Search results for "Physics::Optics"

showing 10 items of 1958 documents

The interaction of surface plasmon polaritons with a silver film edge.

2001

A prism coupling arrangement is used to excite surface plasmons at the surface of a thin silver film and a photon scanning tunnelling microscope is used to detect the evanescent field above the silver surface. Excitation of the silver/air mode of interest is performed at lambda1 = 632.8 nm using a tightly focused beam, while the control of the tip is effected by exciting a counter-propagating surface plasmon field at a different wavelength, lambda2 = 543.5 nm, using an unfocused beam covering a macroscopic area. Propagation of the red surface plasmon is evidenced by an exponential tail extending away from the launch site, but this feature is abruptly truncated if the surface plasmon encount…

HistologyMaterials sciencebusiness.industryScatteringSurface plasmonNanophotonicsPhysics::OpticsSurface finishSurface plasmon polaritonPathology and Forensic MedicineOpticsPhysics::Atomic and Molecular ClustersSurface plasmon resonancebusinessExcitationLocalized surface plasmonJournal of microscopy
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Single molecules probe local density of modes (LDOS) around photonic nanostructures

2008

International audience; According to Fermi's golden rule, the fluorescence decay rate is directly proportional to the projected local density of photonic modes (LDOS) at the molecule location. The relevant LDOS depends on the molecule orientation. In this paper, the direct measurement of the fluorescence lifetime near gold dot photonic structures is investigated and compared to calculated LDOS. Detailed analysis of the decay channels is presented on the basis of numerical simulations.

HistologyNanostructureFLUORESCENCE LIFETIME[SPI.NANO] Engineering Sciences [physics]/Micro and nanotechnologies/MicroelectronicsPhysics::Optics02 engineering and technology01 natural sciencesPathology and Forensic MedicineELECTROMAGNETIC SCATTERINGMEDIACondensed Matter::Superconductivity0103 physical sciencesMolecule[SPI.NANO]Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics010306 general physicsChemistrybusiness.industry021001 nanoscience & nanotechnologyCondensed Matter::Mesoscopic Systems and Quantum Hall EffectFluorescenceSPONTANEOUS-EMISSION[ SPI.NANO ] Engineering Sciences [physics]/Micro and nanotechnologies/MicroelectronicsPhotonicsAtomic physics0210 nano-technologybusinessFermi Gamma-ray Space Telescope
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Light field propagation by metal micro- and nanostructures

2001

The ability to sustain plasmon oscillations gives rise to unique properties of metal nanostructures, which can be exploited for the controlled manipulation of light fields on the nanoscale. In this context we investigate electromagnetic coupling effects within lithographically produced ensembles of gold nanoparticles with a photon scanning tunnelling microscope. To provide an interface between these nano-optical devices and classical far-field optics, we investigate surface plasmon propagation on microstructured metal thin films.

HistologyNanostructureMicroscopeMaterials sciencebusiness.industrySurface plasmonNanophotonicsPhysics::OpticsContext (language use)NanotechnologyPathology and Forensic Medicinelaw.inventionlawOptoelectronicsbusinessLight fieldPlasmonQuantum tunnellingJournal of Microscopy
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Millimeter wave absorption by confined acoustic modes in CdSe/CdTe core-shell quantum dots

2007

International audience; Taking advantage of the specific core-shell charge separation structure in the CdSe/CdTe core-shell Type-II quantum dots (QDs), we experimentally observed the resonant-enhanced dipolar interaction between millimeter-wave (MMW) photons and their corresponding (l = 1) confined acoustic phonons. With proper choice of size, the absorption band can be tuned to desired frequency of MMW imaging. Exploiting this characteristic absorption, in a fiber-scanned MMW imaging system, we demonstrated the feasibility of CdSe/CdTe QDs as the contrast agents of MMW imaging.

HistoryPhotonMaterials science[ PHYS.COND.CM-MS ] Physics [physics]/Condensed Matter [cond-mat]/Materials Science [cond-mat.mtrl-sci]Physics::Optics02 engineering and technology01 natural sciencesEducationCore shellCondensed Matter::Materials Science0103 physical sciences010306 general physicsAbsorption (electromagnetic radiation)business.industryCondensed Matter::Other021001 nanoscience & nanotechnologyCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCadmium telluride photovoltaicsComputer Science ApplicationsDipoleQuantum dotAbsorption bandExtremely high frequency[PHYS.COND.CM-MS]Physics [physics]/Condensed Matter [cond-mat]/Materials Science [cond-mat.mtrl-sci]Optoelectronics0210 nano-technologybusiness
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Class-B two-photon Fabry–Pérot laser

1998

Abstract We study the stationary operation and stability properties of a class-B two-photon Fabry–Perot laser. We show that, differently from the one-photon laser, the intensity emitted by the two-photon laser is larger in a Fabry–Perot than in a ring cavity. The lasing solution loses stability through a subcritical Hopf bifurcation, as it occurs in the unidirectional ring laser. The stability domain in the parameter space is larger in the Fabry–Perot than in the ring cavity configuration.

