Search results for "Penning trap"

showing 10 items of 297 documents

A quartz amplifier for high-sensitivity Fourier-transform ion-cyclotron-resonance measurements with trapped ions

2019

Single-ion sensitivity is obtained in precision Penning-trap experiments devoted to light (anti)particles or ions with low mass-to-charge ratios, by adding an inductance coil to an amplifier connected to the trap, both operated at 4 K. However, single-ion sensitivity has not been reached on heavy singly or doubly charged ions. In this publication, we present a new system to reach this point, based on the use of a quartz crystal as an inductance, together with a newly developed broad-band (BB) amplifier. We detect the reduced-cyclotron frequency of 40Ca+ ions stored in a 7-tesla open-ring Penning trap. By comparing the detected electric signal obtained with the BB amplifier and the fluoresce…

010302 applied physicsMaterials scienceEquivalent series resistanceAmplifierPenning trap01 natural sciences7. Clean energySignalFourier transform ion cyclotron resonance010305 fluids & plasmasIonCrystal0103 physical sciencesAtomic physicsInstrumentationSensitivity (electronics)Review of Scientific Instruments
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Theoretical and experimental studies of the neutron rich fission product yields at intermediate energies

2012

A new method to measure the fission product independent yields employing the ion guide technique and a Penning trap as a precision mass filter, which allows an unambiguous identification of the nuclides is presented. The method was used to determine the independent yields in the proton-induced fission of 232 Th and 238 U at 25 MeV. The data were analyzed with the consistent model for description of the fission product formation cross section at the projectile energies up to 100 MeV. Pre-compound nucleon emission is described with the two-component exciton model using Monte Carlo method. Decay of excited compound nuclei is treated within time-dependent statistical model with inclusion of the…

010302 applied physicsNuclear fission productCluster decay010308 nuclear & particles physicsFissionChemistryPhysicsQC1-999Nuclear TheoryPenning trap01 natural sciences7. Clean energyNuclear physics0103 physical sciencesNeutronNuclideAtomic physicsNuclear ExperimentNucleonNuclear densityEPJ Web of Conferences
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On-line commissioning of SHIPTRAP

2006

Abstract The on-line commissioning of the Penning-trap mass spectrometer SHIPTRAP was successfully completed with a mass measurement of holmium and erbium radionuclides produced at SHIP. A large fraction of contaminant ions created in the stopping cell was identified to originate from the buffer-gas supply system. Using a liquid nitrogen cold trap they were reduced to a tolerable amount and mass measurements of Er 147 , Er 148 , and Ho 147 with relative uncertainties of about 1 × 1 0 − 6 were performed.

010308 nuclear & particles physicsAnalytical chemistrychemistry.chemical_elementLiquid nitrogen[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Condensed Matter PhysicsMass spectrometryPenning trap01 natural sciencesAtomic massIonMasschemistry07.75.+h; 21.10.Dr0103 physical sciencesPhysical and Theoretical Chemistry010306 general physicsHolmiumInstrumentationSpectroscopyCold trap
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A New Experiment for the Measurement of the g-Factors of 3He+ and 3He2+.

2018

We describe a new experiment that aims at a parts per billion measurement of the nuclear magnetic moment of 3He2+ and a 100 parts per trillion measurement of the Zeeman effect of the ground-state hyperfine splitting of 3He+. To enable ultrafast and efficient experiment cycles the experiment relies on new technologies such as sympathetic laser cooling of single 3He-ions coupled to a cloud of Doppler-cooled 9Be-ions in a Penning trap or a novel spin-state detection scheme.

