Search results for "RESONANCE IONIZATION"

showing 10 items of 51 documents

Optimising the Collinear Resonance Ionisation Spectroscopy (CRIS) experiment at CERN-ISOLDE

2020

© 2019 The CRIS experiment at CERN-ISOLDE is a dedicated laser spectroscopy setup for high-resolution hyperfine structure measurements of nuclear observables of exotic isotopes. Between 2015 and 2018 developments have been made to improve the background suppression, laser-atom overlap and automation of the beamline. Furthermore, a new ion source setup has been developed for offline studies. Here we present the latest technical developments and future perspectives for the experiment. ispartof: Nuclear Instruments & Methods In Physics Research Section B-Beam Interactions With Materials And Atoms vol:463 pages:384-389 ispartof: location:SWITZERLAND, CERN, Geneva status: published

Nuclear and High Energy Physicshyperfine structuretutkimuslaitteetspektroskopiaCERN-ISOLDEhigh-resolution7. Clean energy01 natural sciencesNuclear physicsCRISIonization0103 physical sciencesDalton Nuclear InstitutePhysics::Atomic PhysicsNuclear Experiment010306 general physicsSpectroscopyInstrumentationHyperfine structurePhysicsLarge Hadron Collider010308 nuclear & particles physicsResonanceIon sourceResearchInstitutes_Networks_Beacons/dalton_nuclear_instituteBeamlineBackground suppressionlaser spectroscopycollinear resonance ionization spectroscopyPhysics::Accelerator PhysicsydinfysiikkaNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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First Offline Results from the S3 Low-Energy Branch

2022

International audience; We present the first results obtained from the S3 Low-Energy Branch , the gas cell setup at SPIRAL2-GANIL, which will be installed behind the S3 spectrometer for atomic and nuclear spectroscopy studies of exotic nuclei. The installation is currently being commissioned offline, with the aim to establish optimum conditions for the operation of the radio frequency quadrupole ion guides, mass separation and ion bunching, providing high-efficiency and low-energy spatial spread for the isotopes of interest. Transmission and mass-resolving power measurements are presented for the different components of the S3-LEB setup. In addition, a single-longitudinal-mode, injection-lo…

Nuclear and High Energy Physicsresonance ionization laser spectroscopy; gas cell; hypersonic gas jets; radio frequency quadrupoles; nuclear ground state properties; isotope shift; hyperfine structurehyperfine structurespektroskopiatutkimuslaitteet[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Physics Atomic Molecular & Chemicalatomifysiikka[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]radio frequency quadrupolesScience & TechnologySPECTROSCOPY[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Physicsgas cellLASER ION-SOURCECondensed Matter PhysicslasertekniikkaAtomic and Molecular Physics and Opticsresonance ionization laser spectroscopyisotope shiftnuclear ground state propertiesPhysical Scienceshypersonic gas jetsIONIZATIONydinfysiikkaSYSTEMAtoms
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The laser and optical system for the RIBF-PALIS experiment

2017

Abstract This paper describes the laser and optical system for the Parasitic radioactive isotope (RI) beam production by Laser Ion-Source (PALIS) in the RIKEN fragment separator facility. This system requires an optical path length of 70 m for transporting the laser beam from the laser light source to the place for resonance ionization. To accomplish this, we designed and implemented a simple optical system consisting of several mirrors equipped with compact stepping motor actuators, lenses, beam spot screens and network cameras. The system enables multi-step laser resonance ionization in the gas cell and gas jet via overlap with a diameter of a few millimeters, between the laser photons an…

Nuclear and High Energy PhysicsspektroskopiaPhysics::Optics01 natural sciencesBeam parameter productlaw.inventionVertical-cavity surface-emitting laserLaser linewidthOpticslaw0103 physical sciencesPhysics::Atomic PhysicsLaser power scaling010306 general physicsInstrumentationPhysicsDistributed feedback laserta114010308 nuclear & particles physicsbusiness.industryFar-infrared lasergas cellLaserlasertekniikkaLaser Ion Sourcegas jetlaser spectroscopyPhysics::Accelerator PhysicsLaser beam qualitylaser resonance ionizationbusinessydinfysiikkaNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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β-delayed fission andαdecay ofAt196

2016

A nuclear-decay spectroscopy study of the neutron-deficient isotope $^{196}\mathrm{At}$ is reported where an isotopically pure beam was produced using the selective Resonance Ionization Laser Ion Source and On-Line Isotope Mass Separator (CERN). The fine-structure $\ensuremath{\alpha}$ decay of $^{196}\mathrm{At}$ allowed the low-energy excited states in the daughter nucleus $^{192}\mathrm{Bi}$ to be investigated. A $\ensuremath{\beta}$-delayed fission study of $^{196}\mathrm{At}$ was also performed. A mixture of symmetric and asymmetric fission-fragment mass distributions of the daughter isotope $^{196}\mathrm{Po}$ (populated by $\ensuremath{\beta}$ decay of $^{196}\mathrm{At}$) was deduce…

PhysicsCold fissionDecay schemeCluster decay010308 nuclear & particles physicsFission01 natural sciencesExcited state0103 physical sciencesResonance ionizationDecay productAtomic physicsNuclear Experiment010306 general physicsSpectroscopyPhysical Review C
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Determination of the ground-state hyperfine structure in neutral229Th

2012

The ground-state hyperfine structure of neutral 229Th has been measured for the first time using high-resolution resonance ionization spectroscopy. The measurements were performed as a preparatory work aimed at the identification of the predicted low-lying 7.6 eV isomer in 229Th through an investigation of its hyperfine structure. The hyperfine coupling constants have been extracted for the atomic ground state as well as for three excited states at 26 096, 26 113 and 38 278 cm−1. Due to rather small splittings not all hyperfine components were completely resolved and therefore an extensive χ2-error analysis was performed to achieve reliable results. The ground-state transition to the excite…

