AIP conference proceedings · 2018 · 120 citations · 18 references
Positron Annihilation LifetimeEngineeringPositron Annihilation SpectroscopyAtomic Emission SpectroscopyAccelerator PhysicSynchrotron Radiation SourceDoppler Broadening SpectroscopyElectron SpectroscopyAccelerator TechnologyMaterials SciencePhysicsElbe FacilityPositron LifetimeSynchrotron RadiationNuclear AstrophysicsElectron BeamNatural SciencesSpectroscopyParticle PhysicsApplied PhysicsThin FilmsParticle Accelerator
The Helmholtz-Zentrum Dresden-Rossendorf operates a superconducting linear accelerator for electrons with energies up to 35 MeV and average beam currents up to 1.6 mA with bunch charges up to 120 pC. The electron beam is employed to produce several secondary beams including X-rays from bremsstrahlung production, coherent IR light in a Free Electron Laser, superradiant THz radiation, neutrons, and positrons. The secondary positron beam after moderation feeds the Monoenergetic Positron Source (MePS) where positron annihilation lifetime (PALS) and positron annihilation Doppler-broadening experiments in materials science are performed. The adjustable repetition rate of the continuous-wave electron beams allows matching of the pulse separation to the positron lifetime in the sample under study. The energy of the positron beam can be set between 0.5 keV and 20 keV to perform depth resolved defect spectroscopy and porosity studies especially for thin films. Bulk materials, fluids, gases, and even radioactive samples can be studied at the unique Gamma-induced Positron Source (GiPS) where an intense bremsstrahlung source generates positrons directly inside the material under study. A 22Na-based monoenergetic positron beam serves for offline experiments and additional depth-resolved Doppler-broadening studies complementing both accelerator-based sources.
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Purely antiferromagnetic magnetoelectric random access memory
Tobias Kosub, Martin Kopte, Ruben Hühne et al. · Nature Communications · 2017 · 296 citations · Full text