Search results for "COPP"

showing 10 items of 3147 documents

Photoluminescent Cu(i) vs. Ag(i) complexes: slowing down emission in Cu(i) complexes by pentacoordinate low-lying excited states.

2019

This work describes the synthesis, and structural, spectroscopic, and theoretical studies of a mononuclear silver(i) complex with the formula [Ag(Xantphos)(4,4'-(MeO)2-2,2'-bipy)]BF4·DCM (1·BF4) [Xantphos: 4,5-bis(diphenylphosphino)-9,9'-dimethylxanthene]. We provide meaningful insights into the enhancement of the photoluminescence features of this silver(i) complex compared to its copper(i) analogue.

PhotoluminescenceMaterials science010405 organic chemistryXantphoschemistry.chemical_element010402 general chemistry01 natural sciencesCopper0104 chemical sciencesInorganic ChemistryCrystallographychemistry.chemical_compoundchemistryExcited stateDalton transactions (Cambridge, England : 2003)
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σ-Hammett parameter: a strategy to enhance both photo- and electro-luminescence features of heteroleptic copper(i) complexes

2017

This work studies the effect of the σ-Hammett parameter (σp) – i.e., the σ-donation effect caused by substitution at the para position of a bipyridine ligand (4,4′-R2bipy, where R is MeO, Me, H, NO2) – on both the photo- and electro-luminescence features of a series of heteroleptic copper(I) complexes – i.e., [Cu(N^N)(P^P)]+ where N^N and P^P ligands are R2bipy and Xantphos, respectively. By virtue of a comprehensive photophysical, theoretical, and thin-film lighting device – i.e., light-emitting electrochemical cells (LECs) – investigation, we note a clear relationship between the σp and the photo- and electro-luminescence parameters, such as photoluminescence quantum yields, excited-state…

PhotoluminescenceXantphosLigandchemistry.chemical_element02 engineering and technology010402 general chemistry021001 nanoscience & nanotechnologyPhotochemistry01 natural sciencesCopper0104 chemical sciencesElectrochemical cellInorganic ChemistryPara positionchemistry.chemical_compoundBipyridinechemistryElectro luminescencePhysical chemistry0210 nano-technologyDalton Transactions
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Photovoltaic module characteristics from CIGS solar cell modelling

2013

We describe our approach to the task of modelling, both at single cell structure and complete module levels, during the solar cell technology development process. This can give very helpful indications, in terms of global photovoltaic module characteristics, for the assessment of intermediate research results and planning of further experiments. We make reference specifically to the fabrication of thin film CIGS solar cells by means of single-step electrodeposition, a technique which appears fairly easy and low-cost but, at the same time, can lead to quite different structural and electrical properties.

Photonic structuresMaterials sciencebusiness.industryCIGS solar cellPhotovoltaic systemSettore ING-INF/02 - Campi ElettromagneticiHybrid solar cellSettore ING-IND/32 - Convertitori Macchine E Azionamenti ElettriciQuantum dot solar cellSettore ING-INF/01 - ElettronicaCopper indium gallium selenide solar cellsEngineering physicsModellingPolymer solar celllaw.inventionPhotovoltaic thermal hybrid solar collectorSolar energyPhotovoltaic modulelawSolar cellOptoelectronicsSolar simulatorThin-film solar cellbusinessSimulation2013 International Conference on Renewable Energy Research and Applications (ICRERA)
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Direct measurement of the electron‐phonon relaxation rate in thin copper films

2004

We have used normal metal-insulator-superconductor (NIS) tunnel junction pairs, known as SINIS structures, for ultrasensitive thermometry at sub-Kelvin temperatures. With the help of these thermometers, we have developed an ac-technique to measure the electron-phonon (e-p) scattering rate directly, without any other material or geometry dependent parameters, based on overheating the electron gas. The technique is based on Joule heating the electrons in the frequency range DC-10 MHz, and measuring the electron temperature in DC. Because of the nonlinearity of the electron-phonon coupling with respect to temperature, even the DC response will be affected, when the heating frequency reaches th…

PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsCondensed Matter - SuperconductivityFOS: Physical scienceschemistry.chemical_element02 engineering and technologyElectron021001 nanoscience & nanotechnology01 natural sciencesCopperSuperconductivity (cond-mat.supr-con)chemistryTunnel junctionScattering rateMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciencesElectron temperature010306 general physics0210 nano-technologyJoule heatingFermi gasOverheating (electricity)physica status solidi (c)
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Electron-phonon interaction in thin copper and gold films

2004

We have studied the electron-phonon (e-p) interaction in thin Cu and Au films at sub-Kelvin temperatures with the help of the hot electron effect, using symmetric normal metal-insulator-superconductor tunnel junction pairs as thermometers. By Joule heating the electron gas and measuring the electron and the lattice temperatures simultaneously, we show that the electron-phonon scattering rate follows a $T^{4}$ temperature dependence in both metals. The result is in accordance with the theory of e-p scattering in disordered films with vibrating boudaries and impurities, in contrast to the $T^{3}$-law expected for pure samples, and $T^{2}$-law for static disorder.

