Search results for "Photon"

showing 10 items of 3171 documents

Hyperspectral near-field imaging : development and applications to nanophotonics devices

2013

The scanning near-field optical microscopy (SNOM) is used to analyze optical phenomena at the sub-wavelength scale such as light localization and propagation in photonic crystals or plasmonic devices. In any case, SNOM experiments rely on the positioning of a local probe in the optical near field of a given structure and on the detection of the surrounding evanescent waves. Depending on the nature of the probe or on the optical detection method, the detected physical properties are the spatial distributions of the amplitude and phase or the intensity of the electric and magnetic components of the probed field. We present here the implementation of an innovative hyperspectral near-field imag…

[SPI.OTHER]Engineering Sciences [physics]/OtherCristaux photoniques[ SPI.OTHER ] Engineering Sciences [physics]/Other[SPI.OTHER] Engineering Sciences [physics]/OtherPlasmon beamNanophotoniqueNear-field opticsChamp proche optique[ PHYS.COND.CM-GEN ] Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]Faisceaux plasmoniquesPhotonic crystals[PHYS.COND.CM-GEN] Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other][CHIM.OTHE] Chemical Sciences/Other[PHYS.COND.CM-GEN]Physics [physics]/Condensed Matter [cond-mat]/Other [cond-mat.other]Hyperspectral imaging method[ CHIM.OTHE ] Chemical Sciences/OtherImagerie hyperspectraleNanophotonics[CHIM.OTHE]Chemical Sciences/Other
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On chip shapeable optical tweezers

2013

International audience; Particles manipulation with optical forces is known as optical tweezing. While tweezing in free space with laser beams was established in the 1980s, integrating the optical tweezers on a chip is a challenging task. Recent experiments with plasmonic nanoantennas, microring resonators, and photonic crystal nanocavities have demonstrated optical trapping. However, the optical field of a tweezer made of a single microscopic resonator cannot be shaped. So far, this prevents from optically driven micromanipulations. Here we propose an alternative approach where the shape of the optical trap can be tuned by the wavelength in coupled nanobeam cavities. Using these shapeable …

[SPI.OTHER]Engineering Sciences [physics]/OtherMultidisciplinaryMaterials sciencebusiness.industryPhysics::Optics02 engineering and technologyOptical field021001 nanoscience & nanotechnologyChip01 natural sciencesArticle010309 opticsResonatorWavelengthOptical tweezers0103 physical sciencesTweezersOptoelectronics0210 nano-technologybusinessPlasmonComputingMilieux_MISCELLANEOUSPhotonic crystal
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Hf02 based RRAM: from materials engineering to integrated modules

2015

10 mars 2015; International audience; no abstract

[SPI]Engineering Sciences [physics][SPI.OPTI] Engineering Sciences [physics]/Optics / Photonic[SPI] Engineering Sciences [physics][SPI.NANO] Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics[ SPI.MAT ] Engineering Sciences [physics]/Materials[ SPI ] Engineering Sciences [physics][SPI.OPTI]Engineering Sciences [physics]/Optics / Photonic[ SPI.NANO ] Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics[ SPI.OPTI ] Engineering Sciences [physics]/Optics / Photonic[SPI.MAT] Engineering Sciences [physics]/Materials[SPI.NANO]Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics[SPI.MAT]Engineering Sciences [physics]/Materials
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Absorption enhancement in monocrystalline Si thin films using pseudodisordered structures

2015

21-25 june 2015; International audience; no abstract

[SPI]Engineering Sciences [physics][SPI.OPTI] Engineering Sciences [physics]/Optics / Photonic[SPI] Engineering Sciences [physics][SPI.NANO] Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics[ SPI.MAT ] Engineering Sciences [physics]/Materials[ SPI ] Engineering Sciences [physics][SPI.OPTI]Engineering Sciences [physics]/Optics / Photonic[ SPI.NANO ] Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics[ SPI.OPTI ] Engineering Sciences [physics]/Optics / Photonic[SPI.MAT] Engineering Sciences [physics]/Materials[SPI.NANO]Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics[SPI.MAT]Engineering Sciences [physics]/Materials
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When nanophotonics meet thin crystalline-silicon photovoltaics

2015

11-18 sept. 2015; International audience; no abstract

[SPI]Engineering Sciences [physics][SPI.OPTI] Engineering Sciences [physics]/Optics / Photonic[SPI] Engineering Sciences [physics][SPI.NANO] Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics[ SPI.MAT ] Engineering Sciences [physics]/Materials[SPI.OPTI]Engineering Sciences [physics]/Optics / Photonic[ SPI ] Engineering Sciences [physics][ SPI.NANO ] Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics[ SPI.OPTI ] Engineering Sciences [physics]/Optics / Photonic[SPI.MAT] Engineering Sciences [physics]/Materials[SPI.NANO]Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics[SPI.MAT]Engineering Sciences [physics]/Materials
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Optical parametric amplification in gas-filled hollow core capillary for the generation of tunable pulses in the infrared

2020

International audience; Ultrashort pulses in the near-infrared (NIR) to mid-infrared (MIR) are widely used for laser matter interaction experiments, e.g. the relaxation process of carrier semiconductors and chemical dynamics at the femtosecond and attosecond time scale [1,2]. Many different approaches based on nonlinear processes or laser devices can be found to generate pulses in theses spectral ranges. Recently, four wave mixing (FWM) based parametric amplification in gas-filled hollow core capillary (HCC) has been used to create a tunable source of ultrashort pulses. For example, pulses can be generated in the visible with an energy at the 10 µJ level [4] and in the near infrared at ~1.4…

