Search results for "ddc:"

showing 10 items of 3080 documents

βdecay of102Y produced in projectile fission of238U

2012

The population of 102Zr following the β decay of 102Y produced in the projectile fission of 238U at the GSI facility in Darmstadt, Germany has been studied. 102Y is known to ß decay into 102Zr via two states, one of high spin and the other low spin. These states preferentially populate different levels in the 102Zr daughter. In this paper the intensities of transitions in 102Zr observed are compared with those from the decay of the low-spin level studied at the TRISTAN facility at Brookhaven National Laboratory and of the high-spin level studied at the JOSEF separator at the Kernforschungsanlage Jülich.

PhysicsHistoryeducation.field_of_studyCluster decayFissionProjectilePopulationBeta decayddc:Computer Science ApplicationsEducationNuclear physicsSubatomic PhysicsHigh Energy Physics::ExperimentAtomic physicsNuclear ExperimentSpin (physics)National laboratoryeducationJournal of Physics: Conference Series
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Green functions for nearest- and next-nearest-neighbor hopping on the Bethe lattice

2005

We calculate the local Green function for a quantum-mechanical particle with hopping between nearest and next-nearest neighbors on the Bethe lattice, where the on-site energies may alternate on sublattices. For infinite connectivity the renormalized perturbation expansion is carried out by counting all non-self-intersecting paths, leading to an implicit equation for the local Green function. By integrating out branches of the Bethe lattice the same equation is obtained from a path integral approach for the partition function. This also provides the local Green function for finite connectivity. Finally, a recently developed topological approach is extended to derive an operator identity whic…

PhysicsImplicit functionBethe latticeStrongly Correlated Electrons (cond-mat.str-el)Operator (physics)Spectrum (functional analysis)General Physics and AstronomyFOS: Physical sciencesPartition function (mathematics)01 natural sciences010305 fluids & plasmask-nearest neighbors algorithmCondensed Matter - Strongly Correlated Electrons0103 physical sciencesPath integral formulationGravitational singularityddc:530Condensed Matter::Strongly Correlated ElectronsStatistical physics010306 general physics
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Super-Planckian axions from near-conformality

2019

We present a novel framework for obtaining large hierarchies in axion decay constants as well as trans-Planckian field excursions, with no need for tuning or a large number of fields. We consider a model with two or more conformal field theories with a common cutoff, which are linked by a gauged diagonal symmetry. This construction is dual to the geometry of a warped space with two or more throats glued at a common brane. Besides allowing for calculability, the dual picture makes it possible to interpret the hierarchy of decay constants entirely in terms of the geometry. Our setup can be applied to any framework which requires large field excursions or multiple hierarchies of decay constant…

PhysicsInflation (cosmology)Field (physics)010308 nuclear & particles physicsDiagonalConformal mapSpace (mathematics)01 natural sciencesSymmetry (physics)High Energy Physics::TheoryTheoretical physics0103 physical sciencesddc:530Brane010306 general physicsAxionPhysical Review D
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Oscillations of ECR ion source beam current along the beam transport of the JYFL K-130 cyclotron

2013

A versatile measurement system has been developed to study the temporal characteristics of ion beams in millisecond time scale. The system is composed of data acquisition hardware and LabVIEW based measurement and analysis program. The measurement system and ion beam current oscillation results measured with a 14 GHz AECR-U type ion source at University of Jyv"askyl"a, Department of Physics (JYFL), are presented. It is shown that the ion beams exhibit periodic current fluctuations at frequencies from 100 Hz to 1.5 kHz with amplitudes ranging from 1 to 65 percent of the average beam current. It is argued that these oscillations originate from the ion source plasma since their characteristics…

PhysicsIon beamCyclotronIon gun01 natural sciencesIon sourceFourier transform ion cyclotron resonance010305 fluids & plasmaslaw.inventionBeamlinePhysics::Plasma Physicslaw0103 physical sciencesPhysics::Accelerator Physicsddc:610Atomic physics010306 general physicsInstrumentationMathematical PhysicsIon cyclotron resonanceBeam (structure)Journal of Instrumentation
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Spectroscopic Tools Applied to Element Z = 115 Decay Chains

2014

Nuclides that are considered to be isotopes of element Z = 115 were produced in the reaction 48Ca + 243Am at the GSI Helmholtzzentrum für Schwerionenforschung Darmstadt. The detector setup TASISpec was used. It was mounted behind the gas-filled separator TASCA. Thirty correlated α-decay chains were found, and the energies of the particles were determined with high precision. Two important spectroscopic aspects of the offline data analysis are discussed in detail: the handling of digitized preamplified signals from the silicon strip detectors, and the energy reconstruction of particles escaping to upstream detectors relying on pixel-by-pixel dead-layer thicknesses.

