Search results for "Physics - Accelerator Physics"

showing 10 items of 19 documents

Controlled turbulence regime of electron cyclotron resonance ion source for improved multicharged ion performance

2020

Fundamental studies of excitation and non-linear evolution of kinetic instabilities of strongly nonequlibrium hot plasmas confined in open magnetic traps suggest new opportunities for fine-tuning of conventional electron cyclotron resonance (ECR) ion sources. These devices are widely used for the production of particle beams of high charge state ions. Operating the ion source in controlled turbulence regime allows increasing the absorbed power density and therefore the volumetric plasma energy content in the dense part of the discharge surrounded by the ECR surface, which leads to enhanced beam currents of high charge state ions. We report experiments at the ECR ion source at the JYFL accel…

010302 applied physicsAccelerator Physics (physics.acc-ph)Materials scienceAcoustics and UltrasonicsIon beamFOS: Physical sciencesPlasmaCondensed Matter PhysicsKinetic energy7. Clean energy01 natural sciencesElectron cyclotron resonanceIon sourcePhysics - Plasma Physics010305 fluids & plasmasSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsIonPlasma Physics (physics.plasm-ph)Physics::Plasma Physics0103 physical sciencesPhysics - Accelerator PhysicsAtomic physicsExcitationBeam (structure)
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Design study for a 500 MeV positron beam at the Mainz Microtron MAMI

2022

A design study has been performed for a positron beam with an energy of 500 MeV to be realized at the applied physics area of the Mainz Microtron MAMI. Positrons will be created after pair conversion of bremsstrahlung, produced by the 855 MeV electron beam af MAMI in a tungsten converter target. From the two conceivable geometries (i) pair conversion in the bremsstrahlung converter target itself, and (ii) bremsstrahlung pair conversion in a separated lead foil, the former was considered in detail. Positrons will be energy selected within an outside open electron beam-line bending magnet, and bent back by an additional sector magnet. Magnetic focusing elements in between are designed to prep…

Accelerator Physics (physics.acc-ph)530 PhysicsPhysics::Instrumentation and DetectorsPhysics::Accelerator PhysicsFOS: Physical sciencesPhysics - Accelerator Physics530 PhysikNuclear ExperimentAtomic and Molecular Physics and Optics
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Optical absorption of divalent metal tungstates: Correlation between the band-gap energy and the cation ionic radius

2008

We have carried out optical-absorption and reflectance measurements at room temperature in single crystals of AWO4 tungstates (A = Ba, Ca, Cd, Cu, Pb, Sr, and Zn). From the experimental results their band-gap energy has been determined to be 5.26 eV (BaWO4), 5.08 eV (SrWO4), 4.94 eV (CaWO4), 4.15 eV (CdWO4), 3.9-4.4 eV (ZnWO4), 3.8-4.2 eV (PbWO4), and 2.3 eV (CuWO4). The results are discussed in terms of the electronic structure of the studied tungstates. It has been found that those compounds where only the s electron states of the A2+ cation hybridize with the O 2p and W 5d states (e.g BaWO4) have larger band-gap energies than those where also p, d, and f states of the A2+ cation contribu…

Accelerator Physics (physics.acc-ph)Condensed Matter - Materials ScienceMaterials scienceIonic radiusBand gapAnalytical chemistryMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciencesGeneral Physics and AstronomyElectronic structureElectronReflectivityDivalent metalValence bandPhysics - Accelerator PhysicsAbsorption (electromagnetic radiation)EPL (Europhysics Letters)
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Present status and first results of the final focus beam line at the KEK Accelerator Test Facility

2011

ATF2 is a final-focus test beam line which aims to focus the low emittance beam from the ATF damping ring to a vertical size of about 37 nm and to demonstrate nanometer level beam stability. Several advanced beam diagnostics and feedback tools are used. In December 2008, construction and installation were completed and beam commissioning started, supported by an international team of Asian, European, and U.S. scientists. The present status and first results are described.

