Search results for "Cathode ray"

showing 10 items of 96 documents

Polarization transfer in then 2 P-excitation of alkali atoms by longitudinally polarized electrons

1989

In (ns — np)-excitation of alkali atoms by polarized electrons some of the spin orientation of the primary electron beam is transfered to the excited atoms because of exchange collisions. In the present work the polarization transfer to Na, K, Rb, and Cs respectively is studied by looking for the circular light polarization of (np — ns)-decay radiation emitted in forward direction following impact excitation by a beam of longitudinally polarized electrons. Maximum polarization transfers are observed at collision energies with values about 1.5 times that ofnp-thresholds. The transfer increases with increasing atomic number. In case of (6s — 6p)-excitation of cesium 45% of primary electron sp…

PhysicsExcited stateCathode rayPhysics::Atomic PhysicsAtomic numberElectronAtomic physicsSpin (physics)Polarization (waves)Atomic and Molecular Physics and OpticsExcitationBeam (structure)Zeitschrift f�r Physik D Atoms, Molecules and Clusters
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Channeling and Radiation of Electrons in Silicon Single Crystals and Si1−xGexCrystalline Undulators

2013

The phenomenon of channeling and the basic features of channeling radiation emission are introduced in a pedestrian way. Both, radiation spectra as well as dechanneling length measurements at electron beam energies between 195 and 855 MeV feature quantum state phenomena for the (110) planar potential of the silicon single crystals. Radiation from a crystalline undulator, produced at the Aarhus University (UAAR), has been investigated at the Mainz Microtron electron accelerator facility MAMI. The 4-period epitaxially grown strained layer Si1−xGex undulator had a period length λu = 9.9 μm. At a beam energy of 375 MeV a broad excess yield around the theoretically expected photon energy of 0.13…

PhysicsHistorySiliconchemistry.chemical_elementParticle acceleratorElectronPhoton energyRadiationUndulatorComputer Science ApplicationsEducationlaw.inventionchemistrylawCathode rayPhysics::Accelerator PhysicsAtomic physicsNuclear ExperimentMicrotronJournal of Physics: Conference Series
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Design of a double-gap Hughes-type coupled-cavity for a Ka-band Extended Interaction Klystron

2020

In this paper, the design of a Ka-band Extended-Interaction Klystron (EIK) working at 2$\pi$ mode. The interaction structure is a three-gap Hughes-type coupled-cavity. Based on the results obtained with the 3D model developed by using CST, “cold electrical parameters” have been calculated, necessary to measure the interaction with the electron beam. The structure stability and the synchronization with the electron beam are analyzed The large-signal analysis is performed by 1D software AJDISK. Under the beam voltage and current of 19.55 kV and 0.95 A, respectively, an RF output power value of 3.86 kW and a bandwidth gain value of 37. 06 dB have been obtained

PhysicsKlystronbusiness.industryextended interaction klystron coupled-cavity Hughes cavity multi-gapBandwidth (signal processing)Measure (mathematics)Settore ING-INF/01 - Elettronicalaw.inventionPower (physics)Synchronization (alternating current)OpticslawCathode rayKa bandRadio frequencybusiness
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Mono-energetic electron induced single-event effects at the VESPER facility

2016

We present experimental evidence of electron induced upsets in a reference ESA SEU monitor, the SEU based particle detector, induced by 200 MeV electron beam at the VESPER facility at CERN. Comparison of experimental cross sections and simulated cross sections are shown and the differences are analyzed. Possible secondary contributions to the upset rate by neutrons and cumulative dose effects are discussed, showing that electronuclear reactions are the expected SEU mechanism. Insight is given as to possible overall electron contribution to the upset rates in the Jovian radiation environment inside a typical spacecraft shielding are evaluated.

PhysicsLarge Hadron Collider010308 nuclear & particles physicsElectronRadiation01 natural sciencesUpsetParticle detectorNuclear physics0103 physical sciencesElectromagnetic shieldingCathode rayNeutron010306 general physics2016 16th European Conference on Radiation and Its Effects on Components and Systems (RADECS)
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The REX-ISOLDE project

2002

REX-ISOLDE is a pilot experiment at ISOLDE/CERN to study the structure of neutron-rich nuclei (N=20, N=28) with post-accelerated radioactive ion beams (1). Therefore radioactive ions with charge state 1+, which are delivered by the online mass separator ISOLDE, are accelerated up to 2.2 MeV/u by means of a new concept. The radioactive ions are first accumulated in a Penning trap, then charge breeded to a charge-to-mass ratio of 1/4.5 in an Electron Beam Ion Source (EBIS) and finally accelerated. The LINAC consists of three components, namely a Radio Frequency Quadrupole (RFQ) accelerator, which accelerates the ions from 5 to 300 keV/u, an interdigital H-type structure (IH) with a final ener…

PhysicsLarge Hadron ColliderMass-to-charge ratioNuclear TheoryParticle acceleratorCoulomb excitationPenning trapLinear particle acceleratorIon sourceIonlaw.inventionNuclear physicsRadio-frequency quadrupolelawCathode rayPhysics::Accelerator PhysicsNeutronBeam emittanceAtomic physicsNuclear ExperimentProceedings of the 1997 Particle Accelerator Conference (Cat. No.97CH36167)
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Measurement and interpretation of the polarization of the x-ray line emission of heliumlike Fe XXV excited by an electron beam

