Search results for " Clusters"

showing 10 items of 1091 documents

Surface plasmon circuitry in opto-electronics

2012

This tutorial reviews the physics of surface plasmon circuitry in order to bring to the fore recently demonstrated applications of surface plasmon in optoelectronics such as on-board optical interconnects or routing in datacom networks.

Optical data processingbusiness.industrySurface plasmonNear-field opticsNanophotonicsPhysics::OpticsSurface plasmon polaritonComputer Science::Hardware ArchitectureComputer Science::Emerging TechnologiesPhysics::Atomic and Molecular ClustersOptoelectronicsIntegrated opticsbusinessPlasmon
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Triple excitation effects in coupled-cluster calculations of frequency-dependent hyperpolarizabilities

1998

Abstract We describe an implementation of an analytic scheme for the calculation of static and dynamical first hyperpolarizabilities at the CC3 level in the framework of coupled-cluster response theory. Calculations are reported for the static, the second harmonic generation, and the optical rectification hyperpolarizabilities of FH. The results indicate the importance of triple excitation effects for accurate theoretical predictions of hyperpolarizabilities and lend further support to previous contentions that an experimental value for the second harmonic generation hyperpolarizabilities of FH should be reconsidered.

Optical rectificationCoupled clusterChemistryPhysics::Atomic and Molecular ClustersGeneral Physics and AstronomyValue (computer science)Second-harmonic generationPhysics::Atomic PhysicsPhysical and Theoretical ChemistryAtomic physicsExcitationChemical Physics Letters
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Excitation of plasmonic nanoantennas by nonresonant and resonant electron tunnelling.

2016

A rigorous theory of photon emission accompanied inelastic tunnelling inside the gap of plasmonic nanoantennas has been developed. The disappointingly low efficiency of the electrical excitation of surface plasmon polaritons in these structures can be increased by orders of magnitude when a resonant tunnelling structure is incorporated inside the gap. Resonant tunnelling assisted surface plasmon emitter may become a key element in future electrically-driven nanoplasmonic circuits.

Orders of magnitude (temperature)FOS: Physical sciencesPhysics::Optics02 engineering and technologyElectron01 natural sciences0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)Physics::Atomic and Molecular ClustersGeneral Materials Science010306 general physicsQuantum tunnellingPlasmonCommon emitterPhysicsCondensed Matter - Mesoscale and Nanoscale Physicsbusiness.industrySurface plasmon021001 nanoscience & nanotechnologySurface plasmon polariton3. Good healthOptoelectronics0210 nano-technologybusinessExcitationOptics (physics.optics)Physics - OpticsNanoscale
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Impacts of Copper Position on the Electronic Structure of [Au25-xCux(SH)18]− Nanoclusters

2015

Here, we use density functional theory to model the impact of heteroatom position on the optoelectronic properties of mixed metal nanoclusters. First, we consider the well-described [Au25(SH)18]− motif, and substitute Cu atoms at the three geometrically unique positions within the cluster. These clusters are atomically precise and show an electronic structure that is a function of both composition and heteroatom position. We then model clusters containing Cu substitutions at two positions, and demonstrate an additional and significant impact from heteroatom proximity with respect to one another. For each system, we report the formation energy, HOMO–LUMO gap, and energy level structure, and …

Organic electronicsta114ChemistryHeteroatomElectronic structureSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsNanoclustersElectronegativityGeneral EnergyComputational chemistryChemical physicsmixed metal nanoclustersPhysics::Atomic and Molecular ClustersCluster (physics)Level structureDensity functional theoryPhysical and Theoretical Chemistryta116Journal of Physical Chemistry C
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Measurement of the first ionization potential of astatine by laser ionization spectroscopy

2013

The radioactive element astatine exists only in trace amounts in nature. Its properties can therefore only be explored by study of the minute quantities of artificially produced isotopes or by performing theoretical calculations. One of the most important properties influencing the chemical behaviour is the energy required to remove one electron from the valence shell, referred to as the ionization potential. Here we use laser spectroscopy to probe the optical spectrum of astatine near the ionization threshold. The observed series of Rydberg states enabled the first determination of the ionization potential of the astatine atom, 9.31751(8) eV. New ab initio calculations are performed to sup…

Other Fields of PhysicsGeneral Physics and Astronomychemistry.chemical_element7. Clean energy01 natural sciencesGeneral Biochemistry Genetics and Molecular BiologyArticlePhysics in GeneralAb initio quantum chemistry methodsCHEMISTRYIonization0103 physical sciencesAtomPhysics::Atomic and Molecular ClustersFACILITYPhysics::Atomic Physics010306 general physicsAstatineSpectroscopyPhysicsMultidisciplinary010308 nuclear & particles physicsGeneral ChemistryION-SOURCEIon source3. Good healthchemistry13. Climate actionIonization energyAtomic physicsValence electronNature Communications
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"Table 2" of "Comprehensive measurements of $t$-channel single top-quark production cross sections at $\sqrt{s} = 7$ TeV with the ATLAS detector"