PhysicsIsotopeSiliconPhysics::Instrumentation and DetectorsPhysicsQC1-999DetectorSeparator (oil production)Mechanical engineeringchemistry.chemical_element7. Clean energyNuclear physicschemistryPhysical SciencesSubatomic Physicsddc:530Decay chainNuclideNuclear ExperimentLine (formation)EPJ Web of Conferences
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Transition from plasma-driven to Kerr-driven laser filamentation.

2011

While filaments are generally interpreted as a dynamic balance between Kerr focusing and plasma defocusing, the role of the higher-order Kerr effect (HOKE) is actively debated as a potentially dominant defocusing contribution to filament stabilization. In a pump-probe experiment supported by numerical simulations, we demonstrate the transition between two distinct filamentation regimes at 800 nm. For long pulses (1.2 ps), the plasma substantially contributes to filamentation, while this contribution vanishes for short pulses (70 fs). These results confirm the occurrence, in adequate conditions, of filamentation driven by the HOKE rather than by plasma.

PhysicsKerr effectgenetic structuresbusiness.industryGeneral Physics and AstronomyPhysics::OpticsSelf-focusingddc:500.2Plasmamacromolecular substancesLaser01 natural scienceslaw.invention010309 opticsProtein filamentQuantitative Biology::Subcellular ProcessesOpticsFilamentationlaw0103 physical sciencesAtomic physics010306 general physicsbusinessSelf-phase modulationPhysical review letters
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Exploiting transport properties for the detection of optical pumping in heavy ions

2020

We present a kinetic model for optical pumping in Lu$^+$ and Lr$^+$ ions as well as a theoretical approach to calculate the transport properties of Lu$^+$ in its ground $^1S_0$ and metastable $^3D_1$ states in helium background gas. Calculations of the initial ion state populations, the field and temperature dependence of the mobilities and diffusion coefficients, and the ion arrival time distributions demonstrate that the ground- and metastable-state ions can be collected and discriminated efficiently under realistic macroscopic conditions.

PhysicsKinetic modelAtomic Physics (physics.atom-ph)FOS: Physical scienceschemistry.chemical_elementSuperheavy Elements01 natural sciencesLutetiumPhysics - Atomic Physics010305 fluids & plasmasIonOptical pumpingchemistry0103 physical sciencesddc:530Atomic physics010306 general physicsLawrenciumPhysical Review A
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Search for polarization effects in the antiproton production process

2015

For the production of a polarized antiproton beam various methods have been suggested including the possibility that antiprotons may be produced polarized which will be checked experimentally. The polarization of antiprotons produced under typical conditions for antiproton beam preparation will be measured at the CERN/PS. If the production process creates some polarization a polarized antiproton beam could be prepared by a rather simple modification of the antiproton beam facility. The detection setup and the expected experimental conditions are described. For the production of a polarized antiproton beam various methods have been suggested including the possibility that antiprotons may be …

PhysicsLarge Hadron ColliderPhysics - Instrumentation and DetectorsFOS: Physical sciencesGeneral Physics and AstronomyParticle acceleratorInstrumentation and Detectors (physics.ins-det)Polarization (waves)law.inventionHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Antiproton beamAntiprotonlawPhysics::Accelerator Physicsddc:530High Energy Physics::ExperimentPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)Detectors and Experimental TechniquesNuclear ExperimentNuclear Experiment
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Recent progress on the calculation of three-loop heavy flavor Wilson coefficients in deep-inelastic scattering

2014

We report on our latest results in the calculation of the three-loop heavy flavor contributions to the Wilson coefficients in deep-inelastic scattering in the asymptotic region $Q^2 \gg m^2$. We discuss the different methods used to compute the required operator matrix elements and the corresponding Feynman integrals. These methods very recently allowed us to obtain a series of new operator matrix elements and Wilson coefficients like the flavor non-singlet and pure singlet Wilson coefficients.

PhysicsLoop (topology)Particle physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesddc:530Deep inelastic scatteringFlavor
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Accurate calculation of the transverse anisotropy of a magnetic domain wall in perpendicularly magnetized multilayers

2015

Bloch domain walls are the most common type of transition between two out-of-plane magnetized domains (one magnetized upwards, one downwards) in films with perpendicular magnetic anisotropy. The rotation of the spins of such domain walls in the plane of the film requires energy, which is described by an effective anisotropy, the so-called transverse or hard axis anisotropy ${K}_{\ensuremath{\perp}}$. This anisotropy and the related D\"oring mass density of the domain wall are key parameters of the one-dimensional model to describe the motion of magnetic domain walls. In particular, the critical field strength or current density where oscillatory domain wall motion sets in (Walker breakdown)…

PhysicsMagnetic domainSpin polarizationCondensed matter physics02 engineering and technologyType (model theory)021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesElectronic Optical and Magnetic MaterialsMagnetic anisotropyDomain wall (magnetism)0103 physical sciencesddc:530010306 general physics0210 nano-technologyAnisotropyCritical fieldEnergy (signal processing)Physical Review B
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