Search results for " high energy physics"

showing 10 items of 8412 documents

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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International workshop on next generation gamma-ray source

2022

Journal of physics / G 49(1), 010502 (2022). doi:10.1088/1361-6471/ac2827

Accelerator Physics (physics.acc-ph)Nuclear and High Energy Physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear Theorynucleon: structurepi: photoproduction[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]conference summarynuclear astrophysicsFOS: Physical scienceslow-energy QCD[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530bremsstrahlung01 natural scienceselectron: acceleratorNuclear Theory (nucl-th)parity: violationnuclear physicsquantum chromodynamics0103 physical sciencesAgency (sociology)ddc:530gamma-rayApplied researchNuclear Experiment (nucl-ex)010306 general physicsphoton: beamNuclear Experimentactivity reportenergy: lowPhysicsastrophysics010308 nuclear & particles physicsInformation sharinglaserhadronic parity violationgamma raynuclear structureSystems engineeringPhysics - Accelerator PhysicsCompton scatteringJournal of Physics G: Nuclear and Particle Physics
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Highly efficient isotope separation and ion implantation of  163Ho for the ECHo project

2019

Abstract The effective electron neutrino mass measurement in the framework of the ECHo experiment requires radiochemically pure 163 Ho, which is ion implanted into detector absorbers. To meet the project specifications in efficiency and purity, the entire process chain of ionization, isotope separation , and implantation of 163Ho was optimized. A new two-step resonant laser ionization scheme was established at the 30 kV magnetic mass separator RISIKO. For ionization and separation, an average efficiency of 69 ( 5 )  stat(4)sys% was achieved using intra-cavity frequency doubled Ti:sapphire lasers. The implantation of undesired 166 m Ho, which is present in trace amounts in the initial  163Ho…

Accelerator Physics (physics.acc-ph)PhysicsNuclear and High Energy PhysicsAtomic Physics (physics.atom-ph)Orders of magnitude (temperature)DetectorAnalytical chemistryFOS: Physical sciencesLaser01 natural sciencesPhysics - Atomic Physics010305 fluids & plasmasIsotope separationlaw.inventionIonIon implantationlawIonization0103 physical sciencesSapphirePhysics - Accelerator Physics010306 general physicsInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Characterization and Tuning of Ultra High Gradient Permanent Magnet Quadrupoles

2009

The application of quadrupole devices with high field gradients and small apertures requires precise control over higher order multipole field components. We present a new scheme for performance control and tuning, which allows the illumination of most of the quadrupole device aperture because of the reduction of higher order field components. Consequently, the size of the aperture can be minimized to match the beam size achieving field gradients of up to $500\text{ }\text{ }\mathrm{T}\text{ }{\mathrm{m}}^{\ensuremath{-}1}$ at good imaging quality. The characterization method based on a Hall probe measurement and a Fourier analysis was confirmed using the high quality electron beam at the M…

Accelerator Physics (physics.acc-ph)electron beamNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorscompactmagneticlensPhysics and Astronomy (miscellaneous)Field (physics)AperturemultipoleFOS: Physical sciencespermanenthalbachx-felNuclear magnetic resonancetuningquadrupolelcsh:Nuclear and particle physics. Atomic energy. RadioactivityQuadrupole magnetMicrotronPhysicsOrder (ring theory)Surfaces and InterfacesInstrumentation and Detectors (physics.ins-det)beam focusingComputational physicsMagnetQuadrupolelcsh:QC770-798Physics::Accelerator PhysicsPhysics - Accelerator PhysicsMultipole expansion
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Developments towards in-gas-jet laser spectroscopy studies of actinium isotopes at LISOL

2015

To study exotic nuclides at the borders of stability with laser ionization and spectroscopy techniques, highest efficiencies in combination with a high spectral resolution are required. These usually opposing requirements are reconciled by applying the in-gas-laser ionization and spectroscopy (IGLIS) technique in the supersonic gas jet produced by a de Laval nozzle installed at the exit of the stopping gas cell. Carrying out laser ionization in the low-temperature and low density supersonic gas jet eliminates pressure broadening, which will significantly improve the spectral resolution. This article presents the required modifications at the Leuven Isotope Separator On-Line (LISOL) facility…

ActiniumNuclear and High Energy PhysicsRocket engine nozzleSeparator (oil production)chemistry.chemical_elementactinium[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesResonance ionization spectroscopylaw.inventionAtmospheric-pressure laser ionizationlawIonization0103 physical sciencesPhysics::Atomic Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsSpectroscopyInstrumentationGas jetJet (fluid)ta114010308 nuclear & particles physicsChemistrygas cellLaserActiniumresonance ionization spectroscopygas jetAtomic physicsGas cellNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Correlation of the highest-energy cosmic rays with nearby extragalactic objects.

2007

Using data collected at the Pierre Auger Observatory during the past 3.7 years, we demonstrated a correlation between the arrival directions of cosmic rays with energy above ~ 6x10^{19} electron volts and the positions of active galactic nuclei (AGN) lying within ~ 75 megaparsecs. We rejected the hypothesis of an isotropic distribution of these cosmic rays with at least a 99% confidence level from a prescribed a priori test. The correlation we observed is compatible with the hypothesis that the highest energy particles originate from nearby extragalactic sources whose flux has not been substantially reduced by interaction with the cosmic background radiation. AGN or objects having a similar…

Active galactic nucleus[SDU.ASTR.CO]Sciences of the Universe [physics]/Astrophysics [astro-ph]/Cosmology and Extra-Galactic Astrophysics [astro-ph.CO]AstronomyAstrophysics::High Energy Astrophysical Phenomenaparticle source [cosmic radiation]Cosmic background radiationFOS: Physical sciencesFluxOsservatorio Pierre AugerCosmic rayanisotropyAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysics01 natural sciences[PHYS.ASTR.CO]Physics [physics]/Astrophysics [astro-ph]/Cosmology and Extra-Galactic Astrophysics [astro-ph.CO]Raggi cosmici0103 physical sciencesUltra-high-energy cosmic ray010303 astronomy & astrophysicsBackground radiationNuclei galattivi attiviPhysicsPierre Auger ObservatorySPECTRUMMultidisciplinary[SDU.ASTR]Sciences of the Universe [physics]/Astrophysics [astro-ph]010308 nuclear & particles physicsMedicine (all); MultidisciplinaryMedicine (all)Settore FIS/01 - Fisica SperimentaleAstrophysics (astro-ph)angular dependence [cosmic radiation]Astrophysics::Instrumentation and Methods for AstrophysicsFísicaEnergia ultra altaExperimental High Energy Physicsddc:500Energy (signal processing)experimental results
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