Search results for "physics.atom-ph"

showing 10 items of 395 documents

The subtraction contribution to the muonic-hydrogen Lamb shift: a point for lattice QCD calculations of the polarizability effect

2020

The proton-polarizability contribution to the muonic-hydrogen Lamb shift is a major source of theoretical uncertainty in the extraction of the proton charge radius. An empirical evaluation of this effect, based on the proton structure functions, requires a systematically improvable calculation of the "subtraction function", possibly using lattice QCD. We consider a different subtraction point, with the aim of accessing the subtraction function directly in lattice calculations. A useful feature of this subtraction point is that the corresponding contribution of the structure functions to the Lamb shift is suppressed. The whole effect is dominated by the subtraction contribution, calculable o…

Nuclear and High Energy PhysicsNuclear TheoryAtomic Physics (physics.atom-ph)FOS: Physical sciences01 natural sciencesPhysics - Atomic PhysicsNuclear Theory (nucl-th)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Charge radiusPolarizabilityLattice (order)0103 physical sciencesPhysics::Atomic Physics010306 general physicsExotic atomPhysics010308 nuclear & particles physicsStructure functionHigh Energy Physics - Lattice (hep-lat)SubtractionLattice QCD3. Good healthLamb shiftHigh Energy Physics - PhenomenologyQuantum electrodynamics
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Weak quadrupole moments

2017

Collective effects in deformed atomic nuclei present possible avenues of study on the non-spherical distribution of neutrons and the violation of the local Lorentz invariance. We introduce the weak quadrupole moment of nuclei, related to the quadrupole distribution of the weak charge in the nucleus. The weak quadrupole moment produces tensor weak interaction between the nucleus and electrons and can be observed in atomic and molecular experiments measuring parity nonconservation. The dominating contribution to the weak quadrupole is given by the quadrupole moment of the neutron distribution, therefore, corresponding experiments should allow one to measure the neutron quadrupoles. Using the …

Nuclear and High Energy PhysicsNuclear TheoryAtomic Physics (physics.atom-ph)Lorentz transformationNuclear TheoryFOS: Physical sciencesElectronLorentz covarianceWeak interaction01 natural sciencesPhysics - Atomic PhysicsNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutronPhysics::Atomic Physics010306 general physicsPhysics010308 nuclear & particles physicsParity (physics)High Energy Physics - PhenomenologyQuadrupoleAtomic nucleussymbolsPhysics::Accelerator PhysicsAtomic physicsJournal of Physics G: Nuclear and Particle Physics
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Implementing the three-particle quantization condition including higher partial waves

2019

We present an implementation of the relativistic three-particle quantization condition including both $s$- and $d$-wave two-particle channels. For this, we develop a systematic expansion about threshold of the three-particle divergence-free K matrix, $\mathcal{K}_{\mathrm{df,3}}$, which is a generalization of the effective range expansion of the two-particle K matrix, $\mathcal{K}_2$. Relativistic invariance plays an important role in this expansion. We find that $d$-wave two-particle channels enter first at quadratic order. We explain how to implement the resulting multichannel quantization condition, and present several examples of its application. We derive the leading dependence of the …

Nuclear and High Energy PhysicsNuclear TheoryAtomic Physics (physics.atom-ph)Relativistic invarianceFOS: Physical sciencesLattice QCD01 natural sciencesPhysics - Atomic PhysicsNuclear Theory (nucl-th)Quantization (physics)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBound statelcsh:Nuclear and particle physics. Atomic energy. RadioactivityQuadratic orderScattering Amplitudes010306 general physicsNuclear theoryCondensed Matter - Statistical MechanicsK matrixMathematical physicsPhysicsLattice Quantum Field TheoryStatistical Mechanics (cond-mat.stat-mech)010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Lattice QCDScattering amplitudeHigh Energy Physics - Phenomenologylcsh:QC770-798Journal of High Energy Physics
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Parity-violating interactions of cosmic fields with atoms, molecules, and nuclei: Concepts and calculations for laboratory searches and extracting li…