[SPI]Engineering Sciences [physics][SPI.OPTI] Engineering Sciences [physics]/Optics / Photonic[SPI] Engineering Sciences [physics][SPI.OPTI]Engineering Sciences [physics]/Optics / Photonic
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Molecular Insights on alpha-synuclein mediated membrane disruption: protein-lipid co-aggregates formation

2014

amyloid intrinsically disordered protein 2-photon fluorescence microscopy
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Photonic crystal intermediate reflector in micromorph tandem solar cells

2011

Experimental and numerical evidences are presented which show that the efficiency of silicon based tandem solar-cells can be increased by incorporating a three-dimensional photonic crystal as an intermediate reflector.

animal structuresMaterials scienceTandemSiliconbusiness.industryMicromorphPhotovoltaic systemfood and beveragesPhysics::Opticschemistry.chemical_elementReflector (antenna)Solar cell efficiencyOpticschemistryOptoelectronicsPhotonicsbusinessPhotonic crystal
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Observation of Higgs boson production in association with a top quark pair at the LHC with the ATLAS detector

2018

Physics letters / B 784, 173 - 191 (2018). doi:10.1016/j.physletb.2018.07.035

associated production [Higgs particle]Yukawa [coupling]13000 GeV-cms01 natural sciencesStandard deviationSubatomär fysikscattering [p p]Z0: pair productionCollisionsmeasured [total cross section]протон-протонные столкновенияGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)ComputingMilieux_MISCELLANEOUSLHC; Higgs; Top-QuarkLarge Hadron ColliderQ007THXlcsh:QC1-999Top-Quark:Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]pair production [Z0]CERN LHC CollHiggs bosonХиггса бозонcolliding beams [p p]top: pair productionHiggs particle: decay modesp p: scatteringmass spectrum: (4lepton)Ciências Naturais::Ciências FísicasAstrophysics::High Energy Astrophysical PhenomenaSTANDARD MODELddc:500.2SEARCHddc:530High Energy Physics010306 general physicstop quarktwo-photon [mass spectrum]Science & TechnologyHiggs particle: coupling010308 nuclear & particles physics(4lepton) [mass spectrum]HIGGSExperimental High Energy PhysicsATLAS детекторp p: colliding beamslcsh:Physicscoupling: Yukawamass spectrum: two-photonHiggsTop quarkHiggs Top LHC observationБольшой адронный коллайдерAtlas detectorCiencias Físicasbranching ratio [Higgs particle]pair production [top]High Energy Physics - Experiment//purl.org/becyt/ford/1 [https]W: pair productionHigh Energy Physics - Experiment (hep-ex)Subatomic Physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Physicsscattering | p p: colliding beams | top: pair production | Higgs particle: associated production | Higgs particle: decay modes | bottom: pair production | W: pair production | Z0: pair production | tau: pair production | photon: pair production | Higgs particle: coupling | coupling: Yukawa | CERN LHC Coll | ATLAS | mass spectrum: two-photon | mass spectrum: (4lepton) | Higgs particle: branching ratio | total cross section: measured | experimental results | 13000 GeV-cms [p p]proton–proton collisionstau: pair productionSettore FIS/01 - Fisica SperimentaleTOPATLASpair production [bottom]pair production [tau]S126STHpair production [W]LHCphoton: pair productionCIENCIAS NATURALES Y EXACTASParticle Physics - Experimentpair production [photon]jetsParticle physicsNuclear and High Energy Physicscoupling [Higgs particle]Higgs boson530 Physics:Ciências Físicas [Ciências Naturais]decay modes [Higgs particle]FOS: Physical sciencesbottom: pair productionFísica de Partículas y Campos5300103 physical sciencesHigh Energy Physics::Phenomenology:Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431 [VDP]//purl.org/becyt/ford/1.3 [https]Higgs particle: associated productionHiggs particle: branching ratiototal cross section: measuredHigh Energy Physics::ExperimentHadron-hadron collisionsexperimental results
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Searching for signatures around 1920 MeV of a N-* state of three hadron nature

2009

We provide a series of arguments which support the idea that the peak seen in the gamma p -> K+ Lambda reaction around 1920 MeV should correspond to the recently predicted state of J(P) = 1/2(+) as a bound state of K(K) over bar N with a mixture of alpha(0)(980)N and f(0)(980)N components. At the same time we propose polarization experiments in that reaction as a further test of the prediction, as well as a study of the total cross-section for gamma p -> K(+)K(-)p at energies close to threshold and of d sigma/dM(inv) for invariant masses close to the two-kaon threshold.

associated production [K+]Nuclear and High Energy PhysicsParticle physicsNuclear TheoryHadronFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)photon p --> Sigma0 K+0103 physical sciencesBound stateddc:530angular distributionbound state [K]010306 general physicstotal cross section(nucleon K anti-K) [bound state]Physicspolarizationhadroproduction [Lambda]intermediate state [f0(980)]photon p --> p K+ K-010308 nuclear & particles physicsFísica(1920) [nucleon resonance]Sigmaintermediate state [a0(980)]Polarization (waves)exclusive reaction [photon p]interpretation of experimentsproposed experimentphoton p --> Lambda K+
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