Search results for "physics.atom-ph"

showing 10 items of 395 documents

The identification of autoionizing states of atomic chromium for the resonance ionization laser ion source of the ISOLDE radioactive ion beam facility

2017

Abstract This paper presents the results of an investigation into autoionizing states of atomic chromium, in the service of the resonance ionization laser ion source (RILIS): the principal ion source of the ISOLDE radioactive ion beam facility based at CERN. The multi-step resonance photo-ionization process enables element selective ionization which, in combination with mass separation, allows isotope specific selectivity in the production of radioactive ion beams at ISOLDE. The element selective nature of the process requires a multi-step “ionization scheme” to be developed for each element. Using the method of in-source resonance ionization spectroscopy, an optimal three-step, three-reson…

Ion beamChemistry010401 analytical chemistryResonanceMass spectrometryphysics.atom-ph01 natural sciencesIon sourceAtomic and Molecular Physics and Optics0104 chemical sciencesAtmospheric-pressure laser ionizationAnalytical ChemistryIon beam depositionIonization0103 physical sciencesPhysics::Atomic and Molecular ClustersPhysics::Accelerator PhysicsNuclear Physics - ExperimentPhysics::Atomic PhysicsAtomic physics010306 general physicsInstrumentationElectron ionizationSpectroscopySpectrochimica Acta Part B: Atomic Spectroscopy
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Measurement of high order Kerr refractive index of major air components

2009

International audience; We measure the instantaneous electronic nonlinear refractive index of N2 , O2 , and Ar at room temperature for a 90 fs and 800 nm laser pulse. Measurements are calibrated by post-pulse molecular alignment through a polarization technique. At low intensity, quadratic coefficients n2 are determined. At higher intensities, a strong negative contribution with a higher nonlinearity appears, which leads to an overall negative nonlinear Kerr refractive index in air above 26 TW/cm2 .

Kerr effectMaterials science[ PHYS.PHYS.PHYS-ATOM-PH ] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Physics::Optics01 natural sciences010309 opticsOpticsSelf-focusing0103 physical sciencesUltrafast nonlinear opticsZ-scan technique[PHYS.PHYS.PHYS-ATOM-PH] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]010306 general physicsSelf-phase modulationOptical Kerr effect[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Molecular alignment320.2250 350.5400 260.5950business.industryFemtosecond phenomenaCross-phase modulationAirSelf-focusingPolarization (waves)Atomic and Molecular Physics and OpticsRefractometryMagneto-optic Kerr effectPlasmasGasesbusinessRefractive indexAlgorithmsEnvironmental Monitoring
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Measurement of high order Kerr refractive index of major air components: erratum

2010

A clarification is missing concerning the high order Kerr non-linearities deduced from our experimental data published in [Opt. Express 17, 13429-13434 (2009)]. Here, we rectify this omission by making explicit the distinction between cross-Kerr and Kerr effects, and by extrapolating the value of the nonlinear refractive index for the last effect. Since the occurrence of sign inversion in the Kerr effect is not affected, the overall report in [Opt. Express 17, 13429-13434] remains valid.

Kerr effect[ PHYS.PHYS.PHYS-ATOM-PH ] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph](320.2250) Femtosecond phenomena; (350.5400) Plasmas; (190.7110) Ultrafast nonlinear optics; (260.5950) Self-focusing01 natural sciences010309 opticsOptics0103 physical sciencesZ-scan techniqueHigh order[PHYS.PHYS.PHYS-ATOM-PH] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]010306 general physicsfemtosecondLaser beamsplasmaPhysics[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Molecular alignmentbusiness.industrySelf-focusingNonlinear refractive indexPolarization (waves)Atomic and Molecular Physics and Opticslaser filamentationbusinessRefractive index) Ultrafast nonlinear optics
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General approach to spatiotemporal modulational instability processes

2011

International audience; In this article, we derive the general exact solution of the modulation instability gain. The solution described here is valid for 1-D, 2-D, and 3-D cases considering any temporal response function of the medium and with possible higher order Kerr nonlinearities. In particular, we show that the gain induced by modulation instability is initial condition dependent, while the usual calculations do not lead to such a dependence. Applications for current and high-interest nonlinear propagation problems, such as 1-D optical fiber propagation with delayed Raman response and 2-D filamentation in gases, are investigated in detail. More specifically, we demonstrate that the 2-D …