2014

We propose methods and present calculations that can be used to search for evidence of cosmic fields by investigating the parity-violating effects, including parity nonconservation amplitudes and electric dipole moments, that they induce in atoms. The results are used to constrain important fundamental parameters describing the strength of the interaction of various cosmic fields with electrons, protons, and neutrons. Candidates for such fields are dark matter (including axions) and dark energy, as well as several more exotic sources described by standard-model extensions. Existing parity nonconservation experiments in Cs, Dy, Yb, and Tl are combined with our calculations to directly place …

Nuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Nuclear TheoryAtomic Physics (physics.atom-ph)Dark matterFOS: Physical sciencesCosmic rayElectron01 natural sciencesPhysics - Atomic PhysicsNuclear physicsNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Physics - Space Physics0103 physical sciencesNeutron010306 general physicsNuclear ExperimentPseudovectorPhysics010308 nuclear & particles physicsSpace Physics (physics.space-ph)PseudoscalarDipoleHigh Energy Physics - PhenomenologyNucleonAstrophysics - Cosmology and Nongalactic Astrophysics
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New generation low-energy probes for ultralight axion and scalar dark matter

2017

We present a brief overview of a new generation of high-precision laboratory and astrophysical measurements to search for ultralight (sub-eV) axion, axion-like pseudoscalar and scalar dark matter, which form either a coherent condensate or topological defects (solitons). In these new detection methods, the sought effects are linear in the interaction constant between dark matter and ordinary matter, which is in stark contrast to traditional searches for dark matter, where the sought effects are quadratic or higher order in the underlying interaction constants (which are extremely small).

Nuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Nuclear TheoryAtomic Physics (physics.atom-ph)Dark matterGeneral Physics and AstronomyFOS: Physical sciences01 natural sciencesPhysics - Atomic PhysicsTopological defectNuclear Theory (nucl-th)Quadratic equationHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsAxionPhysics010308 nuclear & particles physicsAstronomy and AstrophysicsPseudoscalarHigh Energy Physics - PhenomenologyStrong CP problemSolitonAstrophysics - Cosmology and Nongalactic AstrophysicsCoherence (physics)
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Demonstration of sensitivity increase in mercury free-spin-precession magnetometers due to laser-based readout for neutron electric dipole moment sea…

2018

International audience; We report on a laser based $^{199}$Hg co-magnetometer deployed in an experiment searching for a permanent electric dipole moment of the neutron. We demonstrate a more than five times increased signal to-noise-ratio in a direct comparison measurement with its $^{204}$Hg discharge bulb-based predecessor. An improved data model for the extraction of important system parameters such as the degrees of absorption and polarization is derived. Laser- and lamp-based data-sets can be consistently described by the improved model which permits to compare measurements using the two different light sources and to explain the increase in magnetometer performance. The laser-based ma…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsNeutron electric dipole momentAtomic Physics (physics.atom-ph)Magnetometeratomic spectroscopyFOS: Physical sciencesAtomic spectroscopyNeutronelectric dipole moment[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural scienceslaw.inventionHigh Energy Physics - ExperimentPhysics - Atomic PhysicsHigh Energy Physics - Experiment (hep-ex)symbols.namesakeneutronlaw0103 physical sciencesNeutron[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det][ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)010306 general physicsZeeman effect; Atomic spectroscopy; Mercury; Electric dipole moment; Neutron[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]InstrumentationNuclear ExperimentPhysicsZeeman effectElectric dipole moment010308 nuclear & particles physicsInstrumentation and Detectors (physics.ins-det)Zeeman effectMercuryLaserComputational physicsMagnetic fieldElectric dipole momentAtomic spectroscopysymbols
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A facility for production and laser cooling of cesium isotopes and isomers