0301 basic medicinePhysicsHistoryZeeman effectPenning trap01 natural sciencesComputer Science ApplicationsEducation03 medical and health sciencessymbols.namesake030104 developmental biologyLaser coolingTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesNuclear magnetic momentsymbolsPhysics::Atomic PhysicsAtomic physicsPräzisionsexperimente - Abteilung Blaum010306 general physicsUltrashort pulseHyperfine structure
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Buffer-gas-free mass-selective ion centering in Penning traps by simultaneous dipolar excitation of magnetron motion and quadrupolar excitation for i…

2012

A new excitation scheme of the radial ion-motional modes is introduced for Penning-trap ion-cyclotron-resonance experiments. By simultaneous dipolar excitation of the magnetron motion and resonant quadrupolar excitation for the conversion between magnetron motion and cyclotron motion, a mass-selective recentering of the ions of interest is performed while all other (contaminant) ions are ejected from the trap. This new technique does not rely on the application of a buffer gas as presently used [G. Savard, St. Becker, G. Bollen, H.-J. Kluge, R.B. Moore, Th. Otto, L Schweikhard, H. Stolzenberg, U. Wiess, Physics Letters A 158 (1991) 247] and will thus prevent charge-exchange reactions and da…

ACCURACYBuffer gasCyclotronMotion (geometry)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ISOLTRAP01 natural sciencesIonlaw.inventionlaw0103 physical sciencesPhysical and Theoretical Chemistry010306 general physicsInstrumentationSpectroscopyNUCLEIChemistry010401 analytical chemistryRAMSEY METHODRESONANCECondensed Matter PhysicsPenning trap0104 chemical sciencesCAPTUREDipoleOCTUPOLAR EXCITATIONSPECTROMETRYCavity magnetronMODESAtomic physicsAXIALIZATIONExcitationInternational Journal of Mass Spectrometry
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First isomeric yield ratio measurements by direct ion counting and implications for the angular momentum of the primary fission fragments

2018

We report the first experimental determination of independent isomeric yield ratios using direct ion counting with a Penning trap, which offered such a high resolution in mass that isomeric states could be separated. The measurements were performed at the Ion Guide Isotope Separator On-Line (IGISOL) facility at the University of Jyvaskyla. The isomer production ratios of Ge-81, Y-96,Y-97 Sn-128(,1)30, and Sb-129 in the 25-MeV proton-induced fission of U-na(t) and Th-232 were studied. Three isomeric pairs (Ge-81, Y-96, and Sb-129) were measured for the first time for the U-na(t)(p, f) reaction, while all the reported yield ratios for the Th-232(p, f) reaction were determined for the first ti…

Angular momentumResolution (mass spectrometry)Fission01 natural sciencesIonSubatomär fysikydinreaktiotPrimary (astronomy)0103 physical sciencesSubatomic PhysicsPhysics::Atomic and Molecular ClustersfissionYield ratioPhysics::Atomic PhysicsPhysics::Chemical PhysicsNuclear Experiment010306 general physicsnuclear reactionsPhysicsta114010308 nuclear & particles physicsPenning trapfissioYield (chemistry)Atomic physicsisomer decaysydinfysiikka
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Sixfold improved single particle measurement of the magnetic moment of the antiproton

2017

Our current understanding of the Universe comes, among others, from particle physics and cosmology. In particle physics an almost perfect symmetry between matter and antimatter exists. On cosmological scales, however, a striking matter/antimatter imbalance is observed. This contradiction inspires comparisons of the fundamental properties of particles and antiparticles with high precision. Here we report on a measurement of the g-factor of the antiproton with a fractional precision of 0.8 parts per million at 95% confidence level. Our value /2=2.7928465(23) outperforms the previous best measurement by a factor of 6. The result is consistent with our proton g-factor measurement gp/2=2.7928473…

AntiparticleParticle physicsLorentz transformationSciencelorentzGeneral Physics and Astronomysystem01 natural sciencesArticleGeneral Biochemistry Genetics and Molecular BiologyCosmologyNuclear physicssymbols.namesakeStandard-Model Extension0103 physical sciencesNuclear Physics - Experimentcpt010306 general physicsNuclear ExperimentPhysicsMultidisciplinary010308 nuclear & particles physicsQpenning trapParity (physics)General ChemistryPenning trapAntiprotonAntimattersymbolstestsddc:500Präzisionsexperimente - Abteilung Blaum
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Efficient transfer of positrons from a buffer-gas-cooled accumulator into an orthogonally oriented superconducting solenoid for antihydrogen studies