Kerr effect[ PHYS.PHYS.PHYS-ATOM-PH ] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Modulational instability01 natural sciencesInstabilityLaser filamentation010309 opticsFilamentationSelf-focusing0103 physical sciencesInitial value problemUltrafast nonlinear optics010306 general physicsOptical Kerr effect42.65.Ky 42.65.Sf 42.81.DpPhysicsMolecular alignment[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Femtosecond phenomenaSelf-focusingAtomic and Molecular Physics and OpticsNonlinear systemModulational instabilityClassical mechanicsModulationPlasmasQuantum electrodynamics
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Spectral dependence of purely-Kerr driven filamentation in air and argon

2010

5 pags, 4 figs.-- PACS number(s): 42.65.Jx, 42.65.Tg, 78.20.Ci. -- Publisher error corrected 27 September 2010, Erratum Phys. Rev. A 82, 039905 (2010): https://doi.org/10.1103/PhysRevA.82.033826

Kerr effect[ PHYS.PHYS.PHYS-ATOM-PH ] Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]chemistry.chemical_elementFOS: Physical sciencesPhysics::Opticsddc:500.201 natural sciencesLaser filamentationSpectral line010309 opticsFilamentationPhysics::Plasma PhysicsIonizationSelf-focusing0103 physical sciencesSelf focusing and defocusingOptical solitonsOptical constantsUltrafast nonlinear optics010306 general physicsSelf-phase modulationOptical Kerr effectPhysicsArgonMolecular alignment[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Femtosecond phenomena42.65.Jx 42.65.Tg 78.20.CiSelf-focusingSelf-phase modulationBeam trappingAtomic and Molecular Physics and OpticsWavelengthchemistryPlasmasAtomic physicsPhysics - OpticsOptics (physics.optics)
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Mobility of the Singly-Charged Lanthanide and Actinide Cations: Trends and Perspectives

2020

The current status of gaseous transport studies of the singly-charged lanthanide and actinide ions is reviewed in light of potential applications to superheavy ions. The measurements and calculations for the mobility of lanthanide ions in He and Ar agree well, and they are remarkably sensitive to the electronic configuration of the ion, namely, whether the outer electronic shells are 6s, 5d6s or 6s$^2$. The previous theoretical work is extended here to ions of the actinide family with zero electron orbital momentum: Ac$^+$ (7s$^2$, $^1$S), Am$^+$ (5f$^7$7s $^9$S$^\circ$), Cm$^+$ (5f$^7$7s$^2$ $^8$S$^\circ$), No$^+$ (5f$^{14}$7s $^2$S) and Lr$^+$ (5f$^{14}$7s$^2$ $^1$S). The calculations rev…

LanthanideAtomic Physics (physics.atom-ph)Ab initioFOS: Physical sciences02 engineering and technologyElectroninteraction potential010402 general chemistry7. Clean energy01 natural sciencesPhysics - Atomic PhysicsIonlcsh:Chemistryion mobilityAtomlanthanideselectronic configurationOriginal ResearchPhysicsIonic radiussuperheavy ionsactinidesGeneral ChemistryActinide021001 nanoscience & nanotechnology3. Good health0104 chemical sciencesChemistrylcsh:QD1-999ddc:540Electron configurationAtomic physics0210 nano-technology
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Measurement of the Permanent Electric Dipole Moment of the $^{129}$Xe Atom

2019

We report on a measurement of the $CP$-violating permanent electric dipole moment (EDM) of the neutral $^{129}\mathrm{Xe}$ atom. Our experimental approach is based on the detection of the free precession of co-located nuclear spin-polarized $^{3}\mathrm{He}$ and $^{129}\mathrm{Xe}$ samples. The EDM measurement sensitivity benefits strongly from long spin coherence times of several hours achieved in diluted gases and homogeneous weak magnetic fields of about 400 nT. A finite EDM is indicated by a change in the precession frequency, as an electric field is periodically reversed with respect to the magnetic guiding field. Our result $(\ensuremath{-}4.7\ifmmode\pm\else\textpm\fi{}6.4)\ifmmode\t…

