Search results for "RAMAN"

showing 10 items of 1328 documents

Comment on: Application of Raman Spectroscopy to Distinguish Metamorphic and Igneous Zircon (Xian et al., Anal. Lett. 2004, v. 37, p. 119)

2005

Abstract We critically discuss a recently proposed technique ((Xian et al. 2004)) used to distinguish igneous (i.e., magmatic) from metamorphic growth of the mineral zircon according to the intensity of the 1461 cm−1 band observed in those author's Raman spectra. The band evaluated by Xian et al. (2004) is actually due to laser‐induced photoluminescence of trace amounts of the trivalent rare earth element Er, which, as an analytical artefact, overlays the Raman spectrum when green Ar+ laser excitation is used. We demonstrate that this band is not a Raman band, and discuss why the intensity of Er3+ luminescence is not uniquely indicative of the geologic origin of a zircon crystal. The techni…

PhotoluminescenceMineralChemistryRare-earth elementBiochemistry (medical)Clinical BiochemistryAnalytical chemistryMineralogyBiochemistryAnalytical ChemistryCrystalsymbols.namesakeIgneous rockElectrochemistrysymbolsRaman spectroscopyLuminescenceSpectroscopyZirconAnalytical Letters
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Influence of the InAs coverage on the phonon-assisted recombination in InAs/GaAs quantum dots

2002

6 páginas, 3 figuras.

PhotoluminescencePhononLight scatteringsymbols.namesakechemistry.chemical_compoundCondensed Matter::Materials ScienceGallium arsenideMaterials ChemistryPhotoluminescenceIndium arsenideCondensed matter physicsCondensed Matter::OtherLight scatteringHeterojunctionSurfaces and InterfacesQuantum effectsCondensed Matter PhysicsCondensed Matter::Mesoscopic Systems and Quantum Hall EffectSurfaces Coatings and FilmschemistryQuantum dotsymbolsIndium arsenideMolecular beam epitaxyRaman scatteringMolecular beam epitaxy
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Roadmap on STIRAP applications

2019

STIRAP (stimulated Raman adiabatic passage) is a powerful laser-based method, usually involving two photons, for efficient and selective transfer of populations between quantum states. A particularly interesting feature is the fact that the coupling between the initial and the final quantum states is via an intermediate state, even though the lifetime of the latter can be much shorter than the interaction time with the laser radiation. Nevertheless, spontaneous emission from the intermediate state is prevented by quantum interference. Maintaining the coherence between the initial and final state throughout the transfer process is crucial. STIRAP was initially developed with applications in …

PhotonAtomic Physics (physics.atom-ph)Digital storageStimulated Raman adiabatic passage02 engineering and technologyStimulated Raman adiabatic passage (STIRAP)01 natural scienceslaw.inventionPhysics - Atomic PhysicsFTIR SPECTROSCOPYstimulated Raman adiabatic passage (STIRAP)lawStereochemistryRare earthsStatistical physicsMetal ionsmolecular Rydberg statesQCparity violationPhysicseducation.field_of_studyQuantum PhysicsElectric dipole momentsCoherent population transfer021001 nanoscience & nanotechnologyCondensed Matter Physicsacoustic waves; molecular Rydberg states; nuclear coherent population transfer; parity violation; spin waves; stimulated Raman adiabatic passage (STIRAP); ultracold moleculesADIABATIC PASSAGEAtomic and Molecular Physics and OpticsChemical DynamicsMolecular beamsVIOLATING ENERGY DIFFERENCEResearch group A. Pálffy – Division C. H. KeitelStimulated emission0210 nano-technologyCoherence (physics)Experimental parametersPopulationFOS: Physical sciencesacoustic waves530spin wavesMolecular Rydberg statesELECTROMAGNETICALLY INDUCED TRANSPARENCYSINGLE PHOTONSQuantum statePhysics - Chemical Physics0103 physical sciencesUltracold moleculesSpontaneous emissionddc:530Nuclear coherent population transfer010306 general physicseducationStimulated Raman adiabatic passageChemical Physics (physics.chem-ph)Rare-earth-ion doped crystalsPhotonsQuantum opticsnuclear coherent population transferBROAD-BANDControlled manipulationsPOLAR-MOLECULESMoleculesRydberg statesLaserSuperconducting quantum circuitAcoustic wavesParity violationstimulated Raman adiabatic passage (STIRAP); ultracold molecules; parity violation; spin waves; acoustic waves; molecular Rydberg states; nuclear coherent population transferDewey Decimal Classification::500 | Naturwissenschaften::530 | Physikultracold moleculesQuantum Physics (quant-ph)QUANTUM GASSpin waves
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Observation and analysis of the SF6 ν2+ν4−ν5 band: Improved parameters for the v5= 1 state

