Search results for "Physics in General"

showing 10 items of 10 documents

A test of charge-parity-time invariance at the atto-electronvolt scale

2017

We developed a novel fast measurement procedure for cyclotron frequency comparisons of two individual particles in a Penning trap, which enabled us to compare the charge-to-mass ratio of the proton and the antiproton with a fractional precision of 69 parts per trillion. To date this is the most precise test of charge-parity-time invariance using baryons. Our measurements were performed at cyclotron frequencies of about 30 MHz, which means that charge-parity-time symmetry holds at the atto-electronvolt scale.

Nuclear physicsPhysicsBaryonAntiparticleScale (ratio)Physics in GeneralAntimatterElectronvoltPräzisionsexperimente - Abteilung BlaumParity (mathematics)NucleonNuclear ExperimentAtto-
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First Ionization Potentials of Fm, Md, No, and Lr

2018

We report the first ionization potentials (IP1) of the heavy actinides, fermium (Fm, atomic number Z = 100), mendelevium (Md, Z = 101), nobelium (No, Z = 102), and lawrencium (Lr, Z = 103), determined using a method based on a surface ionization process coupled to an online mass separation technique in an atom-at-a-time regime. The measured IP1 values agree well with those predicted by state-of-the-art relativistic calculations performed alongside the present measurements. Similar to the well-established behavior for the lanthanides, the IP1 values of the heavy actinides up to No increase with filling up the 5f orbital, while that of Lr is the lowest among the actinides. These results clear…

ENERGIESThermal ionizationchemistry.chemical_element01 natural sciencesBiochemistryCatalysisColloid and Surface ChemistrySURFACE-IONIZATIONPhysics in GeneralCHEMISTRYIonization0103 physical sciencesELEMENTS010306 general physicsSPECTROSCOPY010304 chemical physicsChemistryFermiumGeneral ChemistryActinideATOMMendeleviumNobeliumAtomic numberAtomic physicsLawrenciumJournal of the American Chemical Society
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Measurement of the first ionization potential of astatine by laser ionization spectroscopy

2013

The radioactive element astatine exists only in trace amounts in nature. Its properties can therefore only be explored by study of the minute quantities of artificially produced isotopes or by performing theoretical calculations. One of the most important properties influencing the chemical behaviour is the energy required to remove one electron from the valence shell, referred to as the ionization potential. Here we use laser spectroscopy to probe the optical spectrum of astatine near the ionization threshold. The observed series of Rydberg states enabled the first determination of the ionization potential of the astatine atom, 9.31751(8) eV. New ab initio calculations are performed to sup…

Other Fields of PhysicsGeneral Physics and Astronomychemistry.chemical_element7. Clean energy01 natural sciencesGeneral Biochemistry Genetics and Molecular BiologyArticlePhysics in GeneralAb initio quantum chemistry methodsCHEMISTRYIonization0103 physical sciencesAtomPhysics::Atomic and Molecular ClustersFACILITYPhysics::Atomic Physics010306 general physicsAstatineSpectroscopyPhysicsMultidisciplinary010308 nuclear & particles physicsGeneral ChemistryION-SOURCEIon source3. Good healthchemistry13. Climate actionIonization energyAtomic physicsValence electronNature Communications
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Recent experiments at the JYFLTRAP Penning trap

2020

AbstractThe JYFLTRAP double Penning trap mass spectrometer at the Ion Guide Isotope Separator On-Line (IGISOL) facility offers excellent possibilities for high-precision mass measurements of radioactive ions. Around 400 atomic masses, including around 50 isomeric states, have been measured since JYFLTRAP became operational. JYFLTRAP has also been used as a high-resolution mass separator for decay spectroscopy experiments as well as an ion counter for fission yield studies. In this contribution, an overview of recent activities at the JYFLTRAP Penning trap is given, with a focus on nuclei discussed in the PLATAN2019 meeting.

nuclear binding energymassaspektrometriaNuclear and High Energy PhysicstutkimuslaitteetFission product yieldMass spectrometry7. Clean energy01 natural sciencesIonNuclear physicsPhysics in General0103 physical sciencesPhysical and Theoretical Chemistry010306 general physicsSpectroscopyPhysicsIsotope010308 nuclear & particles physicsatomic masspenning trapCondensed Matter PhysicsPenning trapAtomic and Molecular Physics and OpticsAtomic massNuclear binding energyisomersydinfysiikkaHyperfine Interactions
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Towards an Improved Measurement of the Proton Magnetic Moment

2017

The BASE collaboration performed the most precise measurement of the proton magnetic moment. By applying the so-called double Penning-trap method with a single proton a fractional precision of 3.3 parts-per-billion was reached. This article describes the primary limitations of the last measurement and discusses improvements to reach the sub-parts-per-billion level.

