Search results for "Dispersion"

showing 10 items of 1101 documents

ODS ferritic steels obtained from gas atomized powders through the STARS processing route: Reactive synthesis as an alternative to mechanical alloying

2018

Authors acknowledge ALBA synchrotron (Spain) for the provision of beamtime on the beam line BL22-CLAESS (Proposal 2016081797). Transmission electron microscopy observations were accomplished at Centro Nacional de Microscopía Electrónica, CNME-UCM. This work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training programme 2014–2018 under grant agreement No 633053. The views and opinions expressed herein do not necessarily reflect those of the European Commission. Financial support from Basque Government through the ELKARTEK ACTIMAT 2016 project is also acknowledged.

Nuclear and High Energy PhysicsMaterials scienceScanning electron microscopeMaterials Science (miscellaneous)Oxidechemistry.chemical_element02 engineering and technology01 natural sciences010305 fluids & plasmasNanoclusterschemistry.chemical_compoundRadiation damageFracture toughnessX-ray photoelectron spectroscopy0103 physical sciences:NATURAL SCIENCES:Physics [Research Subject Categories]Yttria-stabilized zirconiaEngineering & allied operationsMetallurgyYttrium021001 nanoscience & nanotechnologyMicrostructurelcsh:TK9001-9401Fusion reactorsNuclear Energy and Engineeringchemistrylcsh:Nuclear engineering. Atomic powerOxide dispersion strengthened ferritic stainless steels (ODS FS)ddc:6200210 nano-technology
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Investigation of precipitate in an austenitic ODS steel containing a carbon-rich process control agent

2018

This work has been carried out within the framework of the German Helmholtz Association and has received funding from the topic “Materials Research for the Future Energy Supply”. The work of M. Parish and Rainer Ziegler is gratefully acknowledged. Thanks are also due to the team of the chemical laboratory at the KIT for performing the chemical analysis. The help of the beamline staff at ELETTRA (project 20140052 ) synchrotron radiation facility is acknowledged. We acknowledge support by Deutsche Forschungsgemeinschaft and Open Access Publishing Fund of Karlsruhe Institute of Technology.

Nuclear and High Energy PhysicsMaterials scienceYield (engineering)Materials Science (miscellaneous)Oxidechemistry.chemical_elementProcess control agent02 engineering and technology01 natural sciences010305 fluids & plasmasCarbidechemistry.chemical_compound0103 physical sciences:NATURAL SCIENCES:Physics [Research Subject Categories]Process controlAusteniteMetallurgytechnology industry and agricultureX-ray absorption spectroscopy021001 nanoscience & nanotechnologylcsh:TK9001-9401Oxide dispersion strengthened steelNuclear Energy and Engineeringchemistry8. Economic growthlcsh:Nuclear engineering. Atomic powerAustenitic steelMechanical alloying0210 nano-technologyDispersion (chemistry)CarbonTransmission electron microscopyTitaniumNuclear Materials and Energy
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Pion and kaon vector form factors

2001

We develop a unitarity approach to consider the final state interaction corrections to the tree level graphs calculated from Chiral Perturbation Theory ($\chi PT$) allowing the inclusion of explicit resonance fields. The method is discussed considering the coupled channel pion and kaon vector form factors. These form factors are then matched with the one loop $\chi PT$ results. A very good description of experimental data is accomplished for the vector form factors and for the $\pi\pi$ P-wave phase shifts up to $\sqrt{s}\lesssim 1.2$ GeV, beyond which multiparticle states play a non negligible role. In particular the low and resonance energy regions are discussed in detail and for the forme…

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryPartial wave analysisFOS: Physical sciencesPerturbation (astronomy)chiral [perturbation theory]CoincidenceHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Pioninterpretation of experiments [numerical calculations]Dispersion relationtree approximationunitarityddc:530higher-order [Feynman graph]form factor [K]PhysicsUnitarityFísicapartial wave analysisHigh Energy Physics - Phenomenologyform factor [pi]vector [form factor]Quantum electrodynamicsIsospinelastic scattering [pi pi]correction [final-state interaction]
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On the pion cloud of the nucleon

2003

We evaluate the two--pion contribution to the nucleon electromagnetic form factors by use of dispersion analysis and chiral perturbation theory. After subtraction of the rho--meson component, we calculate the distributions of charge and magnetization in coordinate space, which can be interpreted as the effects of the pion cloud. We find that the charge distribution of this pion cloud effect peaks at distances of about 0.3 fm. Furthermore, we calculate the contribution of the pion cloud to the isovector charges and radii of the nucleon.

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear Theorydispersion relationHigh Energy Physics::LatticeisovectorNuclear Theorychiral [perturbation theory]FOS: Physical sciencestwo-pion [effect]form factor [nucleon]density [charge]Nuclear physicsNuclear Theory (nucl-th)PionHigh Energy Physics - Phenomenology (hep-ph)ddc:530Perturbation theoryCoordinate spacenumerical calculationsNuclear ExperimentPhysicsIsovectorpole [rho(770)]Charge densityCharge (physics)High Energy Physics - Phenomenologycloud [pi]High Energy Physics::Experimentspectral representationNucleon
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A dispersive estimate of scalar contributions to hadronic light-by-light scattering

2021

We consider the contribution of scalar resonances to hadronic light-by-light scattering in the anomalous magnetic moment of the muon. While the $f_0(500)$ has already been addressed in previous work using dispersion relations, heavier scalar resonances have only been estimated in hadronic models so far. Here, we compare an implementation of the $f_0(980)$ resonance in terms of the coupled-channel $S$-waves for $\gamma^*\gamma^*\to \pi\pi/\bar K K$ to a narrow-width approximation, which indicates $a_\mu^{\text{HLbL}}[f_0(980)]=-0.2(2)\times 10^{-11}$. With a similar estimate for the $a_0(980)$, the combined effect is thus well below $1\times 10^{-11}$ in absolute value. We also estimate the …

