Search results for "Berg"

showing 10 items of 758 documents

Collinear two-photon excitation of indium rydberg states in a fast atomic beam

1986

The 29p-Rydberg state of neutral indium was produced by double resonant two-photon excitation in a fast atomic beam and detected via field ionization in a longitudinal electric field.

PhysicsAtomic beamPhysics::Instrumentation and Detectorschemistry.chemical_elementAtomic and Molecular Physics and Opticssymbols.namesakechemistryTwo-photon excitation microscopyElectric fieldField desorptionPhysics::Atomic and Molecular ClustersRydberg formulasymbolsPhysics::Accelerator PhysicsPhysics::Atomic PhysicsAtomic physicsExcitationIndiumZeitschrift f�r Physik D Atoms, Molecules and Clusters
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Characterization of a Be(p,xn) Neutron Source for Fission Yields Measurements

2013

We report on measurements performed at The Svedberg Laboratory (TSL) to characterize a proton-neutron converter for independent fission yield studies at the IGISOL-JYFLTRAP facility (Jyv\"askyl\"a, Finland). A 30 MeV proton beam impinged on a 5 mm water-cooled Beryllium target. Two independent experimental techniques have been used to measure the neutron spectrum: a Time of Flight (TOF) system used to estimate the high-energy contribution, and a Bonner Sphere Spectrometer able to provide precise results from thermal energies up to 20 MeV. An overlap between the energy regions covered by the two systems will permit a cross-check of the results from the different techniques. In this paper, th…

PhysicsBonner sphereNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsSpectrometerta114010308 nuclear & particles physicsFissionNuclear TheoryNuclear dataFOS: Physical sciencesFission product yieldInstrumentation and Detectors (physics.ins-det)7. Clean energy01 natural sciencesThe Svedberg LaboratoryNuclear physics0103 physical sciencesNeutron sourceNeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentNuclear Data Sheets
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Collisional and thermal ionization of sodium Rydberg atoms I. Experiment for nS and nD atoms with n=8-20

2005

Collisional and thermal ionization of sodium nS and nD Rydberg atoms with n=8-20 has been studied. The experiments were performed using a two-step pulsed laser excitation in an effusive atomic beam at atom density of about 2 10^{10} cm^{-3}. Molecular and atomic ions from associative, Penning, and thermal ionization processes were detected. It has been found that the atomic ions were created mainly due to photoionization of Rydberg atoms by photons of blackbody radiation at the ambient temperature of 300K. Blackbody ionization rates and effective lifetimes of Rydberg states of interest were determined. The molecular ions were found to be from associative ionization in Na(nL)+Na(3S) collisio…

PhysicsChemical Physics (physics.chem-ph)Atomic Physics (physics.atom-ph)Thermal ionizationFOS: Physical sciencesPhotoionizationCondensed Matter PhysicsAtomic and Molecular Physics and OpticsIonPhysics - Atomic Physicssymbols.namesakeIonizationPhysics - Chemical PhysicsRydberg atomAtomRydberg formulasymbolsPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsAtomic physicsExcitation
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Dynamics of Confined Crowd Modelled Using Fermionic Operators

2014

An operatorial method based on fermionic operators is used to describe the dynamics of a crowd made of different kind of populations mutually interacting and moving in a two–dimensional bounded closed region. The densities of the populations are recovered through the Heisenberg equation and the diffusion process is driven by the Hamiltonian operator defined by requiring that the populations move along optimal paths. We apply the model obtained in a concrete situation and we discuss the effect of the interaction between the populations during their motion.

PhysicsClassical mechanicsPhysics and Astronomy (miscellaneous)Diffusion processGeneral MathematicsQuantum dynamicsBounded functionQuantum mechanicsDynamics (mechanics)Motion (geometry)Settore MAT/07 - Fisica MatematicaHeisenberg pictureFermionic operatorsQuantum dynamics Heisenberg-like dynamics Dynamics of competing populations
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Quantum rings for beginners: Energy spectra and persistent currents

2003

Theoretical approaches to one-dimensional and quasi-one-dimensional quantum rings with a few electrons are reviewed. Discrete Hubbard-type models and continuum models are shown to give similar results governed by the special features of the one-dimensionality. The energy spectrum of the many-body states can be described by a rotation-vibration spectrum of a 'Wigner molecule' of 'localized' electrons, combined with the spin-state determined from an effective antiferromagnetic Heisenberg Hamiltonian. The persistent current as a function of the magnetic flux through the ring shows periodic oscillations arising from the 'rigid rotation' of the electron ring. For polarized electrons the periodic…

PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)Heisenberg modelFOS: Physical sciencesPersistent currentElectronic structureElectronCondensed Matter PhysicsAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsCondensed Matter - Strongly Correlated Electronssymbols.namesakeLuttinger liquidQuantum mechanicsMagnetic flux quantumMesoscale and Nanoscale Physics (cond-mat.mes-hall)symbolsHamiltonian (quantum mechanics)Quantum
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Determination of the154Sm ionization energy by high-precision laser spectroscopy

