Search results for "Dye laser"

showing 10 items of 63 documents

Determination of trace elements by resonant ionization mass spectrometry (RIMS)

1988

A resonant ionization mass spectrometer has been developed as an analytical tool for the detection of trace elements, especially of plutonium and other radionuclides. The sample, deposited on a rhenium filament, is evaporated by electrical heating and the atoms of the element under investigation are selectively ionized by laser light delivered from three dye lasers pumped by a copper vapour laser. The resulting photoions are detected in a time-of-flight spectrometer with a channelplate detector. For plutonium a mass resolution of M/δM=1500 was obtained and an overall detection efficiency of 4×10−6 was determined for stepwise excitation and ionization via autoionizing states. With a laser li…

Dye laserSpectrometerPhysics::Instrumentation and DetectorsChemistryClinical BiochemistryAnalytical chemistryGeneral MedicineThermal ionization mass spectrometryMass spectrometryBiochemistryAnalytical ChemistryIonizationGeneral Materials SciencePhysics::Atomic PhysicsAtomic vapor laser isotope separationHyperfine structureHybrid mass spectrometerFresenius Zeitschrift f�r Analytische Chemie
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High-resolution non-linear Raman spectroscopy in gases

1990

The resolution in the Raman spectra of gases has been greatly improved by the development of the different methods of non-linear Raman scattering. When two laser beams, one of which has a tunable frequency, are focused in a sample, a stimulated Raman process occurs as soon as the frequency difference between the two lasers is equal to a Raman-active rovibrational or rotational transition frequency. The Raman resonance can be detected in different ways: by coherent anti-Stokes Raman scattering (CARS) or the corresponding Stokes process (CSRS), by a gain in one of the beams (stimulated Raman gain spectroscopy, SRGS) or a loss in the other (inverse Raman spectroscopy, IRS), or even by detectio…

Dye laserbusiness.industryChemistryPhysics::OpticsLaserlaw.inventionsymbols.namesakeOpticsRaman coolingX-ray Raman scatteringlawsymbolsGeneral Materials SciencePhysics::Atomic PhysicsCoherent anti-Stokes Raman spectroscopyAtomic physicsbusinessSpectroscopyRaman spectroscopySpectroscopyRaman scatteringJournal of Raman Spectroscopy
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Iodine hyperfine structure and absolute frequency measurements at 565, 576, and 585nm

2006

Abstract The hyperfine structure splittings of the P(10)14-1, R(15)14-1, and R(99)15-1 transitions at 585 nm, P(62)17-1 at 576 nm, and P(80)21-1 at 565 nm in 127 I 2 are measured by heterodyne spectroscopy using two dye lasers. In addition, the absolute frequencies of the hyperfine components P(10)14-1 a 15 and P(80)21-1 a 10 are determined using a self-referenced frequency comb. These frequencies are used in an experiment testing relativistic time dilation by laser spectroscopy on a fast ion beam.

HeterodyneDye laserMaterials scienceIon beambusiness.industryAbsolute frequencychemistry.chemical_elementIodineAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsFrequency combOpticschemistryElectrical and Electronic EngineeringPhysical and Theoretical ChemistrySpectroscopybusinessHyperfine structureOptics Communications
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Isotope shift and hyperfine structure of stable platinum isotopes

1987

Isotope shift (IS) and hyperfine structure (hfs) measurements have been performed on seven lines of the platinum I spectrum with interference as well as laser fluorescence spectroscopy. In the latter case a frequency-doubled single-mode cw dye laser was applied. The IS of190Pt with a natural abundance of only 0.01% was determined to beδν 190, 192=−38.65(8) mK in theλ306.47 nm transition. The IS parameters and the effective hfs integrals in the configuration (5d+6s)10 were determined in intermediate coupling by a least squares fit of the IS and hfs data with eigenvectors obtained from the platinum fine structure (fs). The results are compared with theoretical values and yield improvedδ〈r 2〉 …

Materials scienceDye laserIsotopeAnalytical chemistrychemistry.chemical_elementElectronic structureAtomic and Molecular Physics and OpticsMolecular electronic transitionNuclear magnetic resonancechemistryKinetic isotope effectNuclear Physics - ExperimentSpectroscopyPlatinumHyperfine structure
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A high-temperature laser ion source for trace analysis and other applications

1990

We report here on the development of a high-temperature laser ion source useful for trace analysis and other applications. It consists of a high temperature ionization chamber, three tunable dye lasers pumped by copper vapor lasers for stepwise resonant ionization and a Mattauch-Herzog mass spectrometer for the analysis of photo-ions. The principle of the laser ion source and its theoretical efficiency are discussed, where the efficiency of a laser ion source is the ratio of photo-ions extracted out to the number of atoms introduced into the cavity. Experimentally, an efficiency of 2×10−3 has been achieved for technetium. The scheme of gated detection is described which is used for suppress…

Materials scienceDye laserPhysics and Astronomy (miscellaneous)General EngineeringPhysics::OpticsGeneral Physics and AstronomyLaser pumpingPhotoionizationMass spectrometryLaserIon sourceIonlaw.inventionlawIonizationPhysics::Atomic PhysicsAtomic physicsApplied Physics B Photophysics and Laser Chemistry
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Frequency tripling for resonance ionization spectroscopy (RIS) of Cd

