Search results for "Cathode ray"

showing 10 items of 96 documents

First transmission of electrons and ions through the KATRIN beamline

2018

The Karlsruhe Tritium Neutrino (KATRIN) experiment is a large-scale effort to probe the absolute neutrino mass scale with a sensitivity of 0.2 eV (90% confidence level), via a precise measurement of the endpoint spectrum of tritium β-decay. This work documents several KATRIN commissioning milestones: the complete assembly of the experimental beamline, the successful transmission of electrons from three sources through the beamline to the primary detector, and tests of ion transport and retention. In the First Light commissioning campaign of autumn 2016, photoelectrons were generated at the rear wall and ions were created by a dedicated ion source attached to the rear section; in July 2017, …

Physics - Instrumentation and DetectorsIon beamFOS: Physical sciencesbeam transportion: beam[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]KATRIN7. Clean energy01 natural sciencesIonNuclear physics0103 physical sciences[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]electron: beam010306 general physicsInstrumentation[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear ExperimentMathematical Physicsactivity reportPhysics010308 nuclear & particles physicsphotoelectron: emissionInstrumentation and Detectors (physics.ins-det)Photoelectric effectstabilitysensitivityIon sourceddc:BeamlineCathode rayNeutrinoperformanceKATRIN
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Beam normal spin asymmetry for the ep→eΔ(1232) process

2017

We calculate the single spin asymmetry for the $e p \to e \Delta(1232)$ process, for an electron beam polarized normal to the scattering plane. Such single spin asymmetries vanish in the one-photon exchange approximation, and are directly proportional to the absorptive part of a two-photon exchange amplitude. As the intermediate state in such two-photon exchange process is on its mass shell, the asymmetry allows one to access for the first time the on-shell $\Delta \to \Delta$ as well as $N^\ast \to \Delta$ electromagnetic transitions. We present the general formalism to describe the $e p \to e \Delta$ beam normal spin asymmetry, and provide a numerical estimate of its value using the nucle…

Physics010308 nuclear & particles physicsScatteringmedia_common.quotation_subject01 natural sciencesAsymmetryFormalism (philosophy of mathematics)AmplitudeQuantum mechanics0103 physical sciencesCathode rayIntermediate state010306 general physicsNucleonNuclear theorymedia_commonPhysical Review D
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The First Terrestrial Electron Beam Observed by the Atmosphere‐Space Interactions Monitor

2019

We report the first Terrestrial Electron Beam detected by the Atmosphere‐Space Interactions Monitor. It happened on 16 September 2018. The Atmosphere‐Space Interactions Monitor Modular X and Gamma ray Sensor recorded a 2 ms long event, with a softer spectrum than typically recorded for Terrestrial Gamma ray Flashes (TGFs). The lightning discharge associated to this event was found in the World Wide Lightning Location Network data, close to the northern footpoint of the magnetic field line that intercepts the International Space Station location. Imaging from a GOES‐R geostationary satellite shows that the source TGF was produced close to an overshooting top of a thunderstorm. Monte‐Carlo si…

Physics010504 meteorology & atmospheric sciencesElectronSpace (mathematics)01 natural sciencesComputational physicsAtmosphereGeophysicsEarth's magnetic fieldPositron13. Climate actionSpace and Planetary ScienceCathode rayThunderstorm0105 earth and related environmental sciencesJournal of Geophysical Research: Space Physics
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Constraining spectral models of a terrestrial gamma‐ray flash from a terrestrial electron beam observation by the Atmosphere‐Space Interactions Monit…

2021

Terrestrial Gamma ray Flashes (TGFs) are short flashes of high energy photons, produced by thunderstorms. When interacting with the atmosphere, they produce relativistic electrons and positrons, and a part gets bounded to geomagnetic field lines and travels large distances in space. This phenomenon is called a Terrestrial Electron Beam (TEB). The Atmosphere-Space Interactions Monitor (ASIM) mounted on-board the International Space Station detected a new TEB event on March 24, 2019, originating from the tropical cyclone Johanina. Using ASIM's low energy detector, the TEB energy spectrum is resolved down to 50 keV. We provide a method to constrain the TGF source spectrum based on the detected…

PhysicsAtmosphereGeophysicsCathode rayGeneral Earth and Planetary SciencesSpace (mathematics)Computational physicsTerrestrial gamma-ray flash
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Observation of electronic and geometric shell structures of small silver clusters

1999

Singly charged silver clusters Open image in new window in the size range n = 17 to n = 78 have been captured and stored in a Penning trap, size selected and subjected to an electron beam which leads to further ionization as well as dissociation. The resulting abundance spectra of doubly and triply charged clusters show several features: (1) A critical size for the production of doubly charged clusters which can be understood in terms of the decay pathways as previously investigated by collision induced dissociation, (2) an odd-even alternation in the abundance of singly and doubly charged clusters which inverses sign with change of charge state, (3) prominent signals for particular doubly …

