Search results for "strah"

showing 10 items of 123 documents

Heavy isotopes of actinium: 229Ac, 230Ac, 231Ac and 232Ac

1973

Abstract By irradiation of 232Th with 150-MeV bremsstrahlung and with 14-MeV neutrons, three new neutron-rich isotopes of actinium, 230Ac, 231Ac and 232Ac, were produced and identified and the previously reported isotope, 229Ac, was confirmed. The actinium isotopes were chemically isolated by a fast procedure based on elution with α-hydroxyisobutyric acid from cation exchange resins. For 229Ac, a half-life of 62·7 ± 0·5 min and a β-ray energy of 1·14 ± 0·15 MeV were found; 35 γ-rays were observed, the strongest ones with the following energies and relative intensities: 135·3(34), 146·4(35), 164·6(100), 252·2(24), 261·9(39), 317·0(23), 539·9(20), 569·1(91), and 605·2 keV(23). For 230Ac, a ha…

Nuclear reactionActiniumIsotopes of actiniumPolymers and PlasticsIsotopeChemistryRadiochemistryMaterials ChemistryBremsstrahlungHalf-lifechemistry.chemical_elementIrradiationIsotopes of thoriumJournal of Inorganic and Nuclear Chemistry
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Photoproduction of $ \pi^{0}$ -pairs off protons and off neutrons

2015

Total cross sections, angular distributions, and invariant-mass distributions have been measured for the photoproduction of $\pi^0\pi^0$ pairs off free protons and off nucleons bound in the deuteron. The experiments were performed at the MAMI accelerator facility in Mainz using the Glasgow photon tagging spectrometer and the Crystal Ball/TAPS detector. The accelerator delivered electron beams of 1508 and 1557~MeV, which produced bremsstrahlung in thin radiator foils. The tagged photon beam covered energies up to 1400~MeV. The data from the free proton target are in good agreement with previous measurements and were only used to test the analysis procedures. The results for differential cros…

Nuclear reactionPhysicsNuclear and High Energy PhysicsProtonMesonNuclear TheoryBremsstrahlung7. Clean energyDelta baryonNuclear physicsPhysics::Accelerator PhysicsNeutronAtomic physicsNuclear ExperimentNucleonNuclear ExperimentCrystal BallThe European Physical Journal A
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Beam-Helicity Asymmetries in Double-Charged-Pion Photoproduction on the Proton

2005

Beam-helicity asymmetries for the two-pion-photoproduction reaction gamma + p --> p pi+ pi- have been studied for the first time in the resonance region for center-of-mass energies between 1.35 GeV and 2.30 GeV. The experiment was performed at Jefferson Lab with the CEBAF Large Acceptance Spectrometer using circularly polarized tagged photons incident on an unpolarized hydrogen target. Beam-helicity-dependent angular distributions of the final-state particles were measured. The large cross-section asymmetries exhibit strong sensitivity to the kinematics and dynamics of the reaction. The data are compared with the results of various phenomenological model calculations, and show that these…

Particle physicsPhotonProtonGeneral Physics and AstronomyFOS: Physical sciences13.60.-r 13.60.Le 13.88.+e[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Pion0103 physical sciencesPhenomenological model[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysics010308 nuclear & particles physicsBremsstrahlungHelicity3. Good healthPair productionNucleon
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Effect of quantized conductivity on the anomalous photon emission radiated from atomic-size point contacts

2019

We observe anomalous visible to near-infrared electromagnetic radiation emitted from electrically driven atomic-size point contacts. We show that the number of photons released strongly depends on the quantized conductance steps of the contact. Counter-intuitively, the light intensity features an exponential decay dependence with the injected electrical power. We propose an analytical model for the light emission considering an out-of-equilibrium electron distribution. We treat photon emission as bremsstrahlung process resulting from hot electrons colliding with the metal boundary and a find qualitative accord with the experimental data.

PhotonQC1-999FOS: Physical sciences02 engineering and technologybremsstrahlung01 natural sciences7. Clean energyElectromagnetic radiationelectromigrationMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciences[PHYS.COND]Physics [physics]/Condensed Matter [cond-mat]Electrical and Electronic EngineeringExponential decay010306 general physicsPhysicsCondensed Matter - Mesoscale and Nanoscale Physicsquantized conductivityPhysicsBremsstrahlungConductancevisible light emission021001 nanoscience & nanotechnologyAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsLight intensityAtomic radiuspoint contactLight emissionAtomic physics0210 nano-technologyOptics (physics.optics)BiotechnologyPhysics - Optics
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Photonuclear reactions with zinc: A case for clinical linacs

2015

WOS: 000365732300003

Physics - Instrumentation and DetectorsPhotonRAYGeneral Physics and AstronomyFOS: Physical sciencesNUCLEAR01 natural sciences7. Clean energyLinear particle acceleratorS-DALINACNuclear physicsNucleosynthesis0103 physical sciencesSCATTERINGFACILITYNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentGA-67PhysicsNUCLEOSYNTHESIS010308 nuclear & particles physicsScatteringBremsstrahlungInstrumentation and Detectors (physics.ins-det)[0-Belirlenecek]3. Good healthPhysics::Accelerator PhysicsHpge detectorDECAYBremsstrahlung photonBeam (structure)
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X-ray emitting hot plasma in solar active regions observed by the SphinX spectrometer

