Search results for "EXCITATION"

showing 10 items of 1290 documents

Molecular structures inT=1states of10B

2011

Multi-center (molecular) structures can play an important role in light nuclei. The highly deformed rotational band in 10Be with band head at 6.179 MeV has been observed recently and suggested to have an exotic alpha:2n:alpha configuration. A search for states with alpha:pn:alpha two-center molecular configurations in 10B that are analogous to the states with alpha:2n:alpha structure in 10Be has been performed. The T=1 isobaric analog states in 10B were studied in the excitation energy range of E=8.7-12.1 MeV using the reaction 1H(9Be,alpha)6Li*(T=1, 0+, 3.56 MeV). An R-matrix analysis was used to extract parameters for the states observed in the (p,alpha) excitation function. Five T=1 stat…

Excitation functionPhysicsNuclear and High Energy PhysicsRange (particle radiation)Light nucleus010308 nuclear & particles physicsAlpha (ethology)State (functional analysis)01 natural sciences0103 physical sciencesIsobaric processAtomic physics010306 general physicsExcitationPhysical Review C
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A new resonance in thee-H2-scattering

1969

A short-lived compound state of the systeme-H2 in the energy region from 13.5 to 15 eV has been investigated. It desintegrates preferably into theC 1 π u v=0, 1, 2, 3,... vibrational states of H2. Excitation functions and angular dependences of these states have been measured. The H2 vibrational levels are situated at 13.63, 13.93, 14.20, 14.70, 14.92,... eV. The shape of the potential energy curve and the internuclear distance of the compound state should be very similar to that of theC 1 π u resp.D 1 π u state ofH 2.

Excitation functionPhysicsNuclear and High Energy PhysicsScatteringMoleculeNuclear fusionState (functional analysis)Atomic physicsPotential energyResonance (particle physics)ExcitationZeitschrift für Physik A Hadrons and nuclei
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Crossing the dripline to11Nusing elastic resonance scattering

2000

The level structure of the unbound nucleus N-11 has been studied by C-10+p elastic resonance scattering in inverse geometry with the LISE3 spectrometer at GANIL, using a C-10 beam with an energy of 9.0 MeV/ nucleon. An additional measurement was done at the A1200 spectrometer at MSU. The excitation function above the C-10+p threshold has been determined up to 5 MeV. A potential-model analysis revealed three resonance states at energies 1.27(-0.05)(+0.18) MeV (Gamma = 1.44 +/- 0.2 MeV), 2.01(-0.05)(+0.15) MeV (Gamma = 0.84 +/- 0.2 MeV), and 3.75 +/- 0.05 MeV (Gamma = 0.60 +/- 0.05 MeV) with the spin-parity assignments I-pi=1/2+,1/2,-,5/2+, respectively. Hence, N-11 is shown to have a ground …

Excitation functionPhysicsNuclear and High Energy PhysicsSpectrometer010308 nuclear & particles physicsNuclear Theory01 natural sciencesResonance (particle physics)0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary AstrophysicsAtomic physicsNuclear Experiment010306 general physicsGround stateSpin (physics)NucleonSpectroscopyParity (mathematics)Physical Review C
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Determination of theη′-Proton Scattering Length in Free Space

2014

Taking advantage of both the high mass resolution of the COSY-11 detector and the high energy resolution of the low-emittance proton beam of the cooler synchrotron COSY, we determine the excitation function for the $pp\ensuremath{\rightarrow}pp{\ensuremath{\eta}}^{\ensuremath{'}}$ reaction close to threshold. Combining these data with previous results, we extract the scattering length for the ${\ensuremath{\eta}}^{\ensuremath{'}}$-proton potential in free space to be $\mathrm{Re}({a}_{p{\ensuremath{\eta}}^{\ensuremath{'}}})=0\ifmmode\pm\else\textpm\fi{}0.43\text{ }\text{ }\mathrm{fm}$ and $\mathrm{Im}({a}_{p{\ensuremath{\eta}}^{\ensuremath{'}}})={0.37}_{\ensuremath{-}0.16}^{+0.40}\text{ }\t…

Excitation functionPhysicsParticle physicsMeson productionProton010308 nuclear & particles physicsGeneral Physics and AstronomyScattering lengthFree space01 natural sciencesProton scattering0103 physical sciencesHigh massHigh Energy Physics::ExperimentAtomic physicsNuclear Experiment010306 general physicsHigh energy resolutionPhysical Review Letters
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Multinucleon transfer reactions and proton transfer channels

2019

Transfer reactions have always been of great importance for nuclear structure and reaction mechanism studies. So far, in multinucleon transfer studies, proton pickup channels have been completely identified in atomic and mass numbers at energies close to the Coulomb barrier only in few cases. We measured the multinucleon transfer reactions in the 40Ar+208Pb system near the Coulomb barrier, by employing the PRISMA magnetic spectrometer. By using the most neutron-rich stable 40Ar beam we could populate, besidesneutron pickup and proton stripping channels, also neutron stripping and proton pickup channels. Comparison ofcross sections between different systems with the 208Pb target and with pro…

Excitation functionPhysicsReaction mechanismSpectrometer010308 nuclear & particles physicsPhysicsQC1-999Nuclear TheoryNuclear structureCoulomb barriermultinucleon transfer reactions01 natural sciences7. Clean energyStripping (fiber)0103 physical sciencesPhysics::Accelerator PhysicsNeutronPickupAtomic physics010306 general physicsNuclear Experiment
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Inner-shell excitation spectroscopy of closo-carboranes

1997

Oscillator strength spectra in the region of B 1s and C 1s excitation of three isomeric carborane cage compounds [closo-1,2-orthocarborane, closo-1,7-metacarborane, closo-1,12-paracarborane (C2B10H...

