Search results for "Mass analyzer"

showing 10 items of 24 documents

A compact apparatus for mass selective resonance ionization spectroscopy in a buffer gas cell

1997

Abstract An ultra-sensitive laser spectroscopic method for the investigation of transuranium nuclides has been developed based on resonance ionization in an argon buffer gas cell. This method has been combined with ion-guide extraction and mass selective direct detection of the resonantly ionized atoms. Using argon as a buffer gas, recoils of fusion reactions can be thermalized even at low pressure. The differential pumping system consists of only one roots pump and two turbo molecular pumps. The set-up has been tested with 243 Am evaporated from a filament located inside the optical gas cell. Resonance ionization is performed using a two-step excitation with an excimer-dye-laser combinatio…

Nuclear and High Energy PhysicsArgonBuffer gasAnalytical chemistrychemistry.chemical_elementMass spectrometryIon sourceAtmospheric-pressure laser ionizationchemistryIonizationAtomic physicsInstrumentationQuadrupole mass analyzerElectron ionizationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Quadrupole interaction of $^{8}$Li and $^{9}$Li in LiNbO$_{3}$ and the quadrupole moment of $^{9}$Li

1988

The quadrupole interaction of nuclear spin polarized8Li (I=2) and9Li (I=3/2) in LiNbO3 has been studied at room temperature. The polarization was achieved by optical pumping of a fast atomic beam with circularly polarized laser light. The atoms were implanted into a hexagonal LiNbO3 single crystal and the quadrupole splitting ofβ-NMR spectra was measured. A ratio of ¦Q(9Li)/Q(8Li)¦=0.88(4) for the nuclear quadrupole moments was deduced, yielding a new value of ¦Q(9Li)¦=25.3 (9) mb for the quadrupole moment of9Li.

Nuclear and High Energy PhysicsChemistryIsotopes of lithiumNuclear TheoryPhysics::OpticsQuadrupole splittingSpectral lineOptical pumpingQuadrupolePhysics::Accelerator PhysicsNuclear fusionNuclear Physics - ExperimentPhysics::Atomic PhysicsAtomic physicsQuadrupole mass analyzerSingle crystal
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Ramsey technique applied in a Penning trap mass spectrometer

1991

Abstract The Ramsey method has been applied in an experiment aiming for accurate mass determination of unstable isotopes. The ion motion in a Penning trap has been excited with time-separated oscillatory fields and Ramsey fringes were observed in the case of dipole and quadrupole excitation. The experimental resonances are in good agreement with theory. Further applications of the technique are discussed.

Nuclear and High Energy PhysicsChemistryMass spectrometryPenning trapDipoleQuadrupolePhysics::Atomic PhysicsIon trapDetectors and Experimental TechniquesAtomic physicsQuadrupole ion trapInstrumentationQuadrupole mass analyzerHybrid mass spectrometerNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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The squeezer ion guide

1992

Abstract The properties of an ordinary ion guide can be improved by inserting a grid between the nozzle and the skimmer. When positive ions are transported, an electric potential lower than +10 V is connected to the grid and one of the order of − 10 V to the skimmer. Efficient focusing is achieved between the nozzle and the grid by a combined action of the viscous helium flow field and the weak electric field. The focusing device is called a “squeezer”. It can be extended by adding more grids, a second skimmer, and differential pumping. Contrary to the first grid, the additional elements act more or less like electrostatic lenses in medium vacuum. With the squeezer ion guide, ions created i…

Nuclear and High Energy PhysicsChemistryNozzleUltra-high vacuumSkimmer (machine)Electric potentialAtomic physicsInstrumentationQuadrupole mass analyzerElectrostatic lensIonElectric discharge in gasesNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Proton decay of 108I and its significance for the termination of the astrophysical rp-process

2019

Abstract Employing the Argonne Fragment Mass Analyzer and the implantation-decay-decay correlation technique, a weak 0.50(21)% proton decay branch was identified in 108I for the first time. The 108I proton-decay width is consistent with a hindered l = 2 emission, suggesting a d 5 2 origin. Using the extracted 108I proton-decay Q value of 597(13) keV, and the Q α values of the 108I and 107Te isotopes, a proton-decay Q value of 510(20) keV for 104Sb was deduced. Similarly to the 112,113Cs proton-emitter pair, the Q p ( I 108 ) value is lower than that for the less-exotic neighbor 109I, possibly due to enhanced proton-neutron interactions in N ≈ Z nuclei. In contrast, the present Q p ( Sb 104 …

Nuclear and High Energy Physicsalpha decayProton decayQ valueastrofysiikkaNuclear Theory104Sb01 natural sciencesastrophysical rp process108I0103 physical sciencesMass analyzer107Te010306 general physicsNuclear ExperimentPhysicsIsotopeta114010308 nuclear & particles physicsInteraction energyrp-processlcsh:QC1-999proton decayHigh Energy Physics::ExperimentAtomic physicsydinfysiikkalcsh:PhysicsPhysics Letters B
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Selective ultra trace isotope determination in environmental and biomedical studies by high-resolution resonance ionization mass spectrometry

