0000000000441468

AUTHOR

Mikhail Goncharov

showing 4 related works from this author

The decay energy of the pure s-process nuclide ¹²³ Te

2016

Physics letters / B 758, 407 - 411 (2016). doi:10.1016/j.physletb.2016.04.059

Penning-trap mass spectrometryPhysicsNuclear and High Energy Physics010308 nuclear & particles physicsElectron captureAtomic massesIonic bondingAstrophysicsMass spectrometry53001 natural scienceslcsh:QC1-999Atomic massNuclear physicsMassDecay energyTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesddc:530NuclidePräzisionsexperimente - Abteilung BlaumAtomic physics010306 general physicss-processlcsh:Physics
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Phase-Imaging Ion-Cyclotron-Resonance Measurements for Short-Lived Nuclides

2013

A novel approach based on the projection of the Penning-trap ion motion onto a position-sensitive detector opens the door to very accurate mass measurements on the ppb level even for short-lived nuclides with half-lives well below a second. In addition to the accuracy boost, the new method provides a superior resolving power by which low-lying isomeric states with excitation energy on the 10-keV level can be easily separated from the ground state. A measurement of the mass difference of ^{130}Xe and ^{129}Xe has demonstrated the great potential of the new approach.

Physics010308 nuclear & particles physicsDetectorGeneral Physics and AstronomyMass spectrometry01 natural sciences7. Clean energyIon trappingIonNuclear physics0103 physical sciencesNuclideAtomic physics010306 general physicsGround stateExcitationIon cyclotron resonancePhysical Review Letters
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Direct Measurement of the Mass Difference ofHo163andDy163Solves theQ-Value Puzzle for the Neutrino Mass Determination

2015

The atomic mass difference of (163)Ho and (163)Dy has been directly measured with the Penning-trap mass spectrometer SHIPTRAP applying the novel phase-imaging ion-cyclotron-resonance technique. Our measurement has solved the long-standing problem of large discrepancies in the Q value of the electron capture in (163)Ho determined by different techniques. Our measured mass difference shifts the current Q value of 2555(16) eV evaluated in the Atomic Mass Evaluation 2012 [G. Audi et al., Chin. Phys. C 36, 1157 (2012)] by more than 7σ to 2833(30(stat))(15(sys)) eV/c(2). With the new mass difference it will be possible, e.g., to reach in the first phase of the ECHo experiment a statistical sensit…

Physics010308 nuclear & particles physicsElectron captureQ valueElectron rest massGeneral Physics and AstronomyMass spectrometry7. Clean energy01 natural sciencesBeta decayAtomic massNuclear physicsAtomic mass constant0103 physical sciencesNeutrino010306 general physicsPhysical Review Letters
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Isotope dependence of the Zeeman effect in lithium-like calcium

2016

The magnetic moment μ of a bound electron, generally expressed by the g-factor μ=−g μB s ħ−1 with μB the Bohr magneton and s the electron's spin, can be calculated by bound-state quantum electrodynamics (BS-QED) to very high precision. The recent ultra-precise experiment on hydrogen-like silicon determined this value to eleven significant digits, and thus allowed to rigorously probe the validity of BS-QED. Yet, the investigation of one of the most interesting contribution to the g-factor, the relativistic interaction between electron and nucleus, is limited by our knowledge of BS-QED effects. By comparing the g-factors of two isotopes, it is possible to cancel most of these contributions an…

ScienceGeneral Physics and Astronomychemistry.chemical_elementElectron01 natural sciencesGeneral Biochemistry Genetics and Molecular BiologyArticle010305 fluids & plasmasIonBohr magnetonsymbols.namesakeRecoilNuclear magnetic resonance0103 physical sciencesPhysics::Atomic Physics010306 general physicsSpin (physics)Nuclear ExperimentPhysicsCondensed Matter::Quantum GasesMultidisciplinaryZeeman effectMagnetic momentQGeneral ChemistrychemistrysymbolsLithiumddc:500Präzisionsexperimente - Abteilung BlaumAtomic physicsNature Communications
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