Excitation spectroscopyOscillator strengthChemistryParticle acceleratorSpectral lineSurfaces Coatings and Filmslaw.inventionlawMaterials ChemistryCarboraneInner shellPhysical and Theoretical ChemistryAtomic physicsExcitation
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Colloidal Nanoplatelet/Conducting Polymer Hybrids: Excitonic And Material Properties

2016

WOS:000370678700053 Here we present the first account of conductive polymer/colloidal nanoplatelet hybrids. For this, we developed DEH-PPV-based polymers with two different anchor groups (sulfide and amine) acting as surfactants for CdSe nanoplatelets, which are atomically flat semiconductor nanocrystals. Hybridization of the polymers with the nanoplatelets in the solution phase was observed to cause strong photoluminescence quenching in both materials. Through steady-state photoluminescence and excitation spectrum measurements, photoluminescence quenching was shown to result from dominant exciton dissociation through charge transfer at the polymer/nanoplatelet interfaces that possess a sta…

Excitation spectrumMaterials sciencePhotoluminescenceSulfideDEH-PPV-Based PolymersSulfideExcitonCdSe NanoplateletsNanotechnology02 engineering and technologySurface active agents010402 general chemistryOptoelectronic devices01 natural sciencesDissociation (chemistry)ColloidCharge transferQuenchingHybrid optoelectronic devicesPhysical and Theoretical ChemistryPhotoluminescenceSulfur compoundsAmineSemiconductor nanocrystalsConductive polymerchemistry.chemical_classificationExcited statesBuilding blockesPolymerInterface statesEmission quenching021001 nanoscience & nanotechnology0104 chemical sciencesSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsPolymer/Colloidal Nanoplatelet HybridsGeneral EnergyChemical engineeringchemistryExcited stateAnchorsExcitons0210 nano-technologyDissociationConductive polymerPhotoluminescence quenchingExciton dissociation
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Transient and near‐edge absorption in YVO 4 crystals

2007

The process of near-edge absorption annealing in air was studied up to 1500C in YVO4. In this annealing process, two stages with activation energies of 0.16 eV and 0.38 eV were obtained. (Should combine to make this one paragraph)In addition to the annealing study, the transient absorption induced by pulsed electron beam excitation (270 keV, 8 ns) was completed on a set of YVO4 samples with different near-edge absorption levels in the spectral region 3.2-3.5 eV. The spectral range from ∼1.25 eV up to 3.0 eV is covered by strong transient absorption. Transient absorption spectra show at least three broad overlapping bands (∼1.3 eV, ∼2.0 eV and ∼3.0 eV). The 3 eV peak position is close to the…

Extended X-ray absorption fine structureChemistryAbsorption bandAnnealing (metallurgy)Ultrafast laser spectroscopyElectronAtomic physicsCondensed Matter PhysicsPolaronExcitationSpectral linephysica status solidi c
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Acoustic Scene Classification with Squeeze-Excitation Residual Networks

2020

Acoustic scene classification (ASC) is a problem related to the field of machine listening whose objective is to classify/tag an audio clip in a predefined label describing a scene location (e. g. park, airport, etc.). Many state-of-the-art solutions to ASC incorporate data augmentation techniques and model ensembles. However, considerable improvements can also be achieved only by modifying the architecture of convolutional neural networks (CNNs). In this work we propose two novel squeeze-excitation blocks to improve the accuracy of a CNN-based ASC framework based on residual learning. The main idea of squeeze-excitation blocks is to learn spatial and channel-wise feature maps independently…

FOS: Computer and information sciencesSound (cs.SD)Computer Science - Machine LearningGeneral Computer ScienceCalibration (statistics)Computer scienceResidualConvolutional neural networkField (computer science)Computer Science - SoundMachine Learning (cs.LG)030507 speech-language pathology & audiology03 medical and health sciencesAudio and Speech Processing (eess.AS)Acoustic scene classificationFeature (machine learning)FOS: Electrical engineering electronic engineering information engineeringGeneral Materials ScienceBlock (data storage)Artificial neural networkbusiness.industrypattern recognitionGeneral Engineeringdeep learningPattern recognitionmachine listeningsqueeze-excitationArtificial intelligencelcsh:Electrical engineering. Electronics. Nuclear engineering0305 other medical sciencebusinesslcsh:TK1-9971Electrical Engineering and Systems Science - Audio and Speech Processing
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Faraday patterns in bose-Einstein condensates.

2002

Temporal periodic modulation of the interatomic s-wave scattering length in Bose-Einstein condensates is shown to excite subharmonic patterns of atom density through a parametric resonance. The dominating wavelength of the spatial structures is shown to be primarily selected by the excitation frequency but also affected by the depth of the spatial modulation via a nonlinear resonance. These phenomena represent macroscopic quantum analogues of the Faraday waves excited in vertically shaken liquids.

FOS: Physical sciencesGeneral Physics and AstronomyPattern formationPattern Formation and Solitons (nlin.PS)Resonance (particle physics)law.inventionFaraday wavesymbols.namesakelawQuantum mechanicsFaraday effectFaraday cageFeshbach resonanceCondensed Matter - Statistical MechanicsPhysicsCondensed Matter::Quantum GasesStatistical Mechanics (cond-mat.stat-mech)Condensed matter physicsScatteringCondensed Matter::OtherResonanceScattering lengthNonlinear Sciences - Pattern Formation and SolitonsSymmetry (physics)Magnetic fieldModulationNonlinear resonanceExcited statesymbolsDissipative systemState of matterAtomic physicsParametric oscillatorExcitationBose–Einstein condensatePhysical review letters
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