review Accelerators and Beams
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Measurement of the spin density matrix for the rho(0), K*(0)(892) and phi produced in Z(0) decays

1997

The spin density matrix elements for the rho(0), K-*0(892) and phi produced in hadronic Z(0) decays are measured in the DELPHI detector. There is no evidence for spin alignment of the K-*0(892) and phi, in the region x(p) less than or equal to 0.3 (x(p) = p/p(beam)), where rho(00) = 0.33 +/- 0.05 and rho(00) = 0.30 +/- 0.04, respectively. In the fragmentation region, x(p) greater than or equal to 0.4, there is some indication for spin alignment of the rho(0) and K-*0(892), since rho(00) = 0.43 +/- 0.05 and rho(00) = 0.46 +/- 0.08, respectively. These values are compared with those found in meson-induced hadronic reactions. For the phi, rho(00) = 0.30 +/- 0.04 for x(p) greater than or equal …

Nuclear and High Energy PhysicsMesonElectron–positron annihilationD-STARHadronANNIHILATIONSPartícules (Física nuclear)QUARK FRAGMENTATION; D-STAR; ANNIHILATIONS; HADRONS; MESONSNuclear physicsAngular distribution[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Matrix elementSpin densityDetectors de radiacióDELPHIPhysicsHADRONSD-STARQUARK FRAGMENTATIONLARGE ELECTRON POSITRON COLLIDERMESONSPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIMass spectrumPARTICLE PHYSICSAtomic physicsParticle Physics - ExperimentPHYSICS LETTERS B
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Large-angle production of charged pions with 3-12.9 GeV/c incident protons on nuclear targets

2008

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

Nuclear and High Energy PhysicsMesonProtonPhysics::Instrumentation and DetectorsHadronNuclear TheoryFOS: Physical sciencesddc:500.27. Clean energy01 natural sciencesParticle detectorHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear interaction length010306 general physicsNuclear ExperimentPhysicsTime projection chamber010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleFísicaCharged particlePhysics::Accelerator PhysicsHigh Energy Physics::ExperimentAtomic physicsNucleonParticle Physics - Experiment
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The electronic field shift factor of the 4s2S1/2?4p2PJ transitions in CaII

1993

The isotope shifts (IS) of the resonance lines 4s2S1/2−4p2PJin CaII (seven isotopes) have been measured by fast ion beam collinear laser spectroscopy (FIBCLS) with non-optical detection of the resonant laser-ion interaction. The electronic field shift factorF was derived from the experimental IS via a King plot procedure using the mean square nuclear charge radii from muon spectroscopy andelectron scattering. TheJ-independent resultF=−283(6) Mhz/fm2 was obtained. TheF-value resulting from extensive many body perturbation theory (MBPT) calculations, recently performed by Martensson-Pendrill et al., is in excellent agreement with the experimental value, confirming the reliability of the MBPT …

Nuclear and High Energy PhysicsMuonIon beamField (physics)ScatteringChemistryCondensed Matter PhysicsResonance (particle physics)Atomic and Molecular Physics and OpticsEffective nuclear chargePhysics::Atomic PhysicsPhysical and Theoretical ChemistryAtomic physicsPerturbation theorySpectroscopyHyperfine Interactions
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Time projection chambers for the T2K near detectors

2011

The T2K experiment is designed to study neutrino oscillation properties by directing a high intensity neutrino beam produced at J-PARC in Tokai, Japan, towards the large Super-Kamiokande detector located 295 km away, in Kamioka, Japan. The experiment includes a sophisticated near detector complex, 280 m downstream of the neutrino production target in order to measure the properties of the neutrino beam and to better understand neutrino interactions at the energy scale below a few GeV. A key element of the near detectors is the ND280 tracker, consisting of two active scintillator–bar target systems surrounded by three large time projection chambers (TPCs) for charged particle tracking. The d…

Nuclear and High Energy PhysicsNeutrino oscillationPhysics::Instrumentation and Detectorsddc:500.2Tracking (particle physics)01 natural sciences7. Clean energyNuclear physics0103 physical sciences010306 general physicsNeutrino oscillationInstrumentationPhysicsTime projection chamber010308 nuclear & particles physicsDetectorT2K experimentDrift chamber Gas system Micromegas Neutrino oscillation Time projection chamberFísicaMicroMegas detectorTime projectionchamberGas systemCharged particleTime projection chamberDrift chamberHigh Energy Physics::ExperimentNeutrinoMicromegas
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Implementing the three-particle quantization condition including higher partial waves

2019

We present an implementation of the relativistic three-particle quantization condition including both $s$- and $d$-wave two-particle channels. For this, we develop a systematic expansion about threshold of the three-particle divergence-free K matrix, $\mathcal{K}_{\mathrm{df,3}}$, which is a generalization of the effective range expansion of the two-particle K matrix, $\mathcal{K}_2$. Relativistic invariance plays an important role in this expansion. We find that $d$-wave two-particle channels enter first at quadratic order. We explain how to implement the resulting multichannel quantization condition, and present several examples of its application. We derive the leading dependence of the …

Nuclear and High Energy PhysicsNuclear TheoryAtomic Physics (physics.atom-ph)Relativistic invarianceFOS: Physical sciencesLattice QCD01 natural sciencesPhysics - Atomic PhysicsNuclear Theory (nucl-th)Quantization (physics)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBound statelcsh:Nuclear and particle physics. Atomic energy. RadioactivityQuadratic orderScattering Amplitudes010306 general physicsNuclear theoryCondensed Matter - Statistical MechanicsK matrixMathematical physicsPhysicsLattice Quantum Field TheoryStatistical Mechanics (cond-mat.stat-mech)010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Lattice QCDScattering amplitudeHigh Energy Physics - Phenomenologylcsh:QC770-798Journal of High Energy Physics
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QCD Challenges from pp to A-A Collisions

2020

This paper is a write-up of the ideas that were presented, developed and discussed at the third International Workshop on QCD Challenges from pp to A-A, which took place in August 2019 in Lund, Sweden. The goal of the workshop was to focus on some of the open questions in the field and try to come up with concrete suggestions for how to make progress on both the experimental and theoretical sides. The paper gives a brief introduction to each topic and then summarizes the primary results.

Nuclear and High Energy PhysicsNuclear Theorynucl-thFOS: Physical sciencesLibrary scienceHEAVY-ION COLLISIONShiukkasfysiikkaPROTONnucl-exAtomic01 natural sciencesHigh Energy Physics - ExperimentJET PRODUCTIONNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Particle and Plasma PhysicsDEPENDENCE0103 physical sciencesNuclearNuclear Physics - ExperimentPARTICLE-PRODUCTIONNuclear Experiment (nucl-ex)LONG-RANGE010306 general physicsNuclear ExperimentNuclear theoryParticle Physics - PhenomenologyQuantum chromodynamicsPhysicsELLIPTIC FLOW010308 nuclear & particles physicshep-exPB COLLISIONSMolecularhep-phNuclear & Particles PhysicsANGULAR-CORRELATIONSHigh Energy Physics - PhenomenologySTATISTICAL HADRONIZATIONNuclear Physics - TheoryydinfysiikkaParticle Physics - Experiment
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