PhysicsCollision-induced dissociationIonizationCathode rayAlternation (geometry)Atomic physicsPenning trapAtomic and Molecular Physics and OpticsDissociation (chemistry)Spectral lineCharged speciesThe European Physical Journal D
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Influence of an Electron Beam Exposure on the Surface Plasmon Resonance of Gold Nanoparticles

2013

Electron beam imaging is a common technique used for characterizing the morphology of plasmonic nanostructures. During the imaging process, the electron beam interacts with traces of organic material in the chamber and produces a well-know layer of amorphous carbon over the specimen under investigation. In this paper, we investigate the effect of this carbon adsorbate on the spectral position of the surface plasmon in individual gold nanoparticles as a function of electron exposure dose. We find an optimum dose for which the plasmonic response of the nanoparticle is not affected by the imaging process. The final publication is available at link.springer.com

PhysicsCondensed Matter - Mesoscale and Nanoscale Physicsbusiness.industrySurface plasmonBiophysicsFOS: Physical sciencesNanoparticle02 engineering and technologyElectron010402 general chemistry021001 nanoscience & nanotechnology01 natural sciencesBiochemistry0104 chemical sciencesAmorphous carbonColloidal goldMesoscale and Nanoscale Physics (cond-mat.mes-hall)Cathode rayOptoelectronicsSurface plasmon resonance0210 nano-technologybusinessPlasmonBiotechnologyPlasmonics
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Gyrotron interaction simulations with tapered magnetostatic field

2010

We investigate the interaction of the electron beam with the RF wave in a gyrotron, in the presence of an axially tapered magnetic field. The simulation results of three interaction codes are compared and the different modelings are discussed.

PhysicsCondensed matter physicsField (physics)Terahertz radiationCyclotronMagnetostaticsComputational physicsMagnetic fieldlaw.inventionlawGyrotronCathode rayPhysics::Accelerator PhysicsAxial symmetry35th International Conference on Infrared, Millimeter, and Terahertz Waves
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On the Line Shape of Backward Emitted Parametric X-Radiation

2002

Parametric X radiation, emitted in opposite direction of an electron which traverses a semi infinite single crystal on a hypothetical straight trajectory, features a Lorentzian line shape with extremely narrow width. However, small angle scattering of the electron in the Coulomb potential of the crystal atoms results in a stochastic change of the electron direction. The latter leads to a line broadening which can be understood essentially as a stochastic frequency modulation of the exponentially damped wave train. The line shape has been calculated analytically by well known probabilistic methods. Results are quoted for various reflections of a silicon single crystal at an electron beam ene…

PhysicsCrystalCathode rayElectric potentialElectronRadiationSmall-angle scatteringAtomic physicsSingle crystalLine (formation)
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Forward diffracted parametric X radiation from a silicon single crystal

2005

Experiments were performed with the 855 MeV electron beam of the Mainz Microtron MAMI which focused on still open questions in the X-ray emission process upon traversal of ultra relativistic electrons through single crystals. To elucidate the quest of kinematical versus dynamical production of PXR the radiation from silicon single crystal targets, emitted close to the electron direction, has been studied. The observed interference structures show that PXR is produced in a dynamical process.

PhysicsDiffractionNuclear and High Energy PhysicsSiliconbusiness.industryAstrophysics::High Energy Astrophysical Phenomenachemistry.chemical_elementElectronRadiationOpticschemistryInterference (communication)Cathode rayAtomic physicsNuclear ExperimentbusinessInstrumentationMicrotronSingle crystalNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Performances of the Alpha-X RF gun on the PHIL accelerator at LAL

2015

International audience; The Alpha-X RF-gun was designed to produce an ultra-short (<100 fs rms), 100 pC and 6.3 MeV electron beam with a normalized rms transverse emittance of 1π mm mrad for a gun peak accelerating field of 100 MV/m. Such beams will be required by the Alpha-X project, which aims to study a laser-driven plasma accelerator with a short wavelength accelerating medium. It has been demonstrated on PHIL (Photo-Injector at LAL) that the coaxial RF coupling, chosen to preserve the gun field cylindrical symmetry, is perfectly understood and allows reaching the required peak accelerating field of 100 MV/m giving beam energy of 6.3 MeV. Moreover, a quite low beam rms relative energy s…

PhysicsElectron beamNuclear and High Energy PhysicsBeam dynamicsbusiness.industryRF-gun[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Solenoid7. Clean energyNuclear physicsTransverse planeOpticsMagnetCathode rayPhotocathodesPhysics::Accelerator PhysicsThermal emittanceCoaxialSchottky effectbusinessInstrumentationBeam (structure)Electron gun
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