Search results for "facility"

showing 10 items of 139 documents

Performance studies of the P¯ANDA planar GEM-tracking detector in physics simulations

2018

Abstract The P ¯ ANDA experiment will be installed at the future facility for antiproton and ion research (FAIR) in Darmstadt, Germany, to study events from the annihilation of protons and antiprotons. The P ¯ ANDA detectors can cover a wide physics program about baryon spectroscopy and nucleon structure as well as the study of hadrons and hypernuclear physics including the study of excited hyperon states. One very specific feature of most hyperon ground states is the long decay length of several centimeters in the forward direction. The central tracking detectors of the P ¯ ANDA setup are not sufficiently optimized for these long decay lengths. Therefore, using a set of the planar GEM-trac…

PhysicsNuclear and High Energy PhysicsAnnihilation010308 nuclear & particles physicsNuclear TheoryHadronHyperon01 natural sciencesBaryonNuclear physicsAntiproton0103 physical sciencesGas electron multiplierFacility for Antiproton and Ion ResearchHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsNucleonInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Antihyperon potentials in nuclei via exclusive antiproton–nucleus reactions

2015

Abstract The exclusive production of hyperon–antihyperon pairs close to their production threshold in p ‾ -nucleus collisions offers a unique and hitherto unexplored opportunity to elucidate the behavior of antihyperons in nuclei. For the first time we analyze these reactions in a microscopic transport model using the Giesen Boltzmann–Uehling–Uhlenbeck transport model. The calculation takes the delicate interplay between the strong absorption of antihyperons, their rescattering and mean field deflection as well as the Fermi motion of the struck nucleon into account. We find a substantial sensitivity of transverse momentum correlations of coincident Λ ‾ Λ -pairs to the assumed depth of the Λ…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theorylcsh:QC1-999IonNuclear physicsmedicine.anatomical_structureDeflection (physics)Mean field theoryAntiprotonmedicineFacility for Antiproton and Ion ResearchNuclear ExperimentNucleonNucleuslcsh:PhysicsFermi Gamma-ray Space TelescopePhysics Letters B
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The PANDA Barrel DIRC detector

2014

Abstract The PANDA experiment at the new Facility for Antiproton and Ion Research in Europe (FAIR) at GSI, Darmstadt, will study fundamental questions of hadron physics and QCD using high-intensity cooled antiproton beams with momenta between 1.5 and 15 GeV/c. Efficient Particle Identification for a wide momentum range and the full solid angle is required for reconstructing the various physics channels of the PANDA program. Hadronic Particle Identification in the barrel region of the detector will be provided by a DIRC counter. The design is based on the successful BABAR DIRC with important improvements, such as focusing optics and fast photon timing. Several of these improvements, includin…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonLarge Hadron ColliderPhysics::Instrumentation and DetectorsHadronDetectorParticle identificationNuclear physicsConceptual designAntiprotonPhysics::Accelerator PhysicsFacility for Antiproton and Ion ResearchHigh Energy Physics::ExperimentNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Simulation and reconstruction of the PANDA Barrel DIRC

2014

Hadronic particle identification (PID) in the barrel region of the PANDA experiment at the new Facility for Antiproton and Ion Research in Europe (FAIR) at GSI, Darmstadt will be provided by a DIRC (Detection of Internally Reflected Cherenkov light) counter. To optimize the performance and reduce the detector cost, detailed simulations of different design elements, such as the width of the radiators, the shape of the expansion volume, and the type of focusing system, were performed using Geant. Custom reconstruction algorithms were developed to match the detector geometry. We will discuss the single photon resolution and photon yield as well as the PID performance for the Barrel DIRC baseli…

PhysicsNuclear and High Energy PhysicsPhotonPhysics::Instrumentation and DetectorsCherenkov detectorDetectorBarrel (horology)PID controllerParticle identificationlaw.inventionNuclear physicsDetection of internally reflected Cherenkov lightlawFacility for Antiproton and Ion ResearchHigh Energy Physics::ExperimentNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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High brilliance uranium beams for the GSI FAIR

2017

The 40 years old GSI-UNILAC (Universal Linear Accelerator) as well as the heavy ion synchrotron SIS18 will serve as a high current heavy ion injector for the new FAIR (Facility for Antiproton and Ion Research) synchrotron SIS100. In the context of an advanced machine investigation program in combination with the ongoing UNILAC upgrade program, a new uranium beam intensity record (11.5 emA, ${\mathrm{U}}^{29+}$) at very high beam brilliance was achieved recently in a machine experiment campaign. This is an important step paving the way to fulfill the FAIR heavy ion high intensity beam requirements. Results of high current uranium beam measurements applying a newly developed pulsed hydrogen g…

PhysicsNuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicschemistry.chemical_elementContext (language use)Surfaces and InterfacesUranium01 natural sciencesSynchrotronlaw.inventionNuclear physicsUpgradechemistrylawUniversal linear accelerator0103 physical sciencesPhysics::Accelerator PhysicsFacility for Antiproton and Ion Researchlcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment010306 general physicsIntensity (heat transfer)Beam (structure)Physical Review Accelerators and Beams
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The PANDA DIRC detectors