2012

Positrons accumulated in a room-temperature buffer-gas-cooled positron accumulator are efficiently transferred into a superconducting solenoid which houses the ATRAP cryogenic Penning trap used in antihydrogen research. The positrons are guided along a 9 m long magnetic guide that connects the central field lines of the 0.15 T field in the positron accumulator to the central magnetic field lines of the superconducting solenoid. Seventy independently controllable electromagnets are required to overcome the fringing field of the large-bore superconducting solenoid. The guide includes both a 15° upward bend and a 105° downward bend to account for the orthogonal orientation of the positron accu…

Antiparticlesuperconductivity [solenoid]Physics::Instrumentation and DetectorsPenning trapGeneral Physics and Astronomybeam transportSuperconducting magnetlaw.inventionenergy spectrum [positron]Nuclear physicslawddc:530AntihydrogenPhysicsElectromagnetspatial distribution [magnetic field]ATRAPPenning trapMagnetic fieldbeam opticscryogenicsAntimatterMagnetPhysics::Accelerator Physicsaccumulator [positron]Atomic physicsperformanceNew Journal of Physics
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Constraints on the Coupling between Axionlike Dark Matter and Photons Using an Antiproton Superconducting Tuned Detection Circuit in a Cryogenic Penn…

2021

We constrain the coupling between axionlike particles (ALPs) and photons, measured with the superconducting resonant detection circuit of a cryogenic Penning trap. By searching the noise spectrum of our fixed-frequency resonant circuit for peaks caused by dark matter ALPs converting into photons in the strong magnetic field of the Penning-trap magnet, we are able to constrain the coupling of ALPs with masses around $2.7906-2.7914\,\textrm{neV/c}^2$ to $g_{a\gamma}< 1 \times 10^{-11}\,\textrm{GeV}^{-1}$. This is more than one order of magnitude lower than the best laboratory haloscope and approximately 5 times lower than the CERN axion solar telescope (CAST), setting limits in a mass and cou…

Astrophysics and AstronomyCosmology and Nongalactic Astrophysics (astro-ph.CO)PhotonAtomic Physics (physics.atom-ph)Dark matterOther Fields of PhysicsFOS: Physical sciencesGeneral Physics and Astronomyphysics.atom-ph01 natural sciences7. Clean energyPhysics - Atomic PhysicsNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesddc:530Physics::Atomic Physics010306 general physicsParticle Physics - PhenomenologySuperconductivityPhysicshep-phPenning trapCoupling (probability)Magnetic fieldHigh Energy Physics - PhenomenologyAntiprotonastro-ph.COPräzisionsexperimente - Abteilung BlaumCERN Axion Solar TelescopeAstrophysics - Cosmology and Nongalactic AstrophysicsPhysical Review Letters
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Improved comparison of bar P and P charge-to-mass ratios

1995

The measured ratio of charge-to-mass ratios for the antiproton and proton is 1.000 000 001 5 ± 0.000 000 001 1. This 1 part in 109 comparison (1 ppb) is possible because a single or p is now directly observed while trapped in an open access Penning trap. The comparison is the most accurate mass spectrometry of particles with opposite charge and is the most sensitive test of CPT invariance for a baryon system. It is 40 times more accurate than our earlier comparison with many trapped antiprotons and protons, and is more than 45 000 times more accurate than earlier comparisons made with other techniques.

BaryonPhysicsProtonCPT symmetryAntiprotonCharge (physics)Atomic physicsCondensed Matter PhysicsMass spectrometryPenning trapMathematical PhysicsAtomic and Molecular Physics and OpticsBar (unit)Physica Scripta
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