1998

To explore the nucleosynthesis of heavy elements in the rapid neutron-capture process, investigations on short- lived, very neutron-rich Cd isotopes are planned that require pure samples. These will be produced at the CERN-ISOLDE on-line mass separator in combination with a chemically se- lective laser ion source. The excitation scheme for resonance ionization of Cd was tested in Mainz with a copper-vapor- pumped dye laser system. Due to the high ionization potential of Cd, frequency tripling was required for the first excita- tion step.1D 228: 8n m/. Laser light with an average power of 2m Wwas obtained after frequency tripling and was suc- cessfully used for RIS test measurements on cadmi…

Materials scienceDye laserPhysics and Astronomy (miscellaneous)IsotopeGeneral EngineeringAnalytical chemistryGeneral Physics and AstronomyMass spectrometryLaserIon sourcelaw.inventionNuclear magnetic resonancelawIonization energyNuclear ExperimentSpectroscopyExcitationApplied Physics B: Lasers and Optics
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High-power pulsed dye laser with Fourier-limited bandwidth

1986

A high-peak-power, narrow-linewidth light source with a homogeneous beam profile has been constructed by modifications to a commercially available pulsed-dye-laser system. Output pulses of up to 10 mJ were generated with linewidths of about 50 MHz for 12-nsec pulses. The pulse-to-pulse frequency stability was better than the linewidth, and the center frequency could be scanned over a frequency range of 142.5 GHz at a wavelength of 600 nm. The performance of the system was demonstrated by observing the 6s2 1S0–6s7s1S0 transition in atomic mercury at 2λ = 312.8 nm and the 6s2S1/2–8s2S1/2 transition in atomic gold at 2λ = 308.9 nm using up to 1 mJ of frequency-doubled output for two-photon non…

Materials scienceDye laserbusiness.industryStatistical and Nonlinear PhysicsLaserAtomic and Molecular Physics and Opticslaw.inventionLaser linewidthWavelengthOpticslawExcited stateOptoelectronicsDetectors and Experimental TechniquesCenter frequencySpectroscopybusinessHyperfine structureJournal of the Optical Society of America B
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Microchip Random Laser based on a disordered TiO2-nanomembranes arrangement

2012

International audience; We developed a new scheme for obtaining coherent random lasing based on a chip consisting of a polymer film doped with Rhodamine 6G, having as scatterers butterfly-like TiO2 nanomembranes (TiO2-NM) supported on a glass substrate. The feedback mechanism for laser action is due to the multiple scattering of light by TiO2-NM rather than provided by localized variations of the refractive index in the polymer film. The above-threshold multiple spikes signature indicative of random laser emission with coherent feedback is confirmed. As nanomembranes are foreseen as new MEMS/NEMS building blocks, a new generation of combined active/passive photonic devices can be envisaged.

Materials sciencePhysics::Optics02 engineering and technology01 natural sciencesLight scatteringlaw.inventionRhodamine 6Gchemistry.chemical_compoundCondensed Matter::Materials ScienceOpticslaw0103 physical sciencesSCATTERING010306 general physicsDye laserRandom laserbusiness.industry021001 nanoscience & nanotechnologyLaserAtomic and Molecular Physics and OpticschemistryOptoelectronicsPhotonics0210 nano-technologybusinessRefractive indexLasing threshold
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Performance of a high repetition pulse rate laser system for in-gas-jet laser ionization studies with the Leuven laser ion source @ LISOL

2012

The Leuven Isotope Separator On-Line (LISOL) facility at the Cyclotron Research Center (CRC) Louvain-la-Neuve; The laser ionization efficiency of the Leuven gas cell-based laser ion source was investigated under on- and off-line conditions using two distinctly different laser setups: a low-repetition rate dye laser system and a high-repetition rate Ti:sapphire laser system. A systematic study of the ion signal dependence on repetition rate and laser pulse energy was performed in off-line tests using stable cobalt and copper isotopes. These studies also included in-gas-jet laser spectroscopy measurements on the hyperfine structure of 63Cu. A final run under on-line conditions in which the ra…

Nuclear and High Energy PhysicsActive laser medium29.25.Ni 29.25.Rm 41.85.ArPhysics::OpticsLaser pumping[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesAtmospheric-pressure laser ionizationlaw.inventionlaw0103 physical sciencesUltrafast laser spectroscopyddc:530[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Physics::Atomic Physics010306 general physicsInstrumentationDye laserta114010308 nuclear & particles physicsChemistryLaserIon sourceAtomic physicsAtomic vapor laser isotope separationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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First observation of a resonance ionization signal on242mAm fission isomers

1992

The feasibility of a hyperfine spectroscopy on242mAm fission isomers has been demonstrated at the low target production rate of 10/s. The experimental method employed is based on resonance ionization spectroscopy in a buffer gas cell with detection of the ionization process by means of the fission decay of the isomers. The resonance ionization has been performed in two steps, utilizing an excimer dye laser combination with a repetition rate of 300 Hz. The first resonant step proceeds through theJ=7/2 term at 21440.35 cm−1, which has been excited with the tuncable dye laser beam of a wavelength of 466.28 nm, the second non-resonant step is achieved with the 351 nm radiation of the excimer la…

Nuclear and High Energy PhysicsDye laserExcimer laserChemistrymedicine.medical_treatmentAnalytical chemistryPhysics::OpticsResonancePhotoionizationCondensed Matter PhysicsAtomic and Molecular Physics and OpticsAtmospheric-pressure laser ionizationIonizationPhysics::Atomic and Molecular ClustersmedicinePhysics::Atomic PhysicsPhysical and Theoretical ChemistryAtomic physicsSpectroscopyHyperfine structureHyperfine Interactions
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