Search results for "BUFFER GAS"

showing 10 items of 47 documents

The MARA-LEB ion transport system

2020

Abstract A low-energy branch is under development for the MARA vacuum-mode recoil separator at the Accelerator Laboratory of the University of Jyvaskyla. This development will allow for the study of proton-rich nuclei through laser ionisation spectroscopy and mass measurements. After stopping and extraction from a buffer gas cell, the ions of interest will be accelerated and transported to dedicated experimental setups by an ion transport system consisting of several focusing, accelerating and mass-separating elements. This article presents the current design and simulations for the ion transport.

Nuclear and High Energy PhysicsMaterials scienceBuffer gasLaser01 natural sciencesRecoil separatorlaw.inventionIonNuclear physicslawIonization0103 physical sciencesCurrent (fluid)Nuclear Experiment010306 general physicsSpectroscopy010303 astronomy & astrophysicsInstrumentationIon transporterNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Controlling diffusion of 3He by buffer gases: a structural contrast agent in lung MRI.

2006

Purpose: To study the influence of admixing inert buffer gases to laser-polarized 3 He in terms of resulting diffusion coefficients and the consequences for image contrast and resolution. Materials and Methods: The diffusion coefficient of 3 He was altered by admixing buffer gases of various molecular weights ( 4 He, N2, and SF6). The influence of the pulse sequence and the diffusion coefficient on the appearance of MRI of (laserpolarized) gases was analyzed by comparison of basic theoretical concepts with demonstrative experiments. Results: Excellent agreement between theoretical description and observed signal in simple gradient echoes was observed. A maximum signal gain can be predicted …

InertMaterials sciencePhantoms ImagingDiffusionPhysics::Medical PhysicsBuffer gasResolution (electron density)Contrast MediaReproducibility of ResultsPulse sequenceImage EnhancementSignalMolecular physicsHeliumSensitivity and SpecificityDiffusion Magnetic Resonance ImagingIsotopesRestricted DiffusionEffective diffusion coefficientHumansRadiology Nuclear Medicine and imagingGasesLungJournal of magnetic resonance imaging : JMRI
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Deconvolution of the spectral line profiles for the plasma temperature estimation

2010

Abstract The Hg 253.7 nm spectral line profiles, emitted from the mercury–argon high-frequency electrodeless discharge lamps (HFEDL) have been measured by means of a high-resolution scanning Fabry–Perrot interferometer at the mercury cold spot temperature value at 20 °C, different discharge current and buffer gas values. The deconvolution procedure by means of the Tikhonov's regularization method was performed to obtain the real spectral line shape. The influence of the instrumental function and absorption, real width of the Hg 253.7 nm resonance line and temperature of the radiating atoms are obtained. The results were compared with the results of the nonlinear multiparameter mathematical …

PhysicsNuclear and High Energy PhysicsGas-discharge lampbusiness.industryBuffer gasPlasmaSpectral lineSpectral line shapelaw.inventionTikhonov regularizationInterferometryOpticslawDeconvolutionbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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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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Production of neutron deficient rare isotope beams at IGISOL; on-line and off-line studies

2004

This article reports on recent on-line yield measurements employing the light-ion and heavy-ion reaction-based ion guide systems and new results on a-recoil ion transport properties in ion guides with and without electric fields. In addition, the presently used ion guide designs for fusion evaporation reactions are introduced. The present study investigated different schemes for ion extraction from the gas cell. The addition of an extra ring electrode between the traditional skimmer electrode and the exit hole led to transmission independent of the primary beam intensity as opposed to strong intensity dependence observed earlier with the plain skimmer only. Furthermore, the mass resolving p…

FUSION-EVAPORATION REACTIONSISOMERNuclear and High Energy PhysicsEFFICIENCYIon beamChemistryHF-171Buffer gasion guideElectronIon gunSTATEon-line isotope separationIonION-GUIDE TECHNIQUEIon beam depositionPhysics::Plasma PhysicsNeutronSEPARATOR ONLINEAtomic physicsLASER SPECTROSCOPYSPIGInstrumentationIon transporterNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Study of optical and magneto processes in Rb atomic vapor layer of nanometric thickness

2012

Using a narrow-band resonant fluorescence spectra from a nano-cell with a thickness of L= [lambda]/2, and VSOP resonances formed at a thickness L =[lambda] ([lambda] is the wavelength of the resonant radiation), for the first time it was experimentally investigated the behaviour of the frequency and intensity (transition probabilities) of the atomic hyperfine structure transitions between the 85Rb, 87Rb, D1 and D2 lines Zeeman sublevels in external magnetic fields in range 5 - 7000G. The behaviour of tens of previously unstudied atomic transitions was analyzed and it is demonstrated that the intensities of these lines can both greatly increase, and decrease (tenfold). For the first time it …