2002

The precise determination of relative abundances of ultra trace isotopes in the range below 10 -9 is of importance for a wide spectrum of applications in fields like environmental protection, cosmo-chemistry, bio-medical tracer studies or geological and geo-chronological investigations. The necessary high isotopic selectivity, rather complete isobaric suppression and good overall efficiency for these investigations is provided by high-resolution resonance ionization mass spectrometry. Multi-step continuous wave laser excitation and ionization using diode lasers at a compact quadrupole mass spectrometer has been optimized to become a powerful and reliable experimental method, which is just b…

Nuclear magnetic resonanceSpectrometerIsotopelawIonizationAnalytical chemistryPhysics::Atomic PhysicsThermal ionization mass spectrometryMass spectrometryLaserQuadrupole mass analyzerAccelerator mass spectrometrylaw.inventionSPIE Proceedings
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Penning-trap mass measurements of neutron-deficient Rb and Sr isotopes

1993

Abstract The Penning-trap mass spectrometer ISOLTRAP installed at the on-line mass separator ISOLDE 2 at CERN has been used for mass determination of 75–87 Rb and 78–83,87 Sr. Ions are captured in a Penning trap and their cyclotron frequency ω c = ( q m )B in the trapping field B is measured. Ratios of these frequencies lead to the determination of the atomic mass of these isotopes. A resolving power of typically m Δm = 10 6 and an accuracy of δm ≈10 keV is obtained. The mass of 78 Sr is measured for the first time and, in most cases, the mass values of the other isotopes are significantly improved. The experimental masses are compared with theoretical predictions.

PhysicsNuclear and High Energy Physics010308 nuclear & particles physics[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Isotopes of chlorine[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Penning trapMass spectrometry7. Clean energy01 natural sciencesISOLTRAPIsotopes of oxygenAtomic massNuclear physicsMass0103 physical sciencesNuclear Physics - ExperimentAtomic physics010306 general physicsQuadrupole mass analyzer
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Direct mass measurements of neutron-deficient xenon isotopes with the ISOLTRAP mass spectrometer

2000

Abstract The masses of Xe isotopes with 124⩾ A ⩾114 have been measured using the ISOLTRAP spectrometer at the on-line mass separator ISOLDE/CERN. A mass resolving power of 500 000 was chosen resulting in an accuracy of δm ≈12 keV for all isotopes investigated. Conflicts with existing mass data of several standard deviations were found.

PhysicsNuclear and High Energy PhysicsSpectrometer[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Physics::Instrumentation and Detectors010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometry01 natural sciencesISOLTRAPAtomic massIsotopes of oxygenNuclear physics0103 physical sciencesIsotopes of xenonAtomic physicsParticle PhysicsNuclear Experiment010306 general physicsQuadrupole mass analyzerHybrid mass spectrometer
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Mass measurements on neutron-deficient Sr and neutron-rich Sn isotopes with the ISOLTRAP mass spectrometer

2005

Abstract The atomic masses of 76,77,80,81,86,88 Sr and 124,129,130,131,132 Sn were measured by means of the Penning trap mass spectrometer ISOLTRAP at ISOLDE/CERN. 76 Sr is now the heaviest N = Z nucleus for which the mass is measured to a precision better than 35 keV. For the tin isotopes in the close vicinity of the doubly magic nucleus 132 Sn, mass uncertainties below 20 keV were achieved. An atomic mass evaluation was carried out taking other experimental mass values into account by performing a least-squares adjustment. Some discrepancies between older experimental values and the ones reported here emerged and were resolved. The results of the new adjustment and their impact will be pr…

PhysicsNuclear and High Energy Physicsatomic masses010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometryISOLTRAP01 natural sciencesISOLTRAPAtomic massNuclear physicsMasstin0103 physical sciencesIsotopes of tinNeutronstrontiumAtomic physics010306 general physicsNuclear ExperimentQuadrupole mass analyzerhigh-precision mass spectrometryHybrid mass spectrometer07.75.+h 21.10.Dr 32.10.Bi
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Peak shape for a quadrupole mass spectrometer: comparison of computer simulation and experiment

2000

Abstract Computer simulations of ion trajectories have been used to evaluate the performance of a quadrupole mass spectrometer. Consideration has been given to realistic fields modeled on a commercial system as well as experimental distributions with respect to ion entry position, axial and radial velocity and relative phase of the quadrupole field. Determination of the mass filter acceptance-area as a function of the mass setting yields mass peak shapes with a dynamic range of more than seven orders of magnitude and thus provides estimates for abundance sensitivity. Results from these simulations are found to give excellent agreement with experimental measurements for different elements in…

Range (particle radiation)ChemistryDynamic rangeMonte Carlo methodCondensed Matter PhysicsIonRadial velocityOrders of magnitude (time)SubstructurePhysical and Theoretical ChemistryAtomic physicsInstrumentationQuadrupole mass analyzerSpectroscopyInternational Journal of Mass Spectrometry
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