Search results for "Coupling"

showing 10 items of 1862 documents

Low-lying shears bands in very light odd—odd Bi isotopes

2003

The concept of magnetic rotation in nuclei was introduced to explain the observed regular bands with enhanced M1 transitions and weak or absent E2 crossover transitions in nearly spherical nuclei around 198Pb [1]. These bands can be described by the coupling of high-j proton and neutron configurations to a total spin tilted at an angle of ~ 45° with respect to the symmetry axis. As the proton and neutron spins align with increasing excitation energy, a sequence of ΔI = 1 levels of fixed parity (“shears band”) is formed [2].

CouplingPhysicsProtonSpins010308 nuclear & particles physicsNuclear TheoryParity (physics)01 natural sciencesSymmetry (physics)0103 physical sciencesNeutronAtomic physicsNuclear Experiment010306 general physicsSpin (physics)Excitation
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Shuttling of Rydberg ions for fast entangling operations

2019

We introduce a scheme to entangle Rydberg ions in a linear ion crystal, using the high electric polarizability of the Rydberg electronic states in combination with mutual Coulomb coupling of ions that establishes common modes of motion. After laser-initialization of ions to a superposition of ground- and Rydberg-state, the entanglement operation is driven purely by applying a voltage pulse that shuttles the ion crystal back and forth. This operation can achieve entanglement on a sub-$\mu$s timescale, more than two orders of magnitude faster than typical gate operations driven by continuous-wave lasers. Our analysis shows that the fidelity achieved with this protocol can exceed $99.9\%$ with…

CouplingPhysicsQuantum PhysicsAtomic Physics (physics.atom-ph)General Physics and AstronomyFOS: Physical sciencesQuantum entanglementQuantum Physics7. Clean energy01 natural sciencesIonPhysics - Atomic PhysicsSuperposition principlesymbols.namesakeOrders of magnitude (time)Polarizability0103 physical sciencesRydberg formulasymbolsCoulombPhysics::Atomic PhysicsAtomic physics010306 general physicsQuantum Physics (quant-ph)
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Quantum simulation of the spin-boson model with a microwave circuit

2017

We consider superconducting circuits for the purpose of simulating the spin-boson model. The spin-boson model consists of a single two-level system coupled to bosonic modes. In most cases, the model is considered in a limit where the bosonic modes are sufficiently dense to form a continuous spectral bath. A very well known case is the ohmic bath, where the density of states grows linearly with the frequency. In the limit of weak coupling or large temperature, this problem can be solved numerically. If the coupling is strong, the bosonic modes can become sufficiently excited to make a classical simulation impossible. Here, we discuss how a quantum simulation of this problem can be performed …

CouplingPhysicsQuantum PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed Matter - SuperconductivityFOS: Physical sciencesQuantum simulator01 natural sciences010305 fluids & plasmasSuperconductivity (cond-mat.supr-con)ResonatorCircuit quantum electrodynamicsQuantum mechanicsQubitQuantum electrodynamicsMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciencesDensity of statesQuantum Physics (quant-ph)010306 general physicsBosonSpin-½
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Array of planar Penning traps as a nuclear magnetic resonance molecule for quantum computation

2005

An array of planar Penning traps, holding single electrons, can realize an artificial molecule suitable for NMR-like quantum information processing. The effective spin-spin coupling is accomplished by applying a magnetic field gradient, combined to the Coulomb interaction acting between the charged particles. The system lends itself to scalability, since the same substrate can easily accommodate an arbitrary number of traps. Moreover, the coupling strength is tunable and under experimental control. Our theoretical predictions take into account a realistic setting, within the reach of current technology.

CouplingPhysicsQuantum PhysicsFOS: Physical sciencesElectronPenning trapAtomic and Molecular Physics and OpticsCharged particleMagnetic fieldNuclear magnetic resonancePlanarAtomic physicsQuantum informationQuantum Physics (quant-ph)Quantum computerPhysical Review A
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Search for flavor changing neutral currents in decays of top quarks

2011

We present a search for flavor changing neutral currents in decays of top quarks. The analysis is based on a search for ttbar -> l'null + jets (l, l' = e, mu) final states using 4.1 fb^-1 of integrated luminosity of ppbar collisions at sqrt(s) = 1.96 TeV. We extract limits on the branching ratio B(t -> Zq) (q = u, c quarks), assuming anomalous tuZ or tcZ couplings. We do not observe any sign of such anomalous coupling and set a limit of B < 3.2% at 95% C.L.

