Search results for "Computer Science Application"

showing 10 items of 3998 documents

Beta decay and isomer spectroscopy in the 132Sn region: New results from EURICA

2013

A. Jungclaus et al.; XX International School on Nuclear Physics, Neutron Physics and Applications (Varna2013); Open Access. 4 pags.; 1 fig.

PhysicsHistoryIsotope010308 nuclear & particles physicsHigh intensitychemistry.chemical_elementUranium[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesBeta decayComputer Science ApplicationsEducationNuclear physicschemistry0103 physical sciencesExtensive dataNeutronAtomic physics010306 general physicsSpectroscopy
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Dealing with contaminants in Coulomb excitation of radioactive beams

2020

Abstract Data analysis of the Coulomb excitation experiment of the exotic 206Hg nucleus, recently performed at CERN’s HIE-ISOLDE facility, needs to account for the contribution to target excitation due to the strongly-present beam contaminant 130Xe. In this paper, the contamination subtraction procedure is presented.

PhysicsHistoryLarge Hadron Collider010308 nuclear & particles physicsCoulomb excitationSubtraction proceduretutkimuslaitteetCoulomb excitationContaminationhiukkaskiihdyttimet01 natural sciencesAccelerators and Storage Rings3100Computer Science ApplicationsEducationNuclear physics0103 physical sciencesPhysics::Accelerator PhysicsNuclear Physics - Experiment010306 general physicsNuclear ExperimentydinfysiikkaBeam (structure)ExcitationRadioactive beams
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Fast timing and trigger Cherenkov detector for collider experiments

2016

Analysis of fast timing and trigger Cherenkov detector's design for its use in collider experiments is presented. Several specific requirements are taken into account - necessity of the radiator's placement as close to the beam pipe as possible along with the requirement of gapless (solid) radiator's design. Characteristics of the Cherenkov detector's laboratory prototype obtained using a pion beam at the CERN Proton Synchrotron are also presented, showing the possibility of obtaining sufficiently high geometrical efficiency along with good enough time resolution (50 ps sigma).

PhysicsHistoryLarge Hadron ColliderPhysics::Instrumentation and DetectorsCherenkov detectorProton SynchrotronTime resolutionComputer Science ApplicationsEducationlaw.inventionNuclear physicsGapless playbacklawRadiator (engine cooling)Physics::Accelerator PhysicsHigh Energy Physics::ExperimentColliderBeam (structure)Journal of Physics: Conference Series
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Comparison between the fCCZ4 and BSSN formulations of Einstein equations in spherical polar coordinates

2015

Recently, we generalized a covariant and conformal version of the Z4 system of the Einstein equations using a reference metric approach, that we denote as fCCZ4. We successfully implemented and tested this approach in a 1D code that uses spherical coordinates and assumes spherical symmetry, obtaining from one to three orders of magnitude reduction of the Hamiltonian constraint violations with respect to the BSSN formulation in tests involving neutron star spacetimes. In this work, we show preliminary results obtained with the 3D implementation of the fCCZ4 formulation in a fully 3D code using spherical polar coordinates.

PhysicsHistoryLog-polar coordinatesSpherical coordinate systemAction-angle coordinatesSymmetry (physics)Computer Science ApplicationsEducationClassical mechanicsGeneralized coordinatesHamiltonian constraintEinstein field equationsCovariant transformationMathematical physicsJournal of Physics: Conference Series
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Loop quantum gravity and Planck-size black hole entropy

2007

The Loop Quantum Gravity (LQG) program is briefly reviewed and one of its main applications, namely the counting of black hole entropy within the framework is considered. In particular, recent results for Planck size black holes are reviewed. These results are consistent with an asymptotic linear relation (that fixes uniquely a free parameter of the theory) and a logarithmic correction with a coefficient equal to -1/2. The account is tailored as an introduction to the subject for non-experts.

PhysicsHistoryLogarithmFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Loop quantum gravityLinear-quadratic-Gaussian controlGeneral Relativity and Quantum CosmologyComputer Science ApplicationsEducationsymbols.namesakeTheoretical physicsGeneral Relativity and Quantum CosmologysymbolsLinear relationPlanckBlack hole thermodynamicsFree parameter
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HITRAP – a facility for experiments on heavy highly charged ions and on antiprotons

2009

HITRAP is a facility for very slow highly-charged heavy ions at GSI. HITRAP uses the GSI relativistic ion beams, the Experimental Storage Ring ESR for electron cooling and deceleration to 4 MeV/u, and consists of a combination of an interdigital H-mode (IH) structure with a radiofrequency quadrupole structure for further deceleration to 6 keV/u, and a Penning trap for accumulation and cooling to low temperatures. Finally, ion beams with low emittance will be delivered to a large variety of atomic and nuclear physics experiments. Presently, HITRAP is in the commissioning phase. The deceleration of heavy-ion beam from the ESR storage ring to an energy of 500 keV/u with the IH structure has be…

PhysicsHistoryLow emittancePenning trapComputer Science ApplicationsEducationIonlaw.inventionNuclear physicslawAntiprotonQuadrupolePhysics::Accelerator PhysicsPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentBeam (structure)Storage ringElectron coolingJournal of Physics: Conference Series
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Upgrade of the ATLAS Level-1 Trigger with event topology information

2015

The Large Hadron Collider (LHC) in 2015 will collide proton beams with increased luminosity from \unit{10^{34}} up to \unit{3 \times 10^{34}cm^{-2}s^{-1}}. ATLAS is an LHC experiment designed to measure decay properties of high energetic particles produced in the protons collisions. The higher luminosity places stringent operational and physical requirements on the ATLAS Trigger in order to reduce the 40MHz collision rate to a manageable event storage rate of 1kHz while at the same time, selecting those events with valuable physics meaning. The Level-1 Trigger is the first rate-reducing step in the ATLAS Trigger, with an output rate of 100kHz and decision latency of less than 2.5$\mu s$. It…

PhysicsHistoryLuminosity (scattering theory)Large Hadron ColliderPhysics::Instrumentation and DetectorsEvent (computing)Processor designReal-time computingProcess (computing)Computer Science ApplicationsEducationmedicine.anatomical_structureUpgradeAtlas (anatomy)medicineAdvanced Telecommunications Computing ArchitectureParticle Physics - ExperimentJournal of Physics: Conference Series
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Underground cosmic-ray experiment EMMA

2013

EMMA (Experiment with MultiMuon Array) is a new approach to study the composition of cosmic rays at the knee region (1 − 10 PeV). The array will measure the multiplicity and lateral distribution of the high-energy muon component of an air shower and its arrival direction on an event-by-event basis. The array operates in the Pyh¨asalmi Mine, Finland, at a depth of 75 metres (or 210 m.w.e) corresponding to the cut-off energy of approximately 50 GeV for vertical muons. The data recording with a partial array has started and preliminary results of the first test runs are presented. nonPeerReviewed

PhysicsHistoryMuonPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaAstrophysics::Instrumentation and Methods for AstrophysicsCosmic rayKnee regionComputer Science ApplicationsEducationNuclear physicsAstrohiukkasfysiikkaAir showerData recordingAstroparticle physics
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β-decay measurements ofA≃ 70 − 110 r-process nuclei at the National Superconducting Cyclotron Laboratory

2011

The present paper reports on several r-process motivated β-decay experiments undertaken at the National Superconducting Cyclotron Laboratory. β-decay half-lives and β-delayed neutron-emission probabilities were measured for nuclei around the r-process A = 70–80 and A = 90 – 110 mass regions. The data are discussed on the basis of quasi-random phase approximation calculations. The emphasis is made on the impact of these data upon calculations of r-process abundances.

PhysicsHistoryNeutron emissionHadronCyclotronComputer Science ApplicationsEducationlaw.inventionNuclear physicslawr-processNeutronAtomic physicsNucleonRandom phase approximationRadioactive decayJournal of Physics: Conference Series
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Improving on numerical simulations of nonlinear CMB anisotropies

2015

An Adaptative-Particle-Particle-Particle-Mesh code (HYDRA) plus a ray-tracing procedure was used in [1] to perform an exhaustive analysis of the weak lensing anisotropy. Other nonlinear Cosmic Microwave Background anisotropies, such as the Rees-Sciamaand the Sunyaev-Zel.dovicheffects are also being studied by using the same tools. Here we present some advances in our study of these nonlinear anisotropies. The primary advance is due to the use of better simulations with greater particle densities and appropriate softening, although other parameters have also been adjusted to get better estimates. Thus, we improve on a previous paper [2] where the Rees-Sciamaeffect was studied with Particle-M…

PhysicsHistoryNonlinear systemCosmic microwave backgroundResolution improvementAstrophysics::Cosmology and Extragalactic AstrophysicsStatistical physicsFocus (optics)AnisotropySofteningWeak gravitational lensingComputer Science ApplicationsEducationJournal of Physics: Conference Series
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