Search results for " atom"

showing 10 items of 1526 documents

Enhanced nuclear Schiff moment in stable and metastable nuclei

2019

Nuclei with static intrinsic octupole deformation or a soft octupole vibrational mode lead to strongly enhanced collective nuclear Schiff? moments. Interaction between electrons and these Schiff moments produce enhanced time reversal (T) and parity (P) violating electric dipole moments (EDM) in atoms and molecules. Corresponding experiments may be used to test CP-violation theories predicting T,P-violating nuclear forces and to search for axions. Nuclear octupole deformations are predicted in many short lived isotopes. This paper investigates octupole deformations in stable and very long lifetime nuclei such as 153Eu, 235U, 237Np and 227Ac, which can ease atomic experiments substantially. T…

PhysicsNuclear TheoryAtomic Physics (physics.atom-ph)010308 nuclear & particles physicsNuclear TheoryFOS: Physical sciences01 natural sciencesPhysics - Atomic Physics3. Good healthNuclear Theory (nucl-th)High Energy Physics - PhenomenologyDipoleHigh Energy Physics - Phenomenology (hep-ph)Metastability0103 physical sciencesPhysics::Atomic and Molecular ClustersNuclear forceMoleculePhysics::Atomic PhysicsAtomic physicsNuclear Experiment010306 general physicsAxionNuclear theoryPhysical Review C
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Two-photon exchange on the neutron and the hyperfine splitting

2018

We calculate the contribution from the two-photon exchange on the neutron to the hyperfine splitting of S energy levels. We update the value of the neutron Zemach radius, estimate total recoil and polarizability corrections. The resulting two-photon exchange in electronic atoms exceeds by an order of magnitude the leading Zemach term and has different sign both in electronic and muonic hydrogen.

PhysicsNuclear TheoryAtomic Physics (physics.atom-ph)FOS: Physical sciencesRadiusPhysics - Atomic PhysicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)RecoilPolarizabilityNeutronPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)Atomic physicsNuclear ExperimentHyperfine structureOrder of magnitudeExotic atomSign (mathematics)Physical Review D
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Breakdown of the expansion of finite-size corrections to the hydrogen Lamb shift in moments of charge distribution

2015

We quantify a limitation in the usual accounting of the finite-size effects, where the leading $[(Z\alpha)^4]$ and subleading $[(Z\alpha)^5]$ contributions to the Lamb shift are given by the mean-square radius and the third Zemach moment of the charge distribution. In the presence of any non-smooth behaviour of the nuclear form factor at scales comparable to the inverse Bohr radius, the expansion of the Lamb shift in the moments breaks down. This is relevant for some of the explanations of the "proton size puzzle". We find, for instance, that the de R\'ujula toy model of the proton form factor does not resolve the puzzle as claimed, despite the large value of the third Zemach moment. Withou…

PhysicsNuclear TheoryProtonAtomic Physics (physics.atom-ph)Form factor (quantum field theory)Electric form factorFOS: Physical sciencesRadiusAtomic and Molecular Physics and OpticsPhysics - Atomic PhysicsLamb shiftNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Charge radiusQuantum mechanicsMoment (physics)Atomic physicsBohr radiusPhysical Review A
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Magnetic field driven enhancement of the weak decay width of charged pions

2020

We study the effect of a uniform magnetic field B→ on the decays π⁻ → l⁻ ν⁻l, where l⁻ = e⁻, μ⁻, carrying out a general analysis that includes four π⁻ decay constants. Taking the values of these constants from a chiral effective Nambu-Jona-Lasinio (NJL) model, it is seen that the total decay rate gets strongly increased with respect to the B = 0 case, with an enhancement factor ranging from ∼ 10 for eB = 0.1 GeV² up to ∼ 10³ for eB = 1 GeV². The ratio between electronic and muonic decays gets also enhanced, reaching a value of about 1 : 2 for eB = 1 GeV². In addition, we find that for large B the angular distribution of outgoing antineutrinos shows a significant suppression in the direction…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciences//purl.org/becyt/ford/1.3 [https]QCD Phenomenology7. Clean energy01 natural sciencesMagnetic fieldNuclear physics//purl.org/becyt/ford/1 [https]High Energy Physics - PhenomenologyPionHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::Experiment010306 general physicsCiencias Exactas
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Calibration of the ISOLDE acceleration voltage using a high-precision voltage divider and applying collinear fast beam laser spectroscopy

2011

A high-voltage divider with accuracy at the ppm level and collinear laser spectroscopy were used to calibrate the highvoltage installation at the radioactive ion beam facility ISOLDE at CERN. The accurate knowledge of this voltage is particularly important for collinear laser spectroscopy measurements. Beam velocity measurements using frequencycomb based collinear laser spectroscopy agree with the new calibration. Applying this, one obtains consistent results for isotope shifts of stable magnesium isotopes measured using collinear spectroscopy and laser spectroscopy on laser-cooled ions in a trap. The long-term stability and the transient behavior during recovery from a voltage dropout were…

PhysicsNuclear and High Energy PhysicsIon beamAtomic Physics (physics.atom-ph)Voltage dividerOther Fields of PhysicsFOS: Physical sciencesLaserAcceleration voltagelaw.inventionPhysics - Atomic PhysicslawCalibrationPhysics::Accelerator PhysicsPhysics::Atomic PhysicsAtomic physicsDetectors and Experimental TechniquesSpectroscopyNuclear ExperimentInstrumentationBeam (structure)Voltage
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Behavior of the nuclear charge radii systematics in thes-dshell from muonic atom measurements