2021

Detailed list of the contribution of each source of uncertainty to the total uncertainty on the measured values of $\sigma(tq)$, $\sigma(\bar{t}q)$, $R_t$, and $\sigma(tq+\bar{t}q)$. The evaluation of the systematic uncertainties has a statistical uncertainty of $0.3\,\%$. Uncertainties contributing less than $1.0\,\%$ are marked with "$<1$" in the paper. To provide numerical values for this table in HEPdata, these uncertainties are approximated with $\pm 0.5\,\%$. This approximation is applied to all measurements for the following uncertainties$:$ JES statistical, JES physics modeling, JES mixed detector and modeling, JES close-by-jets, JES pileup, $b$-JES, jet vertex fraction, mistag e…

P P --> TOP XHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologySystematic uncertaintiesTop7000.0SIGComputer Science::Computers and SocietyInclusiveSingle Differential Cross SectionP P --> TOPBAR XNonlinear Sciences::Exactly Solvable and Integrable SystemsTotal cross sectionProton-Proton ScatteringPhysics::Atomic and Molecular Clusterst-channel productionDSIG/DPTHigh Energy Physics::ExperimentTransverse Momentum Dependence
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"Table 4" of "Comprehensive measurements of $t$-channel single top-quark production cross sections at $\sqrt{s} = 7$ TeV with the ATLAS detector"

2021

Parametrization factors for the $m_{t}$ dependence [see Eq. (4) in the paper] of $\sigma(tq)$, $\sigma(\bar tq)$, and $\sigma(t q+\bar t q)$.

P P --> TOP XHigh Energy Physics::LatticeRapidity DependenceHigh Energy Physics::PhenomenologyTop7000.0DSIG/DYRAPSIGSingle Differential Cross SectionP P --> TOPBAR XInclusiveNonlinear Sciences::Exactly Solvable and Integrable SystemsTotal cross-sectionProton-Proton ScatteringPhysics::Atomic and Molecular ClustersHigh Energy Physics::Experiment
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"Table 1" of "Comprehensive measurements of $t$-channel single top-quark production cross sections at $\sqrt{s} = 7$ TeV with the ATLAS detector"

2014

Predicted and observed events yields for the 2-jet and 3-jet channels considered in this measurement. The multijet background is estimated using data-driven techniques (see Sec. VB); an uncertainty of $50\%$ is applied. All the other expectations are derived using theoretical cross sections and their uncertainties (see Secs. VA and VC in the paper).

P P --> TOP XHigh Energy Physics::PhenomenologyTop7000.0event yieldNComputer Science::Computers and SocietyP P --> TOPBAR XNonlinear Sciences::Chaotic DynamicsInclusiveSingle Differential Cross SectionNonlinear Sciences::Exactly Solvable and Integrable SystemsProton-Proton ScatteringPhysics::Atomic and Molecular Clusterst-channel productionDSIG/DPTTransverse Momentum Dependence
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"Table 12" of "Comprehensive measurements of $t$-channel single top-quark production cross sections at $\sqrt{s} = 7$ TeV with the ATLAS detector"

2021

Differential t-channel top-quark production cross section as a function of $p_{\mathrm{T}}(\bar t)$ with the uncertainties for each bin given in percent.

P P --> TOPBAR XInclusiveNonlinear Sciences::Exactly Solvable and Integrable SystemsSingle differential cross-sectionProton-Proton ScatteringHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyPhysics::Atomic and Molecular ClustersTop7000.0High Energy Physics::ExperimentDSIG/DPTTransverse Momentum Dependence
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"Table 18" of "Comprehensive measurements of $t$-channel single top-quark production cross sections at $\sqrt{s} = 7$ TeV with the ATLAS detector"

2021

Normalized differential t-channel top-quark production cross section as a function of $|y(\bar t)|$ with the uncertainties for each bin given in percent.

P P --> TOPBAR XInclusiveNonlinear Sciences::Exactly Solvable and Integrable SystemsSingle differential cross-sectionProton-Proton ScatteringHigh Energy Physics::LatticeRapidity DependenceHigh Energy Physics::PhenomenologyPhysics::Atomic and Molecular ClustersTop7000.0High Energy Physics::Experiment1/SIG*DSIG/DYRAP
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