Search results for "Penn"

showing 10 items of 568 documents

High-accuracy mass determination of unstable cesium and barium isotopes

1999

Direct mass measurements of short-lived Cs and Ba isotopes have been performed with the tandem Penning trap mass spectrometer ISOLTRAP installed at the on-line isotope separator ISOLDE at CERN. Typically, a mass resolving power of 600 000 and an accuracy of $\delta \mbox{m} \approx 13$ keV have been obtained. The masses of $^{123,124,126}$Ba and $^{122m}$Cs were measured for the first time. A least-squares adjustment has been performed and the experimental masses are compared with theoretical ones, particularly in the frame of a macroscopic-microscopic model.

PhysicsNuclear and High Energy PhysicsIsotope[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]010308 nuclear & particles physicschemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometryPenning trap7. Clean energy01 natural sciencesISOLTRAPAtomic massNuclear physicsMasschemistryCaesium0103 physical sciencesNuclear Physics - ExperimentAtomic physicsNuclear Experiment010306 general physicsHybrid mass spectrometer
researchProduct

Electron and positron cooling of highly charged ions in a cooler Penning trap

2004

Abstract Electron cooling is a well-established technique to increase the phase space density of particle beams in storage rings. In this paper, we discuss the feasibility of electron and positron cooling of ions in a Penning trap. We calculate the cooling times for the cases of trapped bare ions with nuclear charge Z =1 (protons), Z =36 (krypton) and Z =92 (uranium) with the Spitzer formula. Our calculations show that for typical experimental conditions the time for cooling from initial energies of 10 keV per charge down to rest is in the order of a second. We investigate the dependence of the cooling time on the number of ions and electrons, and their charge and mass.

PhysicsNuclear and High Energy PhysicsKryptonchemistry.chemical_elementElectronPenning trapEffective nuclear chargelaw.inventionIonPositronchemistrylawLaser coolingPhysics::Atomic PhysicsAtomic physicsInstrumentationElectron coolingNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
researchProduct

Mass Measurement on the rp-Process Waiting Point 72Kr

2004

The mass of one of the three major waiting points in the astrophysical rp process $^{72}$Kr was measured for the first time with the Penning trap mass spectrometer ISOLTRAP. The measurement yielded a relative mass uncertainty of $\deltam/m = 1.2\times 10–7 (\deltam$ = 8 keV). $^{73,74}$Kr, also needed for astrophysical calculations, were measured with more than 1 order of magnitude improved accuracy. We use the ISOLTRAP masses of $^{72–74}$Kr to reanalyze the role of $^{72}$Kr (T$_{1/2}$ = 17.2 s) in the rp process during x-ray bursts and conclude that $^{72}$Kr is a strong waiting point delaying the burst duration with at least 80\% of its $\beta$-decay half-life.

PhysicsNuclear and High Energy PhysicsLarge Hadron Collider26.30.+k 21.10.Dr 27.50.+e 32.10.Bi010308 nuclear & particles physicsHadronrp-process[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometryPenning trap01 natural sciencesISOLTRAPnuclei with mass number 59 to 89particle trapsNuclear physicsnuclear massNucleosynthesis0103 physical sciencesNuclear fusionNuclear Physics - Experimentnucleon-nucleus reactions010306 general physicsNuclear Experimentbeta-decayNuclear Physics
researchProduct

QECvalues of the superallowedβemittersC10,Ar34,Ca38, andV46

2011

The ${Q}_{\mathrm{EC}}$ values of the superallowed ${\ensuremath{\beta}}^{+}$ emitters $^{10}\mathrm{C}$, $^{34}\mathrm{Ar}$, $^{38}\mathrm{Ca}$, and $^{46}\mathrm{V}$ have been measured with the JYFLTRAP Penning-trap mass spectrometer to be 3648.12(8), 6061.83(8), 6612.12(7), and 7052.44(10) keV, respectively. All four values are substantially improved in precision over previous results. Of the well-known superallowed emitters, only $^{14}\mathrm{O}$ has yet to have had its ${Q}_{\mathrm{EC}}$ value measured with a Penning trap.

PhysicsNuclear and High Energy PhysicsLight nucleusQ valueIsotopes of vanadiumAtomic physicsNuclear ExperimentPenning trapEnergy (signal processing)Physical Review C
researchProduct

TRIGA-SPEC: A setup for mass spectrometry and laser spectroscopy at the research reactor TRIGA Mainz

2008

The research reactor TRIGA Mainz is an ideal facility to provide neutron-rich nuclides with production rates sufficiently large for mass spectrometric and laser spectroscopic studies. Within the TRIGA-SPEC project, a Penning trap as well as a beam line for collinear laser spectroscopy are being installed. Several new developments will ensure high sensitivity of the trap setup enabling mass measurements even on a single ion. Besides neutron-rich fission products produced in the reactor, also heavy nuclides such as 235-U or 252-Cf can be investigated for the first time with an off-line ion source. The data provided by the mass measurements will be of interest for astrophysical calculations on…