2018

We report on the design, installation, and test of an experimental facility for the production of ultra-cold atomic isotopes and isomers of cesium. The setup covers a broad span of mass numbers and nuclear isomers, allowing one to directly compare chains of isotopes and isotope/isomer pairs. Cesium nuclei are produced by fission or fusion-evaporation reactions using primary proton beams from a 130 MeV cyclotron impinging upon a suitable target. The species of interest is ejected from the target in ionic form, electrostatically accelerated, mass separated, and routed to a science chamber. Here, ions are neutralized by implantation in a thin foil, and extracted by thermal diffusion. A neutral…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsProtonCesium IsotopesAtomic Physics (physics.atom-ph)FissiontutkimuslaitteetCyclotronFOS: Physical scienceschemistry.chemical_element7. Clean energy01 natural sciencesPhysics - Atomic Physicslaw.inventionIonlaser coolinglawLaser cooling0103 physical sciencesPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear ExperimentInstrumentationPhysicsultra-cold nucleita114Isotope010308 nuclear & particles physicsInstrumentation and Detectors (physics.ins-det)3. Good healthchemistryCaesiumAtomic physicsydinfysiikkaisotopes and isomersNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Demonstration of the double Penning Trap technique with a single proton

2013

Spin flips of a single proton were driven in a Penning trap with a homogeneous magnetic field. For the spin-state analysis the proton was transported into a second Penning trap with a superimposed magnetic bottle, and the continuous Stern-Gerlach effect was applied. This first demonstration of the double Penning trap technique with a single proton suggests that the antiproton magnetic moment measurement can potentially be improved by three orders of magnitude or more. Spin flips of a single proton were driven in a Penning trap with a homogeneous magnetic field. For the spin-state analysis the proton was transported into a second Penning trap with a superimposed magnetic bottle, and the cont…

Nuclear and High Energy PhysicsProtonOrders of magnitude (temperature)Atomic Physics (physics.atom-ph)Other Fields of PhysicsFOS: Physical sciencesGeonium atomPenning traps01 natural sciencesphysics.atom-phPhysics - Atomic Physics010305 fluids & plasmasFundamental symmetries0103 physical sciencesPhysics::Atomic and Molecular ClustersPhysics::Atomic Physics010306 general physicsSpin (physics)Nuclear ExperimentPhysicsPenning trapCPT testsMagnetic fieldAntiprotonPhysics::Accelerator PhysicsIon trapAtomic physicsPhysics Letters B
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Scintillation light produced by low-energy beams of highly-charged ions

2007

Measurements have been performed of scintillation light intensities emitted from various inorganic scintillators irradiated with low-energy beams of highly-charged ions from an electron beam ion source (EBIS) and an electron cyclotron resonance ion source (ECRIS). Beams of xenon ions Xe$^{q+}$ with various charge states between $q$=2 and $q$=18 have been used at energies between 5 keV and 17.5 keV per charge generated by the ECRIS. The intensity of the beam was typically varied between 1 and 100 nA. Beams of highly charged residual gas ions have been produced by the EBIS at 4.5 keV per charge and with low intensities down to 100 pA. The scintillator materials used are flat screens of P46 YA…

Nuclear and High Energy PhysicsScintillationPhysics - Instrumentation and DetectorsIon beamChemistryPhysics::Instrumentation and DetectorsAtomic Physics (physics.atom-ph)FOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)ScintillatorIon gunIon sourceIonPhysics - Atomic PhysicsLight intensityIon beam depositionPhysics::Accelerator PhysicsAtomic physicsInstrumentation
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First application of the Laser Ion Source and Trap (LIST) for on-line experiments at ISOLDE

2012

The Laser Ion Source and Trap (LIST) provides a new mode of operation for the resonance ionization laser ion source (RILIS) at ISOLDE/CERN, reducing the amount of surface-ionized isobaric contaminants by up to four orders of magnitude. After the first successful on-line test at ISOLDE in 2011 the LIST was further improved in terms of efficiency, selectivity, and reliability through several off-line tests at Mainz University and at ISOLDE. In September 2012, the first on-line physics experiments to use the LIST took place at ISOLDE. The measurements of the improved LIST indicate more than a twofold increase in efficiency compared to the LIST of the 2011 run. The suppression of surface-ionize…

Nuclear and High Energy Physics[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Ion trapchemistry.chemical_element01 natural sciencesIn-source laser spectroscopylaw.inventionFranciumTrap (computing)LISTlawIonization0103 physical sciences010306 general physicsInstrumentationLaser ion sourceLarge Hadron Collider[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]010308 nuclear & particles physicsChemistryOn-line mass separatorOrders of magnitude (angular velocity)LaserIon sourceIon trapAtomic physics
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