Nuclear and High Energy PhysicsParticle physicsNuclear Theory530 PhysicsQC1-999Scalar (mathematics)HadronFOS: Physical sciencesAbsolute value01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Dispersion relation0103 physical sciences010306 general physicsPhysicsMuonAnomalous magnetic dipole moment010308 nuclear & particles physicsScatteringPhysicsHigh Energy Physics - Lattice (hep-lat)ResonanceHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentPhysics Letters B
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Compton Scattering by the Proton using a Large-Acceptance Arrangement

2001

Compton scattering by the proton has been measured over a wide range covering photon energies 250 MeV lt or approximately=E/sub gamma / lt or approximately=800 MeV and photon scattering angles 30 degrees lt or approximately= theta /sub gamma //sup lab/ lt or approximately=150 degrees , using the tagged-photon facility at MAMI (Mainz) and the large-acceptance arrangement LARA. The previously existing data base on proton Compton scattering is greatly enlarged by more than 700 new data points. The new data are interpreted in terms of dispersion theory based on the SAID-SM99K parametrization of photo-meson amplitudes. It is found that two-pion exchange in the t-channel is needed for a descripti…

Nuclear and High Energy PhysicsProtonNuclear TheoryFOS: Physical sciencesValue (computer science)01 natural sciencesResonance (particle physics)High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Dispersion relation0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentQCSpin-½Physics010308 nuclear & particles physicsCompton scatteringHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics::ExperimentMultipole expansion
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Heuristic Algorithm for the Analysis of Fast Field Cycling (FFC) NMR Dispersion Curves

2021

Evaluation of nuclear magnetic relaxation dispersion (NMRD) curves obtained by the fast field cycling nuclear magnetic resonance (FFC-NMR) relaxometry technique is a valuable tool for analyzing the microscopic dynamics of condensed matter systems. However, quantitative data analysis involves several conceptual and practical issues. Moving forward from previous literature approaches, we propose a new analysis method, relying on the elaboration of the inverse integral transform of the NMRD curve. Our approach results in a true heuristic method, able to unambiguously individuate the dynamic domains in the system, thereby avoiding the possible introduction of any element of discretion. The anal…

Nuclear magnetic relaxationNanospongesRelaxometryMagnetic Resonance SpectroscopyField cyclingHeuristic (computer science)Settore AGR/13 - Chimica AgrariaInverseHeuristic algorithm010402 general chemistry01 natural sciencesAnalytical ChemistryFFC NMRCheeseDispersion (optics)HeuristicsAnalysis methodSettore CHIM/02 - Chimica FisicaCyclodextrinsChemistry010401 analytical chemistrySettore CHIM/06 - Chimica OrganicaIntegral transformMagnetic Resonance Imaging0104 chemical sciencesRelaxometryAlgorithmAlgorithmsAnalytical Chemistry
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Dispersive approach to the nuclear compton amplitude and exchange effects

1981

We discuss the limitation of the standard approach to exchange current effects from photonuclear sum rules. We propose to look for an energy-independent contribution to the real part of the forward Compton-scattering amplitude below pion threshold. Experimental data on photonuclear cross-sections are used to calculate the real part of the amplitude, by means of an once-subtracted dispersion relation. The analysis is made for2H,7Li and9Be at energies varying between 50 and 150 MeV. A remarkably stable value ofK=0.60 is extracted for deuterium. For 1p shell nuclei, the main uncertainty is due to the lack of data above 300 MeV.

Nuclear physicsPhysicsAmplitudePionDeuteriumDispersion relationNuclear TheoryShell (structure)Current (fluid)Nuclear ExperimentIl Nuovo Cimento A
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The energy loss system of the electron scattering facility at the Mainz 300 MeV linear accelerator

1978

Abstract An energy loss system was constructed for the electron scattering facility at the Mainz 300 MeV linear accelerator with the aim of improving the energy resolution and increasing the useful beam current. The main features of the design are: (1) the existing system (conventional mode) is kept in full operation, (2) for the energy loss mode, the electron beam is deflected vertically downwards and then returned to the original beam line by the dispersion matching system, consisting of three dipole magnets and one quadrupole magnet, (3) the dispersion of the beam on the target can be tuned to the dispersion of the spectrometer with the aid of the quadrupole magnet. With the installation…

Nuclear physicsPhysicsDipoleBeamlineSpectrometerMagnetDispersion (optics)Physics::Accelerator PhysicsGeneral MedicineQuadrupole magnetElectron scatteringBeam (structure)Nuclear Instruments and Methods
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HADRONIC CROSS SECTION MEASUREMENT AT BES-III

2014

Measurements of the R ratio are closely related to two pre quantities, the anomalous magnetic moment of the muon (g - 2), and the value of the electromagnetic fine structure constant [Formula: see text]. Hadronic contributions to both quantities can be derived via dispersion integrals, using experimental R data as input. For the phenomenological evaluations of these contributions, different energy ranges of hadronic cross section data are required. At BES-III, Initial State Radiation (ISR) from an existing Ψ(3770) dataset will be used for measurements of hadronic cross sections below [Formula: see text], while for higher energies a dedicated energy scan program will be performed up to [For…

Nuclear physicsPhysicsParticle physicsCross section (physics)MuonAnomalous magnetic dipole momentHadronDispersion (optics)High Energy Physics::ExperimentFine-structure constantRadiationEnergy (signal processing)International Journal of Modern Physics: Conference Series
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