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsLow emittancePhysics and Astronomy (miscellaneous)Nuclear engineering[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]FOS: Physical sciencesbeam transport01 natural sciencesBeam characteristicslaw.inventionNuclear physicslaw0103 physical sciencesddc:530lcsh:Nuclear and particle physics. Atomic energy. RadioactivityBeam handling010306 general physicsAccelerator Test FacilityPhysicsFocus (computing)Research Groups and Centres\Physics\Low Temperature Physics010308 nuclear & particles physicsFaculty of Science\PhysicsBeam commissioningFísicaParticle acceleratorSurfaces and Interfaces29.27.Eg 29.27.Fh 29.20.dbAccelerators and Storage RingsStorage rings and collidersCOLLIDERSTechnology for normal conducting higher energy linear accelerators [9]BeamlineTest beamlcsh:QC770-798Physics - Accelerator PhysicsBeam (structure)
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New exotic beams from the SPIRAL 1 upgrade

2018

Since 2001, the SPIRAL 1 facility has been one of the pioneering facilities in ISOL techniques for reaccelerating radioactive ion beams: the fragmentation of the heavy ion beams of GANIL on graphite targets and subsequent ionization in the Nanogan ECR ion source has permitted to deliver beams of gaseous elements (He, N, O, F, Ne, Ar, Kr) to numerous experiments. Thanks to the CIME cyclotron, energies up to 20 AMeV could be obtained. In 2014, the facility was stopped to undertake a major upgrade, with the aim to extend the production capabilities of SPIRAL 1 to a number of new elements. This upgrade, which is presently under commissioning, consists in the integration of an ECR booster in the…

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsNuclear engineering[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]tutkimuslaitteetCyclotronFOS: Physical scienceshiukkaskiihdyttimet[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-ex7. Clean energy01 natural sciencesIonlaw.inventionion sourceslawIonization0103 physical sciencesIon sourcesNuclear Physics - ExperimentNuclear Experiment (nucl-ex)radioactive ion beams010306 general physicsNuclear ExperimentInstrumentationRadioactive ion beamsphysics.acc-ph[PHYS]Physics [physics]Physics010308 nuclear & particles physicsAccelerators and Storage RingsIon sourceUpgradesäteilyfysiikkaBeamlinePhysics - Accelerator PhysicsAGATABeam (structure)
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Fast photon detection for particle identification with COMPASS RICH-1

2006

Particle identification at high rates is an important challenge for many current and future high-energy physics experiments. The upgrade of the COMPASS RICH-1 detector requires a new technique for Cherenkov photon detection at count rates of several $10^6$ per channel in the central detector region, and a read-out system allowing for trigger rates of up to 100 kHz. To cope with these requirements, the photon detectors in the central region have been replaced with the detection system described in this paper. In the peripheral regions, the existing multi-wire proportional chambers with CsI photocathode are now read out via a new system employing APV pre-amplifiers and flash ADC chips. The ne…

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsPhotomultiplierPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsCherenkov detectorOther Fields of PhysicsFOS: Physical sciencesCOMPASS; RICH; Multi-anode PMT; Particle identificationCOMPASSParticle identificationPhotocathodelaw.inventionParticle identificationNuclear physicsOpticsMulti-anode PMTlawCompassCOMPASS; RICHInstrumentationRICHCherenkov radiationPhysicsbusiness.industryDetectorInstrumentation and Detectors (physics.ins-det)UpgradePhysics - Accelerator PhysicsHigh Energy Physics::Experimentbusiness
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Vertical Beam Polarization at MAMI

2017

For the first time a vertically polarized electron beam has been used for physics experiments at MAMI in the energy range between 180 and 855 MeV. The beam-normal single-spin asymmetry $A_{\mathrm{n}}$, which is a direct probe of higher-order photon exchange beyond the first Born approximation, has been measured in the reaction $^{12}\mathrm C(\vec e,e')^{12}\mathrm C$. Vertical polarization orientation was necessary to measure this asymmetry with the existing experimental setup. In this paper we describe the procedure to orient the electron polarization vector vertically, and the concept of determining both its magnitude and orientation with the available setup. A sophisticated method has …