1992

The present work extends the systematics of nuclear charge radii obtained by the method of muonic atoms to nuclei with 8\ensuremath{\le}Z,N\ensuremath{\le}20. The accuracy of the measured muonic Lyman transition energies of generally \ensuremath{\le}10 eV leads to a precision in the model-independent nuclear charge radii differences of 2--3 am for the isotope shifts and 4--9 am for isotone shifts. Both isotope and isotone shifts within the s-d shell behave ``anomalously'' with respect to the systematics of heavier nuclei. However, such behavior is predicted on theoretical grounds, if mixing in the s-d shells and the strong deformation of some of the nuclei in this region are considered. We …

PhysicsNuclear and High Energy PhysicsIsotopeScatteringIsotoneNuclear TheoryShell (structure)Charge densityCharge (physics)Effective nuclear chargePhysics::Atomic PhysicsAtomic physicsNuclear ExperimentExotic atomPhysical Review C
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Nuclear charge radii of the tin isotopes from muonic atoms.

1990

The muonic atom 2${\mathit{p}}_{1/2}$-1${\mathit{s}}_{1/2}$ and 2${\mathit{p}}_{3/2}$-1${\mathit{s}}_{1/2}$ transition energies were measured with an experimental accuracy of better than 20 ppm for the isotope chain $^{112,114,116,117,118,119,120,122,124}\mathrm{Sn}$. Precise values for the Barrett equivalent nuclear radii ${\mathit{R}}_{\mathit{k}\mathrm{\ensuremath{\alpha}}}$ and their differences as well as root-mean-square radii were deduced. The \ensuremath{\Delta}N=2 isotope shifts between the even Sn isotopes show a subshell effect at the neutron number N=64. Otherwise, there is a nearly linear decrease with increasing N, in accordance with the general systematics of nuclear charge r…

PhysicsNuclear and High Energy PhysicsMuonNeutron numberIsotopes of tinCharge densityElementary particlePhysics::Atomic PhysicsAtomic physicsEffective nuclear chargeExotic atomLeptonPhysical review. C, Nuclear physics
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Ab initio calculation of nuclear structure corrections in muonic atoms

2018

The measurement of the Lamb shift in muonic hydrogen and the subsequent emergence of the proton-radius puzzle have motivated an experimental campaign devoted to measuring the Lamb shift in other light muonic atoms, such as muonic deuterium and helium. For these systems it has been shown that two-photon exchange nuclear structure corrections are the largest source of uncertainty and consequently the bottleneck for exploiting the experimental precision to extract the nuclear charge radius. Utilizing techniques and methods developed to study electromagnetic reactions in light nuclei, recent calculations of nuclear structure corrections to the muonic Lamb shift have reached unprecedented precis…

PhysicsNuclear and High Energy PhysicsNuclear Theory010308 nuclear & particles physicsAtomic Physics (physics.atom-ph)FOS: Physical sciences01 natural sciencesEffective nuclear charge3. Good healthLamb shiftPhysics - Atomic PhysicsNuclear physicsNuclear Theory (nucl-th)DeuteriumCharge radius0103 physical sciencesEffective field theoryPhysics::Atomic and Molecular ClustersVacuum polarizationSum rule in quantum mechanicsPhysics::Atomic Physics010306 general physicsExotic atom
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The RMS charge radius of the proton and Zemach moments

2010

On the basis of recent precise measurements of the electric form factor of the proton, the Zemach moments, needed as input parameters for the determination of the proton rms radius from the measurement of the Lamb shift in muonic hydrogen, are calculated. It turns out that the new moments give an uncertainty as large as the presently stated error of the recent Lamb shift measurement of Pohl et al.. De Rujula's idea of a large Zemach moment in order to reconcile the five standard deviation discrepancy between the muonic Lamb shift determination and the result of electronic experiments is shown to be in clear contradiction with experiment. Alternative explanations are touched upon.

PhysicsNuclear and High Energy PhysicsNuclear TheoryProtonElectric form factorFOS: Physical sciencesCharge densityRadiusLamb shiftNuclear Theory (nucl-th)Charge radiusQuantum electrodynamicsMoment (physics)Physics::Atomic PhysicsNuclear Experiment (nucl-ex)Atomic physicsNuclear ExperimentExotic atomPhysics Letters B
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Bounds on the triplet fermions in type-III seesaw and implications for collider searches

2021

Type-III seesaw is a simple extension of the Standard Model~(SM) with the SU$(2)_\text{L}$ triplet fermion with zero hypercharge. It can explain the origin of the tiny neutrino mass and flavor mixing. After the electroweak symmetry breaking the light neutrino mass is generated by the seesaw mechanism which further ensures the mixings between the light neutrino and heavy neutral lepton mass eigenstates. If the triplet fermions are around the electroweak scale having sizable mixings with the SM sector allowed by the correct gauge symmetry, they can be produced at the high energy colliders leaving a variety of characteristic signatures. Based on a simple and concrete realizations of the model …

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesQC770-79801 natural sciencesStandard ModelHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismSeesaw molecular geometryNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesHigh Energy Physics::ExperimentNeutrinoElectroweak scale010306 general physicsNeutrino oscillationLepton
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