PhysicsHyperfine couplingExcited stateResonance ionizationPhysics::Atomic PhysicsAtomic physicsCondensed Matter PhysicsSpectroscopyGround stateHyperfine structureAtomic and Molecular Physics and OpticsJournal of Physics B: Atomic, Molecular and Optical Physics
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Combined high-resolution laser spectroscopy and nuclear decay spectroscopy for the study of the low-lying states inFr206,At202, andBi198

2016

High-resolution laser spectroscopy was performed on $^{206}\mathrm{Fr}$ with the collinear resonance ionization spectroscopy (CRIS) experiment at CERN-ISOLDE. The hyperfine structure and isotope shift of the ground, first isomeric and second isomeric states were measured. The hyperfine components were unambiguously assigned to each nuclear state by means of laser-assisted nuclear decay spectroscopy. The branching ratios in the $\ensuremath{\alpha}$ decay of $^{206}\mathrm{Fr}$ and $^{202}\mathrm{At}$ were also measured for the first time with isomerically purified beams. The extracted hindrance factors allow determination of the spin of the ground, first isomeric, and second isomeric states…

PhysicsIsotope010308 nuclear & particles physicsNuclear stateHigh resolutionchemistry.chemical_element01 natural sciences7. Clean energyFranciumNuclear physicschemistry0103 physical sciencesResonance ionizationPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsAtomic physicsNuclear Experiment010306 general physicsSpectroscopyHyperfine structureRadioactive decayPhysical Review C
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Isotope Shift Measurements for Superdeformed Fission Isomeric States

1998

Optical isotope shift measurements have been performed for the ${}^{240,242}{\mathrm{Am}}^{f}$ fission isomers with low target production rates of $10{\mathrm{s}}^{\ensuremath{-}1}$ employing resonance ionization spectroscopy in a buffer gas cell. Isotope shift ratios ${\mathrm{IS}}^{240f,241}/{\mathrm{IS}}^{243,241}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}39.2(8)$ and ${\mathrm{IS}}^{242f,241}/{\mathrm{IS}}^{243,241}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}41.4(8)$ have been measured at the 500.02 nm transition. A difference in the nuclear mean charge radii $\ensuremath{\delta}〈{r}^{2}{〉}_{\mathrm{opt}}^{242f,241}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}5.34(2…

PhysicsIsotopeFissionResonance ionizationQuadrupoleGeneral Physics and AstronomyCharge (physics)Production (computer science)Atomic physicsPhysical Review Letters
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Counting IndividualCa41Atoms with a Magneto-Optical Trap

2004

Atom trap trace analysis, a novel method based upon laser trapping and cooling, is used to count individual atoms of $^{41}\mathrm{Ca}$ present in biomedical samples with isotopic abundance levels between ${10}^{\ensuremath{-}8}$ and ${10}^{\ensuremath{-}10}$. The method is calibrated against resonance ionization mass spectrometry, demonstrating good agreement between the two methods. The present system has a counting efficiency of $2\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}7}$. Within 1 h of observation time, its $3\mathrm{\text{\ensuremath{-}}}\ensuremath{\sigma}$ detection limit on the isotopic abundance of $^{41}\mathrm{Ca}$ reaches $4.5\ifmmode\times\else\texttimes\fi{}{10…

PhysicsLaser trappingObservation timeMagneto-optical trapAtomResonance ionizationGeneral Physics and AstronomyNatural abundanceTrace analysisAtomic physicsPhysical Review Letters
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Nuclear Moments and Deformation Change inA184ug,mfrom Laser Spectroscopy

1997

Resonance ionization spectroscopy (RIS) was performed on desorbed Au, and the complete hyperfine spectrum of both isomeric and ground states of the short lived 184Au nucleus has been recorded from the 5d106s S1y2 ! 5d106p P3y2 optical transition. The nuclear moments of both states and the mean square charge radius changes were measured. The magnetic moments were determined to be m 184g I­5 ­ 12.07s2dmN and m I­2 ­ 11.44s2dmN and the spectroscopic quadrupole moments to be Q 184g s ­ 14.65s26db and Q184m s ­ 11.90s16d b. A difference in the mean square charge radius dkr2 c l184g,184m ­ 20.036s3d fm2 was found. [S0031-9007(97)03992-6]

PhysicsMagnetic momentCharge radiusOptical transitionQuadrupoleResonance ionizationGeneral Physics and AstronomyDeformation (engineering)Atomic physicsSpectroscopyHyperfine structurePhysical Review Letters
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Observation of strongly deformed ground-state configurations in $^{184}$Au and $^{183}$Au by laser spectroscopy

1988

Resonance ionization mass spectroscopy (RIMS) and pulsed-laser induced desorption (PLID) have been combined in order to study the isotope shift (IS) and hyperfine structure (HFS) of184Au (T1/2=53 s) and183Au (T1/2=42 s) in the 6s2S1/2 → 6p2P1/2 (λ=267 nm) transition. The Au isotopes were obtained as daughters in the decay of184,183Hg produced and mass separated at the new ISOLDE-3 facility at CERN. It was found that the strong deformationβ2}-0.25 setting in at186Au persists down to183Au.

PhysicsNuclear and High Energy PhysicsIsotopeDesorptionResonance ionizationNuclear fusionNuclear Physics - ExperimentAtomic physicsMass spectrometryGround stateSpectroscopyHyperfine structure
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