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhotonmedia_common.quotation_subjectVertical polarization[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]FOS: Physical sciencesElectron acceleratorElectronMott polarimeter01 natural sciencesAsymmetrylaw.inventionOpticsMøller polarimeterlaw0103 physical sciencesCompton polarimeter[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det][ PHYS.PHYS.PHYS-ACC-PH ] Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Born approximation010306 general physicsNuclear Experiment[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Instrumentationmedia_commonPhysicsWien filter010308 nuclear & particles physicsbusiness.industryParticle acceleratorPolarimeterInstrumentation and Detectors (physics.ins-det)Wien filterPolarization (waves)Electron accelerator ; Vertical polarization ; Wien filter ; Compton polarimeter ; Mott polarimeter ; Møller polarimeterPhysics - Accelerator Physicsbusiness
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Polarization-Dependent Disappearance of a Resonance Signal -- Indication for Optical Pumping in a Storage Ring?

2021

We report on laser spectroscopic measurements on Li$^+$ ions in the experimental storage ring ESR at the GSI Helmholtz Centre for Heavy Ion Research. Driving the $2s\,^3\!{S}_1\;(F=\frac{3}{2}) \,\leftrightarrow\,2p\,^3\!P_2\;(F=\frac{5}{2}) \leftrightarrow 2s\,^3\!{S}_1\;(F=\frac{5}{2})$ $\Lambda$-transition in $^7$Li$^+$ with two superimposed laser beams it was found that the use of circularly polarized light leads to a disappearance of the resonance structure in the fluorescence signal. This can be explained by optical pumping into a dark state of polarized ions. We present a detailed theoretical analysis of this process that supports the interpretation of optical pumping and demonstrate…

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)Atomic Physics (physics.atom-ph)FOS: Physical sciences53001 natural sciencesIonlaw.inventionPhysics - Atomic PhysicsOptical pumpinglaw0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivityddc:530010306 general physicsCircular polarizationPhysics010308 nuclear & particles physicsSurfaces and InterfacesLaserPolarization (waves)FluorescenceDark statelcsh:QC770-798Physics - Accelerator PhysicsAtomic physicsStorage ring
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Direct Measurement of Focusing Fields in Active Plasma Lenses

2018

Physical review accelerators and beams 21(12), 122801 (2018). doi:10.1103/PhysRevAccelBeams.21.122801

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)Field (physics)FOS: Physical sciences01 natural sciences530law.inventionOpticslaw0103 physical sciencesddc:530Thermal emittancelcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsphysics.acc-phPhysics010308 nuclear & particles physicsbusiness.industrySurfaces and InterfacesPlasmaNuclear & Particles PhysicsLens (optics)Physics::Space PhysicsPhysical SciencesCathode raylcsh:QC770-798Physics::Accelerator PhysicsPhysics - Accelerator PhysicsBeam emittancebusinessCharged particle beamBeam (structure)
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Simulations and measurements of beam loss patterns at the CERN Large Hadron Collider

2014

The CERN Large Hadron Collider (LHC) is designed to collide proton beams of unprecedented energy, in order to extend the frontiers of high-energy particle physics. During the first very successful running period in 2010-2013, the LHC was routinely storing protons at 3.5-4 TeV with a total beam energy of up to 146 MJ, and even higher stored energies are foreseen in the future. This puts extraordinary demands on the control of beam losses. An uncontrolled loss of even a tiny fraction of the beam could cause a superconducting magnet to undergo a transition into a normal-conducting state, or in the worst case cause material damage. Hence a multistage collimation system has been installed in ord…

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)Monte Carlo methodFOS: Physical sciencesSuperconducting magnetTracking (particle physics)law.inventionNuclear physicslawlcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment (nucl-ex)Large Hadron Collider (France and Switzerland)Nuclear ExperimentPhysicsLarge Hadron ColliderColliders (Nuclear physics)Particle acceleratorCollimatorSurfaces and InterfacesAccelerators and Storage RingsOrders of magnitude (time)lcsh:QC770-798Physics::Accelerator PhysicsPhysics - Accelerator PhysicsBeam (structure)
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