2020

Abstract The PANDA experiment at the future Facility for Antiproton and Ion Research (FAIR) will address fundamental questions of hadron physics with unprecedented precision. To reach this goal excellent Particle Identification (PID) is essential over a large range of particle momenta and solid angles. Most of the phase space will be covered by two innovative DIRC (Detection of Internally Reflected Cherenkov light) detectors. The Endcap Disc DIRC and Barrel DIRC will cover the polar angle range from 5 to 22°and 22 to 140°, respectively. Both detectors rely on high precision optical components, lifetime-enhanced Microchannel Plate PMTs (MCP-PMTs), and fast readout electronics.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Physics::Instrumentation and Detectors010308 nuclear & particles physicsCherenkov detectorbusiness.industryDetectorSolid angle01 natural sciencesParticle identificationlaw.inventionOpticslawDetection of internally reflected Cherenkov light0103 physical sciencesFacility for Antiproton and Ion ResearchHigh Energy Physics::ExperimentMicrochannel plate detector010306 general physicsbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Characterization of a new modular decay total absorption gamma-ray spectrometer (DTAS) for FAIR

2013

Beta-decay studies are one of the main goals of the DEcay SPECtroscopy experiment (DESPEC) to be installed at the future Facility for Antiproton and Ion Research (FAIR). DESPEC aims at the study of nuclear structure of exotic nuclei. A new modular Decay Total Absorption gamma-ray Spectrometer (DTAS) is being built at IFIC and is specially adapted to studies at fragmentation facilities such as the Super Fragment Separator (Super-FRS) at FAIR. The designed spectrometer is composed of 16 identical NaI(Tl) scintillation crystals. This work focuses on the characterization of these independent modules, as an initial step for the characterization of the full spectrometer. Monte Carlo simulations h…

PhysicsNuclear physicsSpectrometerPhysics::Instrumentation and DetectorsDouble beta decayDetectorMonte Carlo methodNuclear structureFacility for Antiproton and Ion ResearchGamma spectroscopyNuclear ExperimentSpectroscopyAIP Conference Proceedings
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Status of the PANDA Barrel DIRC

2014

The PANDA experiment at the future Facility for Antiproton and Ion Research in Europe GmbH (FAIR) at GSI, Darmstadt will study fundamental questions of hadron physics and QCD using high-intensity cooled antiproton beams with momenta between 1.5 and 15 GeV/c. Hadronic PID in the barrel region of the PANDA detector will be provided by a DIRC (Detection of Internally Reflected Cherenkov light) counter. The design is based on the successful BABAR DIRC with several key improvements, such as fast photon timing and a compact imaging region. Detailed Monte Carlo simulation studies were performed for DIRC designs based on narrow bars or wide plates with a variety of focusing solutions. The performan…

PhysicsParticle physicsLarge Hadron ColliderPhotonPhysics::Instrumentation and DetectorsDetectorParticle identificationNuclear physicsDetection of internally reflected Cherenkov lightAntiprotonPhysics::Accelerator PhysicsFacility for Antiproton and Ion ResearchHigh Energy Physics::ExperimentNuclear ExperimentInstrumentationMathematical PhysicsCherenkov radiationJournal of Instrumentation
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The PANDA Barrel DIRC

2016

The PANDA detector at the international accelerator Facility for Antiproton and Ion Research in Europe (FAIR) addresses fundamental questions of hadron physics. Experiments concerning charmonium spectroscopy, the search for hybrids and glueballs and the interaction of hidden and open charm particles with nucleons and nuclei will be performed with antiproton beams impinging on hydrogen or nuclear targets. Cooled beams allow the precision scan of resonances in formation experiments. The momentum range of the antiproton beam between 1.5 GeV/c and 15 GeV/c tests predictions by perturbation theory and will reveal deviations originating from strong QCD . An excellent hadronic particle identificat…

PhysicsPhotonLarge Hadron Collider010308 nuclear & particles physicsHadron01 natural sciences7. Clean energyParticle identificationNuclear physicsDetection of internally reflected Cherenkov lightAntiproton0103 physical sciencesPhysics::Accelerator PhysicsFacility for Antiproton and Ion ResearchHigh Energy Physics::Experimentddc:610Nuclear Experiment010306 general physicsInstrumentationMathematical PhysicsCherenkov radiation
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Low Energy Protons at RADEF - Application to Advanced eSRAMs

2014

A low energy proton facility has been developed at RADEF, Jyvskyl, Finland. The proton energy selection, calibration and dosimetry are described. The first experiment with external users was performed using two memory test vehicles fabricated with 28 nm technology. Examples of single event upset measurements in the test vehicles embedded SRAMs (eSRAMs) as a function of proton energy are provided.

PhysicsProtonta114ta213business.industryNuclear engineeringElectrical engineeringProton energySEE testLow energyLow energy proton facilitySingle event upsetCalibrationDosimetryMemory testbusiness
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