2016

Abstract In this paper, we present the high resolution analysis of the weak ν 2 + ν 4 - ν 5 band of SF6 around 735 cm−1. The spectra were recorded on the AILES Beamline at the SOLEIL Synchrotron facility using a cryogenic multipass cell coupled to a Bruker 125HR spectrometer with a maximum resolution of 0.00102 cm−1. For this band, we worked with 4 mbar of SF6 at a temperature of 223 ± 2  K. The optical path length was fixed to 141 m and the spectrum recorded with 0.001 cm−1 of resolution. A new, cold spectrum of the ν 2 + ν 4 band was also collected at 153 K, 15-m path length, and 0.0015 cm−1 resolution. The analysis was performed by using the Dijon group XTDS and SPVIEW software, based on…

Physics010304 chemical physics010504 meteorology & atmospheric sciencesSpectrometerbusiness.industry01 natural sciencesAtomic and Molecular Physics and OpticsSpectral lineSynchrotronHot bandlaw.inventionsymbols.namesakeOpticsBeamlinePath lengthlaw0103 physical sciencessymbolsPhysical and Theoretical ChemistryAtomic physicsbusinessRaman spectroscopySpectroscopyOptical path length0105 earth and related environmental sciencesJournal of Molecular Spectroscopy
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Rovibrational controlled-NOT gates using optimized stimulated Raman adiabatic passage techniques and optimal control theory

2009

Implementation of quantum controlled-NOT (CNOT) gates in realistic molecular systems is studied using stimulated Raman adiabatic passage (STIRAP) techniques optimized in the time domain by genetic algorithms or coupled with optimal control theory. In the first case, with an adiabatic solution (a series of STIRAP processes) as starting point, we optimize in the time domain different parameters of the pulses to obtain a high fidelity in two realistic cases under consideration. A two-qubit CNOT gate constructed from different assignments in rovibrational states is considered in diatomic (NaCs) or polyatomic $({\text{SCCl}}_{2})$ molecules. The difficulty of encoding logical states in pure rota…

Physics010304 chemical physicsField (physics)Stimulated Raman adiabatic passageRotational–vibrational spectroscopyOptimal control01 natural sciencesAtomic and Molecular Physics and OpticsControlled NOT gateQuantum mechanics0103 physical sciencesPhysics::Atomic and Molecular ClustersTime domain010306 general physicsAdiabatic processQuantum computerPhysical Review A
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Resonant hyper-Raman scattering in spherical quantum dots

1998

A theoretical model of resonant hyper-Raman scattering by an ensemble of spherical semiconductor quantum dots has been developed. The electronic intermediate states are described as Wannier-Mott excitons in the framework of the envelope function approximation. The optical polar vibrational modes of the nanocrystallites (vibrons) and their interaction with the electronic system are analized with the help of a continuum model satisfying both the mechanical and electrostatic matching conditions at the interface. An explicit expression for the hyper-Raman scattering efficiency is derived, which is valid for incident two-photon energy close to the exciton resonances. The dipole selection rules f…