CouplingPhysicsQuarkNuclear and High Energy PhysicsTop quarkParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsBranching fractionFlavor-changing neutral currentHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSING[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experiment010306 general physicsSign (mathematics)
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Measurements of relative line strengths in N I multiplets for transition arrays 3s–np (n=3, 4, 5)

2008

Abstract Applying the emission method, intensities of 60 spectral lines of neutral nitrogen (N I) belonging to 15 multiplets originating from 3s–np (n=3, 4, 5) transition arrays have been measured. A wall-stabilized arc, operated at atmospheric pressure in helium with some admixture of nitrogen was applied as the excitation source. From measured line intensities, relative line strengths within multiplets have been evaluated. For transitions with Δn=1 and 2, significantly larger discrepancies from LS coupling results are found if compared to transitions 3s–3p (Δn=0). The measured relative line strengths within 3s–3p multiplets are compared with older measurements, recent calculations and wit…

CouplingPhysicsRadiationAtmospheric pressurechemistry.chemical_elementNitrogenAtomic and Molecular Physics and OpticsSpectral linechemistryAtomic physicsSpectroscopyExcitationHeliumLine (formation)Journal of Quantitative Spectroscopy and Radiative Transfer
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Purcell factor for 3D- dipolar emitter coupling to 2D- plasmonic waveguides

2011

We theoretically investigate spontaneous emission of a quantum (3D) dipolar emitter located near a (2D) plasmonic waveguide of arbitrary form. The channels into which emitter couples (plasmon, scattering, electron-hole pairs creation) are well identified.

CouplingPhysicsScatteringbusiness.industrySurface plasmonCavity quantum electrodynamicsPhysics::OpticsSurface plasmon polaritonPhysics::Accelerator PhysicsOptoelectronicsSpontaneous emissionbusinessPlasmonCommon emitter2011 Conference on Lasers and Electro-Optics Europe and 12th European Quantum Electronics Conference (CLEO EUROPE/EQEC)
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Search for anomalous Wtb couplings in single top quark production

2008

Made available in DSpace on 2022-04-28T20:46:40Z (GMT). No. of bitstreams: 0 Previous issue date: 2008-11-25 Science and Technology Facilities Council In 0.9fb-1 of pp̄ collisions, the D0 Collaboration presented evidence for single top quark production in events with an isolated lepton, missing transverse momentum, and two to four jets. We examine these data to study the Lorentz structure of the Wtb coupling. The standard model predicts a left-handed vector coupling at the Wtb vertex. The most general lowest dimension, CP-conserving Lagrangian admits right-handed vector and left- or right-handed tensor couplings as well. We find that the data prefer the left-handed vector coupling and set u…

CouplingPhysicsTop quarkParticle physics010308 nuclear & particles physicsLorentz transformationGeneral Physics and Astronomy01 natural sciencesVertex (geometry)symbols.namesake0103 physical sciencesTransverse momentumsymbols010306 general physicsLagrangianLeptonPhysical Review Letters
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Acousto-optic cavity coupling in 2D phoxonic crystal with combined convex and concave holes

2021

International audience; A two-dimensional cross-like phoxonic crystal (PxC) model is proposed, which exhibits simultaneously large complete photonic crystal (PtC) and phononic crystal (PnC) bandgaps. The most salient trait of the structure is the wide range of geometrical parameters compatible with large complete bandgaps. After geometrical optimization, photonic and phononic bandgaps with gap-to-midgap ratios of 11.5% and 90.7% are obtained, respectively. These values are close to the best topology-optimized reported values but are obtained with simple shapes compatible with nanoscale fabrication technology. These characteristics make the convex–concave topology a promising candidate for P…

CouplingPhysics[SPI.ACOU]Engineering Sciences [physics]/Acoustics [physics.class-ph]PhotonCondensed matter physicsPhononbusiness.industryGeneral Physics and AstronomyPhysics::Optics02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesFinite element method[SPI.MAT]Engineering Sciences [physics]/MaterialsCrystalSuperposition principle0103 physical sciencesPhotonics[SPI.NANO]Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics010306 general physics0210 nano-technologybusinessPhotonic crystal
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Coupling of lattice-Boltzmann solvers with suspended particles using the MPI intercommunication framework

2017

Abstract The MPI intercommunication framework was used for coupling of two lattice-Boltzmann solvers with suspended particles, which model advection and diffusion respectively of these particles in a carrier fluid. Simulation domain was divided into two parts, one with advection and diffusion, and the other with diffusion only (no macroscopic flow). Particles were exchanged between these domains at their common boundary by a direct process to process communication. By analysing weak and strong scaling, it was shown that the linear scaling characteristics of the lattice-Boltzmann solvers were not compromised by their coupling.

CouplingPhysicsadvection-diffusionta114AdvectionGeneral EngineeringLattice Boltzmann methods01 natural sciences010305 fluids & plasmasPhysics::Fluid DynamicsFlow (mathematics)0103 physical sciencesFluid dynamicsLinear scaleMPIStatistical physicsDiffusion (business)coupling010306 general physicsScalingSoftwareLattice-BoltzmannAdvances in Engineering Software
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