2004

High-resolution resonance ionization mass spectrometry has been used to determine the ionization energy of 154Sm. Three-step resonant excitation with single-frequency lasers populates a series of ? = 3, J = 4 Rydberg levels in the range of n = 60?160, covering the range of 30 cm?1 to 4 cm?1 below the first ionization limit. Although samarium has a complex electronic structure with eight valence electrons, series of nearly unperturbed levels could be observed. Analysis includes shifts caused by a single perturbing state, an extended Ritz term for quantum defect variation at lower n, and corrections for residual electric fields. The resulting series convergence limit has an uncertainty of 4 ?…

PhysicsCondensed Matter PhysicsMass spectrometryAtomic and Molecular Physics and OpticsQuantum defectsymbols.namesakeOrders of magnitude (time)Excited stateIonizationRydberg formulasymbolsAtomic physicsIonization energyGround stateJournal of Physics B: Atomic, Molecular and Optical Physics
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Beyond the Heisenberg Model: Anisotropic Exchange Interaction between a Cu-Tetraazaporphyrin Monolayer andFe3O4(100)

2013

The exchange coupling of a single spin localized at the central ion of Cu-tetraazaporphyrin on a magnetite(100) surface has been studied using x-ray magnetic circular dichroism (XMCD). Sum rule analysis of the XMCD spectra results in Cu spin and orbital magnetic moments as a function of the applied external field at low temperatures (20 K). The exchange coupling is positive for magnetization direction perpendicular to the surface (ferromagnetic) while it is negative for in-plane magnetization direction (antiferromagnetic). We attribute the anisotropy of the Heisenberg exchange coupling to an orbitally dependent exchange Hamiltonian.

PhysicsCondensed Matter::Materials ScienceMagnetizationMagnetic momentCondensed matter physicsFerromagnetismMagnetic circular dichroismHeisenberg modelExchange interactionGeneral Physics and AstronomyAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsSum rule in quantum mechanicsPhysical Review Letters
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Controlled long-range interactions between Rydberg atoms and ions

2016

We theoretically investigate trapped ions interacting with atoms that are coupled to Rydberg states. The strong polarizabilities of the Rydberg levels increases the interaction strength between atoms and ions by many orders of magnitude, as compared to the case of ground state atoms, and may be mediated over micrometers. We calculate that such interactions can be used to generate entanglement between an atom and the motion or internal state of an ion. Furthermore, the ion could be used as a bus for mediating spin-spin interactions between atomic spins in analogy to much employed techniques in ion trap quantum simulation. The proposed scheme comes with attractive features as it maps the bene…

PhysicsCondensed Matter::Quantum GasesQuantum PhysicsAtomic Physics (physics.atom-ph)Quantum simulatorFOS: Physical sciencesQuantum entanglement7. Clean energy01 natural sciences3. Good health010305 fluids & plasmasPhysics - Atomic Physicssymbols.namesake0103 physical sciencesAtomRydberg atomQuantum systemRydberg formulasymbolsPhysics::Atomic PhysicsQuantum informationAtomic physics010306 general physicsQuantum Physics (quant-ph)Trapped ion quantum computerPhysical Review A
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Spin Dynamics of the Half-Integer-Spin Quasi-One-Dimensional Heisenberg Antiferromagnet CsMnI3

1994

Magnetic excitations of CsMnI 3 , a quasi-one-dimensional Heisenberg antiferromagnet with S =5/2, have been measured by means of inelastic neutron scattering. Magnetic excitations in the low temperature phase are in good agreement with the predictions of the conventional linear spin-wave theory. In particular, in accordance with the linear spin-wave theory, we found three separate modes at Q =(0, 0, 1) instead of a threefold degenerate mode as seen in CsNiCl 3 ( S =1). It confirms that the spin dynamics of the integer spin value system are very different from those of the half-integer spin value system, even in their three-dimensionally ordered phase. Magnetic excitations in the intermediat…

PhysicsCondensed matter physicsSpin waveHeisenberg modelGeneral Physics and AstronomyAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsHalf-integerInelastic scatteringNeutron scatteringInelastic neutron scatteringSpin-½Journal of the Physical Society of Japan
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Measurement of electroweak parameters from Z decays into fermion pairs

1990

We report on the properties of theZ resonance from 62 500Z decays into fermion pairs collected with the ALEPH detector at LEP, the Large Electron-Positron storage ring at CERN. We findMZ=(91.193±0.016exp±0.030LEP) GeV, ΓZ=(2497±31) MeV, σhad0=(41.86±0.66)nb, and for the partial widths Γinv=(489±24) MeV, Γhad(1754±27) MeV, Γee=(85.0±1.6)MeV, Γμμ=(80.0±2.5) MeV, and Γττ=(81.3±2.5) MeV, all in good agreement with the Standard Model. Assuming lepton universality and using a lepton sample without distinction of the final state we measure Γu=(84.3±1.3) MeV. The forward-backward asymmetry in leptonic decays is used to determine the vector and axial-vector weak coupling constants of leptors,gv2(MZ2…

PhysicsCoupling constantParticle physicsPhysics and Astronomy (miscellaneous)media_common.quotation_subjectElectron–positron annihilationElectroweak interactionWeinberg angleFermionAsymmetryNuclear physicsHigh Energy Physics::ExperimentNeutrinoNuclear ExperimentEngineering (miscellaneous)Particle Physics - ExperimentLeptonmedia_common
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