Hopf bifurcationPhysicsDistributed feedback laserPhysics::Instrumentation and Detectorsbusiness.industryAstrophysics::Instrumentation and Methods for AstrophysicsPhysics::OpticsRing laserLaserAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsRound-trip gainlaw.inventionsymbols.namesakeOpticslawsymbolsLaser power scalingElectrical and Electronic EngineeringPhysical and Theoretical ChemistrybusinessLasing thresholdFabry–Pérot interferometerOptics Communications
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One- and two-photon lasers with injected signal in a high-Q fabry-Pérot cavity

2000

Explicit models are derived for good cavity one- and two-photon lasers with an injected signal in a Fabry-Perot cavity. The steady solutions and their stability properties are obtained analytically and compared with the corresponding ring cavity model ones. Only quantitative differences between both types of cavities are found. In particular we show that (i) the Fabry-Perot cavity reduces significantly the domain of self-pulsing with respect to the ring cavity, and for the two-photon laser case (ii) larger output can be extracted from a Fabry-Perot cavity than from a ring cavity under certain conditions, something impossible in free-running lasers. We conclude that ring cavity models are se…

Hopf bifurcationPhysicsPhysics::Instrumentation and Detectorsbusiness.industryAstrophysics::Instrumentation and Methods for AstrophysicsPhysics::OpticsLaserRing (chemistry)SignalAtomic and Molecular Physics and Opticslaw.inventionLongitudinal modesymbols.namesakeOpticslawOptical cavityDomain (ring theory)symbolsPhysics::Accelerator PhysicsAtomic physicsbusinessFabry–Pérot interferometerJournal of Modern Optics
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Cavity solitons in nondegenerate optical parametric oscillation

2000

Abstract We find analytically cavity solitons in nondegenerate optical parametric oscillators. These solitons are exact localised solutions of a pair of coupled parametrically driven Ginzburg–Landau equations describing the system for large pump detuning. We predict the existence of a Hopf bifurcation of the soliton resulting in a periodically pulsing localised structure. We give numerical evidence of the analytical results and address the problem of cavity soliton interaction.

Hopf bifurcationPhysicsbusiness.industryParametric oscillationGinzburg landau equationPhysics::OpticsNonlinear opticsAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialssymbols.namesakeNonlinear Sciences::Exactly Solvable and Integrable SystemsExact solutions in general relativityOpticsQuantum mechanicsQuantum electrodynamicssymbolsSolitonElectrical and Electronic EngineeringPhysical and Theoretical ChemistrybusinessNonlinear Sciences::Pattern Formation and SolitonsParametric statisticsOptics Communications
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Thermal lens spectrometry in biochemical analysis.

1994

The photothermal spectroscopic techniques, with special emphasis on the thermal lens spectrometry (TLS), are introduced to the non-specialist in laser spectroscopy. The following topics are treated on an elementary basis: fundamentals and analytical characteristics, instrumentation, selectivity and multi-wavelength capability, the models describing the signal-concentration relationship, the sensitivity, background noise and limits of detection, the influence of light scattering and flow. Applications related to the fields of clinical and biochemical analysis and organic pollution are given. The thermal lens circular dichroism and the infrared TLS are also briefly outlined.

Hot TemperatureSpectrophotometry InfraredInfraredbusiness.industryChemistryCircular DichroismLasersBiophysicsPhysics::OpticsPhotothermal therapyLaserMass spectrometryBiochemistryLight scatteringlaw.inventionBackground noiseLens (optics)OpticslawSpectrophotometryScattering RadiationSpectroscopybusinessJournal of biochemical and biophysical methods
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The Optimal Aspect Ratio for Plasmonic Bio-Sensing

2012

The sensitivity of plasmonic particles to the immediate dielectric environment allows to monitor the dielectric constant of liquids and binding events of molecules to the gold particle surface. Here, by means of simulations and experiments, I investigate which aspect ratio (AR) of gold nanorods is ideal for plasmonic sensing by employing various measures for “ideal” behavior.

Ideal (set theory)Materials sciencebusiness.industryPhysics::OpticsOptoelectronicsParticleMoleculeNanorodDielectricSensitivity (control systems)businessAspect ratio (image)Plasmon
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Electro-optic control of photographic imaging quality through ‘Smart Glass’ windows in optics demonstrations

2017

An experimental setup allowing the modeling of conditions in optical devices and in the eye at various degrees of scattering such as cataract pathology in human eyes is presented. The scattering in cells of polymer-dispersed liquid crystals (PDLCs) and 'Smart Glass' windows is used in the modeling experiments. Both applications are used as optical obstacles placed in different positions of the optical information flow pathway either directly on the stimuli demonstration computer screen or mounted directly after the image-formation lens of a digital camera. The degree of scattering is changed continuously by applying an AC voltage of up to 30–80 V to the PDLC cell. The setup uses a camera wi…

Image formationPoint spread functionPhysicsbusiness.product_categorybusiness.industryScatteringPhysics::OpticsGeneral Physics and Astronomy02 engineering and technology021001 nanoscience & nanotechnologyLaser01 natural scienceslaw.invention010309 opticsLens (optics)Opticslaw0103 physical sciencesOptoelectronicsFocal length0210 nano-technologybusinessDigital cameraDiodeEuropean Journal of Physics
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