PhysicsNuclear and High Energy PhysicsNuclear TheoryFOS: Physical sciencesNuclear reactorPenning trapMass spectrometryIon sourcelaw.inventionTRIGANuclear physicsBeamlinelawResearch reactorNuclideNuclear Experiment (nucl-ex)Nuclear ExperimentInstrumentationNuclear Experiment
researchProduct

Density and geometry of single component plasmas

2007

Abstract The density and geometry of p ¯ and e + plasmas in realistic trapping potentials are required to understand and optimize antihydrogen ( H ¯ ) formation. An aperture method and a quadrupole oscillation frequency method for characterizing such plasmas are compared for the first time, using electrons in a cylindrical Penning trap. Both methods are used in a way that makes it unnecessary to assume that the plasmas are spheroidal, and it is shown that they are not. Good agreement between the two methods illustrates the possibility to accurately determine plasma densities and geometries within non-idealized, realistic trapping potentials.

PhysicsNuclear and High Energy PhysicsOscillationGeometryPlasmaTrappingElectronPenning trapPhysics::Plasma PhysicsUpper hybrid oscillationQuadrupolePhysics::Atomic PhysicsAtomic physicsDetectors and Experimental TechniquesAntihydrogen
researchProduct

Q values of the 76Ge and 100Mo double-beta decays

2008

Abstract Penning trap measurements using mixed beams of 76Ge–76Se and 100Mo–100Ru have been utilized to determine the double-beta decay Q-values of 76Ge and 100Mo with uncertainties less than 200 eV. The value for 76Ge, 2039.04(16) keV is in agreement with the published SMILETRAP value, 2039.006(50) keV. The new value for 100Mo, 3034.40(17) keV is 30 times more precise than the previous literature value, sufficient for the ongoing neutrinoless double-beta decay searches in 100Mo. Moreover, the precise Q-value is used to calculate the phase-space integrals and the experimental nuclear matrix element of double-beta decay.

PhysicsNuclear and High Energy PhysicsParticle physicsDecay schemeQ valuePenning trapDouble-beta decayPenning trapQ-valueBeta decayPhase-space integralNuclear physicsNeutrino massPhase spaceDouble beta decayBeta (plasma physics)Value (mathematics)Physics Letters B
researchProduct

Accelerated radioactive beams from REX-ISOLDE

2003

In 2001 the linear accelerator of the Radioactive beam EXperiment (REX-ISOLDE) delivered for the first time accelerated radioactive ion beams, at a beam energy of 2 MeV/u. REX-ISOLDE uses the method of charge-state breeding, in order to enhance the charge state of the ions before injection into the LINAC. Radioactive singly-charged ions from the on-line mass separator ISOLDE are first accumulated in a Penning trap, then charge bred to an A/q < 4.5 in an electron beam ion source (EBIS) and finally accelerated in a LINAC from 5 keV/u to energies between 0.8 and 2.2 MeV/u. Dedicated measurements with REXTRAP, the transfer line and the EBIS have been carried out in conjunction with the first co…

PhysicsNuclear and High Energy PhysicsPhysics::Instrumentation and DetectorsDetectorPenning trapParticle detectorIon sourceLinear particle acceleratorSemiconductor detectorNuclear physicsPhysics::Accelerator PhysicsNeutronAtomic physicsNuclear ExperimentInstrumentationBeam (structure)
researchProduct

Masses of neutron-rich Ni and Cu isotopes and the shell closure at Z = 28 , N = 40

2007

The Penning trap mass spectrometer JYFLTRAP, coupled to the Ion Guide Isotope Separator On-Line (IGISOL) facility at Jyvaskyla, was employed to measure the atomic masses of neutron-rich 70-73Ni and 73, 75Cu isotopes with a typical accuracy less than 5keV. The mass of 73Ni was measured for the first time. Comparisons with the previous data are discussed. Two-neutron separation energies show a weak subshell closure at 68 28Ni40 . A well established proton shell gap is observed at Z = 28 .

PhysicsNuclear and High Energy PhysicsProtonIsotopePenning trapMass spectrometryAtomic massIonNuclear physicsNuclear fusionNeutronPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentThe European Physical Journal A
researchProduct

Direct mass measurements of the heaviest elements with Penning traps

2013

Abstract Penning-trap mass spectrometry (PTMS) is a mature technique to provide atomic masses with highest precision. Applied to radionuclides it enables us to investigate their nuclear structure via binding energies and derived quantities such as nucleon separation energies. Recent progress in slowing down radioactive ion beams in buffer gas cells in combination with advanced ion-manipulation techniques has opened the door to access even the elements above fermium by PTMS. Such elements are produced in complete fusion–evaporation reactions of heavy ions with lead, bismuth, and actinide targets at very low rates. Pioneering high-precision mass measurements of nobelium and lawrencium isotope…

PhysicsNuclear and High Energy PhysicsRadionuclideChemistryFermiumNuclear TheoryNuclear structurechemistry.chemical_elementActinideSuperheavy ElementsCondensed Matter PhysicsPenning trapMass spectrometryAtomic massNuclear physicsNobeliumNuclidePhysical and Theoretical ChemistryAtomic physicsNuclear ExperimentNucleonInstrumentationSpectroscopySpontaneous fissionLawrenciumInternational Journal of Mass Spectrometry
researchProduct