Gaz tamponπ et ơ- polarizations of the laser radiationCoherent Dicke narrowing[PHYS.COND.CM-GEN] Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]High resolution spectroscopyRécissement Dicke cohérentRb hyperfine structureπ et ơ- du rayonnement laserStructure hyperfine RbCellules multi-régions combinéesRésonances VSOPTransitions "interdites''[ PHYS.COND.CM-GEN ] Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]Nano-cellsZeeman effectDiode laserNano-cellulesEffet ZeemanƠ+Polarisations Ơ+"Forbidden'' transitions[PHYS.COND.CM-GEN]Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]Combined multi-region cellsBuffer gasVSOP resonancesSpectroscopie à haute résolution
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Imaging magnetic scalar potentials by laser-induced fluorescence from bright and dark atoms

2014

We present a spectroscopic method for mapping two-dimensional distributions of magnetic field strengths (magnetic scalar potential lines) using charge-coupled device (CCD) recordings of the fluorescence patterns emitted by spin-polarized Cs vapour in a buffer gas exposed to inhomogeneous magnetic fields. The method relies on the position-selective destruction of spin polarization by magnetic resonances induced by multi-component oscillating magnetic fields, such that magnetic potential lines can be directly detected by the CCD camera. We also present a generic algebraic model allowing for the calculation of the fluorescence patterns and find excellent agreement with the experimental observa…

PhysicsAcoustics and UltrasonicsSpin polarizationAtomic Physics (physics.atom-ph)Buffer gasScalar (physics)FOS: Physical sciencesScalar potentialCondensed Matter PhysicsMolecular physicsSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsMagnetic fieldPhysics - Atomic PhysicsMagnetic potentialLaser-induced fluorescenceImage resolution
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B1(1)Π state of KCs: high-resolution spectroscopy and description of low-lying energy levels.

2012

The diode laser induced B(1)(1)Π → X(1)Σ(+) fluorescence spectra of the KCs molecule were recorded by Fourier-transform spectrometer with resolution of 0.03 cm(-1). Buffer gas Ar was used to facilitate appearance of rotation relaxation lines in the spectra, thus enlarging the B(1)(1)Π dataset, allowing one to determine the Λ-splitting constants and to reveal numerous local perturbations. A dataset was systematically obtained for B(1)(1)Π vibrational levels ν(') ∈ [0; 5] nonuniformly covering rotational levels with J(') ∈ [7; 233]. For ν(') ∈ [0; 3], the less-perturbed data of f-components were included in the fit. A pointwise potential energy curve (PEC) based on the inverted perturbation a…

PointwiseSpectrometerChemistryBuffer gasAnalytical chemistryGeneral Physics and AstronomyLaserPotential energySpectral linelaw.inventionAb initio quantum chemistry methodslawPhysical and Theoretical ChemistryAtomic physicsSpectroscopyThe Journal of chemical physics
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High resolution spectroscopy and potential determination of the (3)1Pi state of NaCs.

2006

The (3)(1)Pi state of the NaCs molecule was studied by high resolution Fourier-transform spectroscopy. The (3)(1)Pi--X (1)Sigma(+) laser induced fluorescence was excited by an Ar(+) ion laser or by a single-mode frequency-doubled cw Nd:YAG laser. The presence of argon buffer gas yielded rich rotational relaxation spectra allowing to enlarge the data set for the (3)(1)Pi state term values, as well as to observe Lambda splittings in a wide range of vibrational (v(')) and rotational (J(')) quantum numbers. The data field includes about 820 energy levels of (3)(1)Pi NaCs in the range from v(')=0 to 37 and from J(')=3 to 190, which corresponds to ca. 95% of the potential well depth. Direct fit o…

ChemistryBuffer gasGeneral Physics and AstronomyIon laserQuantum numberLaserPotential energylaw.inventionlawExcited statePhysical and Theoretical ChemistryAtomic physicsLaser-induced fluorescenceSpectroscopyThe Journal of chemical physics
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Lifetime measurements of the 3D3/2 and 3D5/2 metastable states in CaII

1993

The lifetime of the metastable 3D3/2 and 3D5/2 states of Ca+ ions is determined in a r.f. ion trap by laser excitation of this levels and subsequent time delayed probing of the state population by a second laser. In a buffer gas atmosphere of about 10−5−10−6 mbar of He we observe quenching to the ground state and strong finestructure mixing of the two D-states. This mixing allowes only the determination of the combined lifetime. Our result of τ(3D)=1.24(39) s is in good agreement with theoretical calculations.

education.field_of_studyMaterials scienceBuffer gasPopulationLaserAtomic and Molecular Physics and OpticsIonlaw.inventionlawExcited stateMetastabilityIon trapAtomic physicsGround stateeducationZeitschrift f�r Physik D Atoms, Molecules and Clusters
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