2012

Aims. The detection of very hot plasma in the quiescent corona is important for diagnosing heating mechanisms. The presence and the amount of such hot plasma is currently debated. The SphinX instrument on-board the CORONAS-PHOTON mission is sensitive to X-ray emission of energies well above 1 keV and provides the opportunity to detect the hot plasma component. Methods. We analysed the X-ray spectra of the solar corona collected by the SphinX spectrometer in May 2009 (when two active regions were present). We modelled the spectrum extracted from the whole Sun over a time window of 17 days in the 1.34− 7k eV energy band by adopting the latest release of the APED database. Results. The SphinX …

Physics010504 meteorology & atmospheric sciencesSpectrometerX-rayBremsstrahlungAstronomy and AstrophysicsPlasmaAstrophysics01 natural sciencesCoronaSpectral lineSun: corona methods: observational techniques: spectroscopicStars13. Climate actionSpace and Planetary Science0103 physical sciencesCalibration010303 astronomy & astrophysics0105 earth and related environmental sciencesAstronomy & Astrophysics
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A model of M87 nuclear emission without ADAF

2007

We present a simple physical model of the central source emission in the M87 galaxy. It is well known that the observed X‐ray luminosity from this galactic nucleus is much lower than the predicted one, if a standard radiative efficiency is assumed. Up to now the main model invoked to explain such a luminosity is the ADAF (Advection‐Dominated‐Accretion‐Flow) model. Our approach supposes only a simple axis‐symmetric adiabatic accretion with a low angular momentum together with the bremsstrahlung emission process in the accreting gas. With no other special hypothesis on the dynamics of the system, this model agrees well enough with the luminosity value measured by Chandra.

PhysicsAngular momentumActive galactic nucleusAstrophysics::High Energy Astrophysical PhenomenaBremsstrahlungAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsGalactic nucleiGalaxyAccretion (astrophysics)Radiative efficiencyAstrophysics::Solar and Stellar AstrophysicsAdiabatic processAstrophysics::Galaxy Astrophysics
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A Simple Model of Radiative Emission in M87

2005

We present a simple physical model of the central source emission in the M87 galaxy. It is well known that the observed X-ray luminosity from this galactic nucleus is much lower than the predicted one, if a standard radiative efficiency is assumed. Up to now the main model invoked to explain such a luminosity is the ADAF (Advection-Dominated-Accretion-Flow) model. Our approach supposes only a simple axis-symmetric adiabatic accretion with a low angular momentum together with the bremsstrahlung emission process in the accreting gas. With no other special hypothesis on the dynamics of the system, this model agrees well enough with the luminosity value measured by Chandra.

PhysicsAngular momentumAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)BremsstrahlungFOS: Physical sciencesAstronomy and AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsAstrophysicsaccretion accretion disks black hole physics hydrodynamicsGalaxyAccretion (astrophysics)Space and Planetary ScienceRadiative efficiencyRadiative transferAstrophysics::Solar and Stellar AstrophysicsAdiabatic processAstrophysics::Galaxy AstrophysicsThe Astrophysical Journal
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Atomic physics of positronium with intense slow positron beams

2002

Abstract The theory of quantum electrodynamics has presented a complete calculation of the energy levels of positronium (Ps, e + e − ) up to the order R ∞ α 4 . The annihilation rates for para -Ps (1 1 S 0 ) and ortho -Ps (1 1 S 1 ) are completely known up to the order R ∞ α 5 and R ∞ α 6 , respectively. The present experimental uncertainty for spectroscopic results is 5–100 times larger than the theoretical uncertainty. For the annihilation rates the experimental situation is even worse. The theoretical predictions have presently reached a level of precision which is a challenge to experimentalists! The experimental uncertainty for the fine- and hyperfine transitions in the Ps atom is dete…

PhysicsAnnihilationBremsstrahlungGeneral Physics and AstronomySurfaces and InterfacesGeneral ChemistryElectronCondensed Matter PhysicsSurfaces Coatings and Filmslaw.inventionPositroniumNuclear physicsPositronlawAtomBeam dumpAtomic physicsHyperfine structureApplied Surface Science
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The 0.1-100 keV Spectrum of LMC X-4 in the High State: Evidence for a High Energy Cyclotron Absorption Line

2001

We report on the spectral analysis of the X-ray pulsar LMC X-4 in its high state out of eclipse observed by BeppoSAX. During this observation no coherent pulsations are detected. The primary continuum is well described by a power law with a high energy cutoff (E_cutoff ~ E_fold ~ 18 keV). The addition of a cyclotron absorption line at ~100 keV improves the fit significantly. The inferred magnetic moment is 1.1 10^{31} Gauss cm^3, in agreement with the value estimated assuming that the neutron star is at the spin equilibrium, as it has been proposed for this source. The remaining excess at low energies can be fitted by a Comptonization of soft photons by moderately hot electrons (kT ~0.9 keV…

PhysicsAstrophysics::High Energy Astrophysical PhenomenaContinuum (design consultancy)Astrophysics (astro-ph)BremsstrahlungFOS: Physical sciencesAstronomy and AstrophysicsRadiusAstrophysicsAstrophysicsSpectral lineNeutron starPulsarSpace and Planetary ScienceOptical depth (astrophysics)Astrophysics::Solar and Stellar AstrophysicsBlack-body radiationAstrophysics::Earth and Planetary Astrophysics
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