1996

The linear polarization of the 1s2p${\mathrm{}}^{1}$${\mathit{P}}_{1}$\ensuremath{\rightarrow}1${\mathit{s}}^{2}$${\mathrm{}}^{1}$${\mathit{S}}_{0}$ resonance line, the 1s2p${\mathrm{}}^{3}$${\mathit{P}}_{1,2}$\ensuremath{\rightarrow}1${\mathit{s}}^{2}$${\mathrm{}}^{1}$${\mathit{S}}_{0}$ intercombination lines, and the 1s2s${\mathrm{}}^{3}$${\mathit{S}}_{1}$\ensuremath{\rightarrow}1${\mathit{s}}^{2}$${\mathrm{}}^{1}$${\mathit{S}}_{0}$ forbidden line was measured in heliumlike Fe XXV excited near threshold by a monoenergetic electron beam. The measurement was carried out with a high-resolution x-ray spectrometer employing a set of two analyzing crystals that acted as polarizers by selectivel…

PhysicsNear thresholdExcited stateCathode rayX-rayAtomic physicsAstrophysicsPolarization (waves)Forbidden mechanismResonance lineX ray spectraMicrophysicsAtomic and Molecular Physics and OpticsPhysical Review A
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Enhancement of the linear polarization of coherent bremsstrahlung by collimation of the photon beam

1998

A method is described to precisely predict the relative intensities and degrees of linear polarization of coherent bremsstrahlung from diamond crystals, taking into account the collimation of the photon beam and the lateral distribution and angular divergence of the electron beam in addition to the properties of the crystal. It is confirmed that the increase of the degree of linear polarization through collimation of the photon beam is a sizable effect. Compared to previous approaches considerable progress has been made in reproducing the experimentally observed relative intensities of collimated coherent bremsstrahlung, by taking into account the angular distribution of coherent bremsstrah…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsLinear polarizationAstrophysics::High Energy Astrophysical PhenomenaBremsstrahlung01 natural sciencesCollimated lightCrystalDistribution (mathematics)0103 physical sciencesCathode rayPhysics::Accelerator PhysicsRadial polarizationAtomic physics010306 general physicsDivergence (statistics)Physical Review C
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Precision electron beam polarimetry for next generation nuclear physics experiments

2018

Polarized electron beams have played an important role in scattering experiments at moderate to high beam energies. Historically, these experiments have been primarily targeted at studying hadronic structure — from the quark contribution to the spin structure of protons and neutrons, to nucleon elastic form factors, as well as contributions to these elastic form factors from (strange) sea quarks. Other experiments have aimed to place constraints on new physics beyond the Standard Model. For most experiments, knowledge of the magnitude of the electron beam polarization has not been a limiting systematic uncertainty, with only moderately precise beam polarimetry requirements. However, a new …

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsScatteringPolarimetryForm factor (quantum field theory)General Physics and AstronomyElectron01 natural sciencesNuclear physics0103 physical sciencesCathode rayPhysics::Accelerator Physics010306 general physicsNucleonElectron scatteringBeam (structure)International Journal of Modern Physics E
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Astrophysics and spectroscopy with microcalorimeters on an electron beam ion trap

2003

The importance of the combination of electron beam ion trap (EBIT) spectroscopy with X-ray microcalorimeters in the field of astrophysics was discussed. X-ray astronomy involves heavily charged ion instruments , especially EBIT, to obtain improved quality atomic data. In this regard, the research program at the National Institute of Standards and Technology, which uses X-ray spectroscopic methods to study plasma and atomic physics, was also discussed.

PhysicsNuclear and High Energy PhysicsAstrophysics::Instrumentation and Methods for AstrophysicsX-rayHighly charged ionSurfaces Coatings and FilmFizikai tudományokSurfaces and InterfacesPlasmaAstrophysicsHighly charged ionIonX-rayNuclear physicsSettore FIS/05 - Astronomia E AstrofisicaTermészettudományokMicrocalorimeterIonizationCathode rayAtomic physicsLaboratory astrophysicSpectroscopyElectron beam ion trapInstrumentationElectron beam ion trapNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Anomalous behavior of LiF:Mg,Cu,P (TLD100H) irradiated with electron beams

2006

Abstract Thermoluminescent dosimeters of LiF:Mg,Cu,P (TLD100H) were exposed to 60Co γ -ray, protons, high energy electrons and the glow curves were analyzed. We observed an unusual behavior of the TL response of dosimeters to 7 and 14 MeV electron beam. In fact the relative amplitude between two of the five peaks (2° and 3° peaks) assumes values smaller than the unity for doses up to 5 Gy and values greater than the unity for doses equal to or greater than 10 Gy. A possible explanation of this behavior is given adopting a model of the formation of the peaks 2° and 3° and examining the different ways of energy release in matter for each beam. To perform this analysis we deconvoluted the glow…

PhysicsNuclear and High Energy PhysicsDosimeterbusiness.industryTrappingElectronKinetic energyThermoluminescenceOpticsLETCathode rayTLD100HIrradiationAtomic physicsbusinessInstrumentationGOKBeam (structure)thermoluminescenceNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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