PhysicsLarmor precessionMagnetic momentProton magnetic momentCyclotronMagnetic fieldlaw.inventionPhysics in GenerallawAntimatterPrecessionPräzisionsexperimente - Abteilung BlaumAtomic physicsNucleonProceedings of the 12th International Conference on Low Energy Antiproton Physics (LEAP2016)
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High-precision measurements of the hyperfine structure of cobalt ions in the deep ultraviolet range

2023

Scientific reports 13(1), 4783 (2023). doi:10.1038/s41598-023-31378-1

MultidisciplinaryPhysics in Generalcollinear laser spectroscopyhyperfine structurespektroskopiadeep ultraviolet600IGISOLkobolttiydinfysiikkaddc:600cobalt[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Scientific Reports
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High-Precision Multiphoton Ionization of Accelerated Laser-Ablated Species

2018

We demonstrate that the pulsed-time structure and high-peak ion intensity provided by the laser-ablation process can be directly combined with the high resolution, high efficiency, and low background offered by collinear resonance ionization spectroscopy. This simple, versatile, and powerful method offers new and unique opportunities for high-precision studies of atomic and molecular structures, impacting fundamental and applied physics research. We show that even for ion beams possessing a relatively large energy spread, high-resolution hyperfine-structure measurements can be achieved by correcting the observed line shapes with the time-of-flight information of the resonantly ionized ions.…

Materials science010308 nuclear & particles physicsResearchInstitutes_Networks_Beacons/photon_science_institutePhysicsQC1-999General Physics and AstronomyPhoton Science InstituteLaser7. Clean energy01 natural scienceslaw.inventionPhysics in GenerallawIonization0103 physical sciencesPhysics::Accelerator PhysicsPhysics::Atomic PhysicsAtomic physics010306 general physics
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Sympathetic cooling of a trapped proton mediated by an LC circuit

2021

Efficient cooling of trapped charged particles is essential to many fundamental physics experiments1,2, to high-precision metrology3,4 and to quantum technology5,6. Until now, sympathetic cooling has required close-range Coulomb interactions7,8, but there has been a sustained desire to bring laser-cooling techniques to particles in macroscopically separated traps5,9,10, extending quantum control techniques to previously inaccessible particles such as highly charged ions, molecular ions and antimatter. Here we demonstrate sympathetic cooling of a single proton using laser-cooled Be+ ions in spatially separated Penning traps. The traps are connected by a superconducting LC circuit that enable…

Sympathetic coolingProtonAtomic Physics (physics.atom-ph)FOS: Physical sciencesLC circuit7. Clean energy01 natural sciencesArticle010305 fluids & plasmasIonPhysics - Atomic PhysicsPhysics in General0103 physical sciencesAtomic and molecular physicsPhysics::Atomic Physics010306 general physicsPhysicsQuantum PhysicsMultidisciplinaryCharged particleQuantum technologyAntiprotonAntimatterExotic atoms and moleculesddc:500Atomic physicsPräzisionsexperimente - Abteilung BlaumQuantum Physics (quant-ph)
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Simulation of the relative atomic populations of elements 1 ≤ Z ≤89 following charge exchange tested with collinear resonance ionization spectroscopy…

2019

© 2019 The Authors Calculations of the neutralisation cross-section and relative population of atomic states were performed for ions beams (1 ≤ Z ≤ 89) at 5 and 40 keV incident on free sodium and potassium atoms. To test the validity of the calculations, the population distribution of indium ions incident on a vapour of sodium was measured at an intermediate energy of 20 keV. The relative populations of the 5s 2 5p 2 P 1/2 and 5s 2 5p 2 P 3/2 states in indium were measured using collinear resonance ionization spectroscopy and found to be consistent with the calculations. Charge exchange contributions to high-resolution lineshapes were also investigated and found to be reproduced by the calc…

Materials sciencekaliumElectron captureSodiumPotassiumPopulationspektroskopiachemistry.chemical_elementindium01 natural sciencesAnalytical ChemistryIonatomifysiikkaPhysics in General0103 physical sciencesPhysics::Atomic Physicselectron capturenatrium010306 general physicseducationSpectroscopyInstrumentationsodiumSpectroscopyeducation.field_of_studyatomic populationsIsotopeta114010308 nuclear & particles physicspotassiumcharge exchangeAtomic and Molecular Physics and Opticssemi-classical impact parameterchemistrylaser spectroscopycollinear resonance ionization spectroscopyAtomic physicsIndiumSpectrochimica Acta Part B: Atomic Spectroscopy
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A parts-per-billion measurement of the antiproton magnetic moment

2017

The magnetic moment of the antiproton is measured at the parts-per-billion level, improving on previous measurements by a factor of about 350. Comparing the fundamental properties of normal-matter particles with their antimatter counterparts tests charge–parity–time (CPT) invariance, which is an important part of the standard model of particle physics. Many properties have been measured to the parts-per-billion level of uncertainty, but the magnetic moment of the antiproton has not. Christian Smorra and colleagues have now done so, and report that it is −2.7928473441 ± 0.0000000042 in units of the nuclear magneton. This is consistent with the magnetic moment of the proton, 2.792847350 ± 0.0…

ProtonCPT symmetry01 natural sciencesddc:070Standard ModelNuclear physicsPhysics in Generalcharge–parity–time (CPT) invariance0103 physical sciencesddc:530atomic and molecular physicsddc:510010306 general physicsNuclear magnetonPhysicsMultidisciplinaryMagnetic moment010308 nuclear & particles physicsDewey Decimal Classification::500 | Naturwissenschaften::510 | MathematikSymmetry (physics)AntiprotonAntimatterHigh Energy Physics::ExperimentDewey Decimal Classification::500 | Naturwissenschaften::530 | PhysikPräzisionsexperimente - Abteilung BlaumAntiproton Decelerator facility
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