PhysicsCondensed matter physicsCondensed Matter - Mesoscale and Nanoscale PhysicsScatteringCondensed Matter - Superconductivitychemistry.chemical_elementFOS: Physical sciencesElectronCondensed Matter::Mesoscopic Systems and Quantum Hall Effect01 natural sciencesCopper010305 fluids & plasmasSuperconductivity (cond-mat.supr-con)chemistryImpurityTunnel junctionScattering rateCondensed Matter::Superconductivity0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)Condensed Matter::Strongly Correlated Electrons010306 general physicsFermi gasJoule heating
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Magnetostrictive and quadrupolar anisotropy in nuclear magnetic fcc systems

1992

The spin hamiltonian for nuclear magnetic order in copper is investigated with respect to magnetoelastic couplings to the lattice. These arise due to the dipolar, Ruderman Kittel and the quadrupolar interaction. While the latter is quenched for the ideal fcc-lattice, it is found that for copper it will dominate the magnetoelastic terms of the nuclear spin hamiltonian. The absolute size of the quadrupole contribution is determined by the effective charge and (anti-) shielding effects. This interaction can give rise to an effective anisotropy in the fcc-system which can be quite large compared to the small stabilisation energies for nuclear order in copper. Consequences for the nuclear orderi…

PhysicsCondensed matter physicschemistry.chemical_elementMagnetostrictionCondensed Matter PhysicsCopperEffective nuclear chargeElectronic Optical and Magnetic MaterialsCondensed Matter::Materials Sciencesymbols.namesakeDipolechemistryElectromagnetic shieldingQuadrupolesymbolsGeneral Materials ScienceHamiltonian (quantum mechanics)AnisotropyZeitschrift f�r Physik B Condensed Matter
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Spin-coupling topology in the copper hexamer compounds A2Cu3O(SO4)3 (A=Na, K)

2020

The compounds ${A}_{2}\mathrm{C}{\mathrm{u}}_{3}\mathrm{O}{(\mathrm{S}{\mathrm{O}}_{4})}_{3}$ $(A=\mathrm{Na},\phantom{\rule{0.16em}{0ex}}\mathrm{K})$ are characterized by copper hexamers that are weakly coupled to realize antiferromagnetic order below ${T}_{N}\ensuremath{\approx}3\phantom{\rule{0.16em}{0ex}}\mathrm{K}$. They constitute quantum spin systems with $S=1$ triplet ground states. We investigated the energy-level splittings of the copper hexamers by inelastic neutron scattering experiments covering the entire range of the magnetic excitation spectra. The observed transitions are governed by very unusual selection rules that we ascribe to the underlying spin-coupling topology. This…

PhysicsExcitation spectrachemistry.chemical_elementOrder (ring theory)Coupling topology02 engineering and technologyRandom hexamer021001 nanoscience & nanotechnology01 natural sciencesCopperInelastic neutron scatteringCrystallographychemistry0103 physical sciencesAntiferromagnetism010306 general physics0210 nano-technologySpin (physics)Physical Review B
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In-source laser spectroscopy of75,77,78Cu: Direct evidence for a change in the quasiparticle energy sequence in75,77Cu and an absence of longer-lived…

2011

This paper describes measurements on the isotopes (75,77,78)Cu by the technique of in-source laser spectroscopy, at the ISOLDE facility, CERN. The role of this technique is briefly discussed in the ...

PhysicsMass numberNuclear and High Energy PhysicsQuantitative Biology::Neurons and CognitionIsotopeMagnetic momentIsotopes of copperStable isotope ratioIsotope separationlaw.inventionlawQuasiparticlePhysics::Accelerator PhysicsPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentSpectroscopyPhysical Review C
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Investigation of beta strength functions by neutron and gamma-ray spectroscopy

1979

Abstract Neutron spectra from the decay of the β− delayed neutron precursors 55.6 sec 87Br, 24.5 sec 137I, 2.05 sec 85As and 1.71 sec 135Sb have been studied with high resolution 3He ionization chambers. By γ-ray measurements, the partial neutron emission probabilities to excited states in 84Se and 134Te have been determined independently. For the neutron-emitter nuclei 87Kr and 137Xe, from which neutron decay proceeds only to the ground states of the final nuclei, 86Kr and 136Xe, unique information on the shape of the β− strength function Sβ(E) is obtained. For the emitter nuclei 85Se and 135Te, correlations between neutron transition energies and differences in level energies in 84Se and …

PhysicsNuclear and High Energy PhysicsIsotopes of copperNeutron emissionNuclear TheoryNuclear physicsIonizationGiant resonanceNeutronGamma spectroscopyAtomic physicsNuclear Experiments-processDelayed neutronNuclear Physics A
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Production of the charmed baryon $\Lambda_{c}^{+}$ in $\pi^{-}$Cu and K$^{-}$Cu interactions at 230 GeV

1990

Abstract We present results from the NA32 experiment at CERN on the production characteristics of the charmed baryon Λ+c in 230 GeV π−Cu and K−Cu interactions. A high resolution vertex detector consisting of change-coupled devices and silicon microstrip detectors allowed the selection of a very clean sample of 154 Λ+c → pK−π+ (and charge conjugate) decays. Results on differential and integrated cross sections are given.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsResolution (electron density)chemistry.chemical_elementCharge (physics)CopperBaryonNuclear physicschemistryHigh Energy Physics::ExperimentProduction (computer science)Vertex detectorNuclear ExperimentSilicon microstrip detectorsParticle Physics - Experiment
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