Larmor precessionPhysicsField (physics)Atomic Physics (physics.atom-ph)FOS: Physical sciences01 natural sciences010305 fluids & plasmasMagnetic fieldPhysics - Atomic PhysicsElectric dipole momentElectric field0103 physical sciencesAtomddc:530Sensitivity (control systems)Atomic physics010306 general physicsSpin (physics)
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Suppression of nonlinear Zeeman effect and heading error in earth-field-range alkali-vapor magnetometers

2018

The nonlinear Zeeman effect can induce splitting and asymmetries of magnetic-resonance lines in the geophysical magnetic field range. This is a major source of "heading error" for scalar atomic magnetometers. We demonstrate a method to suppress the nonlinear Zeeman effect and heading error based on spin locking. In an all-optical synchronously pumped magnetometer with separate pump and probe beams, we apply a radio-frequency field which is in-phase with the precessing magnetization. In an earth-range field, a multi-component asymmetric magnetic-resonance line with ? 60 Hz width collapses into a single peak with a width of 22 Hz, whose position is largely independent of the orientation of th…

MagnetometerAtomic Physics (physics.atom-ph)General Physics and AstronomyFOS: Physical sciences02 engineering and technology01 natural scienceslaw.inventionPhysics - Atomic Physicssymbols.namesakeMagnetizationOpticslaw0103 physical sciences010306 general physicsPhysicsZeeman effectbusiness.industryLimiting021001 nanoscience & nanotechnologyAlkali metalComputational physicsNonlinear systemAmplitudesymbols0210 nano-technologybusiness
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Micro lensing induced lineshapes in a single mode cold-atom hollow-core fiber interface

2018

We report on the observation of strong transmission line shape alterations in a cold-atom-hollow-core-fiber interface. We show that this can lead to a significant overestimation of the assigned resonant optical depth for high atom densities. By modeling light beam propagation in an inhomogeneous dispersive medium, we attribute the observations to micro lensing in the atomic ensemble in combination with the mode selection of the atom-fiber interface. The approach is confirmed by studies of Rydberg electromagnetically induced transparency line shapes.

Materials scienceAtomic Physics (physics.atom-ph)Electromagnetically induced transparencyFOS: Physical sciencesPhysics::Optics02 engineering and technology01 natural sciencesMolecular physicsPhysics - Atomic Physicssymbols.namesakeOpticsTransmission lineUltracold atom0103 physical sciencesAtomLight beamPhysics::Atomic Physics010306 general physicsLine (formation)Condensed Matter::Quantum GasesQuantum Physicsbusiness.industrySingle-mode optical fiber021001 nanoscience & nanotechnologyAtomic and Molecular Physics and OpticsRydberg formulasymbolsQuantum Physics (quant-ph)0210 nano-technologybusinessOptics (physics.optics)Physics - Optics
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A single-atom heat engine

2015

Making a teeny tiny engine Steam locomotives, cars, and the drinking bird toy all convert heat into useful work as it cycles between two reservoirs at different temperatures. Usually, the working substance where the heat-work conversion occurs is a liquid or a gas, consisting of many molecules. Roβnagel et al. have made a working substance of a single calcium ion in a tapered ion trap. A laser-cooling beam plays the part of a cold reservoir for the calcium ion, and in turn, electric field noise acts as a hot reservoir. Science , this issue p. 325

Materials scienceAtomic Physics (physics.atom-ph)FOS: Physical sciences01 natural sciencesphysics.atom-phPhysics - Atomic Physics010305 fluids & plasmasIonquant-phThermodynamic cycle0103 physical sciencesThermal010306 general physicscond-mat.stat-mechCondensed Matter - Statistical MechanicsHeat engineCouplingQuantum PhysicsMultidisciplinaryStatistical Mechanics (cond-mat.stat-mech)business.industryMechanicsPower (physics)Ion trapQuantum Physics (quant-ph)businessThermal energy
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