PhysicsAngular momentumCondensed matter physicsCondensed Matter - Mesoscale and Nanoscale PhysicsScatteringCondensed Matter::OtherExcitonFOS: Physical sciencesResonanceCondensed Matter::Mesoscopic Systems and Quantum Hall EffectMolecular physicssymbols.namesakeDipoleCondensed Matter::Materials ScienceTotal angular momentum quantum numberQuantum dotMesoscale and Nanoscale Physics (cond-mat.mes-hall)symbolsRaman scattering
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Dipole soliton solution for the homogeneous high-order nonlinear Schrödinger equation with cubic–quintic–septic non-Kerr terms

2015

Abstract We consider a high-order nonlinear Schrodinger equation with third- and fourth-order dispersions, cubic–quintic–septic nonlinearities, self-steepening, and instantaneous Raman response. This equation models describes ultra-short optical pulse propagation in highly-nonlinear media. The ansatz solution of Choudhuri and Porsezian (in Ref. [16]) is adapted to investigate solutions composed of the product of bright and dark solitary waves. Parametric conditions for the existence of the derived soliton solutions are given and their stabilities are numerically discussed. These exact solutions provide insight into balance mechanisms between several high-order nonlinearities of different na…

PhysicsApplied MathematicsSoliton (optics)Quintic functionDipolesymbols.namesakeClassical mechanicsModeling and SimulationProduct (mathematics)Quantum mechanicssymbolsRaman spectroscopyNonlinear Schrödinger equationParametric statisticsAnsatzApplied Mathematical Modelling
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Generation of High-Repetition-Rate Dark Soliton Trains and Frequency Conversion in Optical Fibers

1998

Induced modurational polarization instability in birefringent fibers leads to trains of dark soliton-like pulses. Optimal large-signal cw and soliton frequency conversion is also analysed.

PhysicsBirefringenceOptical fiberbusiness.industryPhysics::OpticsPolarization (waves)Instabilitylaw.inventionModulational instabilityNonlinear Sciences::Exactly Solvable and Integrable SystemsFrequency conversionOpticslawStimulate raman scatteringbusinessNonlinear Sciences::Pattern Formation and Solitons
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Multiple four-wave mixing-induced modulational instability in highly birefringent fibers.

2001

Theoretical and experimental results are presented that illustrate efficient generation of new optical frequencies by means of induced modulational instability in birefringent fibers for an initially highly phase-mismatched process. Modulational instability is assisted by multiple four-wave mixing interactions. This technique relaxes the strict spectral limitations imposed by the phase-matching conditions on the signal used for frequency conversion by means of modulational instability.

PhysicsBirefringencebusiness.industryCross-phase modulationSignalAtomic and Molecular Physics and Opticssymbols.namesakeModulational instabilityFour-wave mixingOpticsOptical frequenciessymbolsbusinessRaman scatteringMixing (physics)Optics letters
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H2-He vibrational line-shape parameters: Measurement and semiclassical calculation

1995

High-resolution inverse Raman spectroscopy has been used to obtain the line shifting and line broadening coefficients of H{sub 2} perturbed by He. Measurements have been made for the {ital Q}-branch transitions ({ital J}=0{r_arrow}5) in a density range of 10 to 20 amagat and from 296 to 995 K. Up to 795 K we have directly deduced from the experimental broadening coefficients the inelastic rotational state-to-state and vibrational dephasing rates. At higher temperatures, owing to the larger number of channels of relaxation which occur, the results have been analyzed using a scaling law. The line shift and broadening coefficients exhibit a square root and a linear dependence on temperature, r…

PhysicsComputer Science::Information RetrievalDephasingRelaxation (NMR)chemistry.chemical_elementInverseSemiclassical physicsAmagatAtomic and Molecular Physics and Opticssymbols.namesakechemistrysymbolsAtomic physicsRaman spectroscopyHeliumLine (formation)Physical Review A
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