Search results for "Quasiparticle"

showing 10 items of 280 documents

Giant, unconventional anomalous Hall effect in the metallic frustrated magnet candidate, KV 3 Sb 5

2020

The anomalous Hall effect soars when Dirac quasiparticles meet frustrated magnetism.

02 engineering and technology01 natural sciencesCondensed Matter::Materials ScienceHall effectCondensed Matter::Superconductivity0103 physical sciencesAstrophysics::Solar and Stellar Astrophysics010306 general physicsAstrophysics::Galaxy AstrophysicsResearch ArticlesPhysicsMultidisciplinaryCondensed matter physicsScatteringDirac (video compression format)PhysicsSciAdv r-articles021001 nanoscience & nanotechnologyCondensed Matter::Mesoscopic Systems and Quantum Hall EffectSemimetalFerromagnetismMagnetQuasiparticleSpin Hall effectCondensed Matter::Strongly Correlated Electrons0210 nano-technologyResearch ArticleScience Advances
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Space-borne Bose–Einstein condensation for precision interferometry

2018

Space offers virtually unlimited free-fall in gravity. Bose-Einstein condensation (BEC) enables ineffable low kinetic energies corresponding to pico- or even femtokelvins. The combination of both features makes atom interferometers with unprecedented sensitivity for inertial forces possible and opens a new era for quantum gas experiments. On January 23, 2017, we created Bose-Einstein condensates in space on the sounding rocket mission MAIUS-1 and conducted 110 experiments central to matter-wave interferometry. In particular, we have explored laser cooling and trapping in the presence of large accelerations as experienced during launch, and have studied the evolution, manipulation and interf…

Atomic Physics (physics.atom-ph)FOS: Physical sciencesSpace (mathematics)01 natural sciencesPhysics - Atomic Physicslaw.invention010309 opticslawLaser cooling0103 physical sciencesAstronomical interferometer010306 general physicsQuantumCondensed Matter::Quantum GasesPhysicsMultidisciplinaryBragg's lawinterferometryBose-EinsteinComputational physicsInterferometryQuantum Gases (cond-mat.quant-gas)QuasiparticleAtomic physicsCondensed Matter - Quantum GasesBose–Einstein condensateNature
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Spectral function for overoccupied gluodynamics from real-time lattice simulations

2018

We study the spectral properties of a highly occupied non-Abelian non-equilibrium plasma appearing ubiquitously in weak coupling descriptions of QCD matter. The spectral function of this far-from-equilibrium plasma is measured by employing linear response theory in classical-statistical real-time lattice Yang-Mills simulations. We establish the existence of transversely and longitudinally polarized quasiparticles and obtain their dispersion relations, effective mass, plasmon frequency, damping rate and further structures in the spectral and statistical functions. Our new method can be interpreted as a non-perturbative generalization of hard thermal loop (HTL) effective theory. We see indica…

CLASSICAL APPROXIMATIONNuclear Theorynucl-thquark-gluon plasmahep-latFOS: Physical sciencesHEAVY-ION COLLISIONShiukkasfysiikka114 Physical sciences01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)0103 physical sciencesquantum chromodynamicsQCD PLASMA INSTABILITIESStatistical physicsGauge theorynonperturbative effects in field theory010306 general physicsHARD THERMAL LOOPSParticle Physics - PhenomenologyPhysicsQuantum chromodynamicsta114010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)kvarkki-gluoniplasmafinite temperature field theorylattice field theoryISOTROPIZATIONParticle Physics - Latticehep-ph16. Peace & justiceFIELD-THEORYGluonHigh Energy Physics - PhenomenologyNuclear Physics - TheoryQuark–gluon plasmaHIGH-TEMPERATUREGAUGE-THEORIESQuasiparticleSpectral functionkvanttikenttäteoriaStatistical correlationrelativistic heavy-ion collisions
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Surface-plasmon hopping along coupled coplanar cavities

2007

International audience; We report on surface-plasmon propagation along coupled coplanar cavities periodically distributed in an otherwise unperturbed plasmonic crystal. We show that the dispersion of particular Bloch modes can exhibit multiple energy gaps that can be adjusted by choosing the cavity size. For resonant sizes, the composite crystals composed of juxtaposed cavities can support plasmon modes at frequencies within the gap of the unperturbed grating. In this case, we demonstrate that the surface-plasmon propagation relies on a hopping mechanism.

Cavity sizePhysics::Optics02 engineering and technologyGrating01 natural sciencesMolecular physicsCrystalOptics0103 physical sciencesDispersion (optics)[SPI.NANO]Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics010306 general physicsComputer Science::DatabasesPlasmonPhysics[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]business.industrySurface plasmon021001 nanoscience & nanotechnologyCondensed Matter PhysicsElectronic Optical and Magnetic Materials[SPI.OPTI]Engineering Sciences [physics]/Optics / PhotonicQuasiparticle[ SPI.NANO ] Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics[ SPI.OPTI ] Engineering Sciences [physics]/Optics / Photonic0210 nano-technologybusinessPhysical Review B
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Noise correlations of the ultracold Fermi gas in an optical lattice

2008

In this paper we study the density noise correlations of the two component Fermi gas in optical lattices. Three different type of phases, the BCS-state (Bardeen, Cooper, and Schieffer), the FFLO-state (Fulde, Ferrel, Larkin, and Ovchinnikov), and BP (breach pair) state, are considered. We show how these states differ in their noise correlations. The noise correlations are calculated not only at zero temperature, but also at non-zero temperatures paying particular attention to how much the finite temperature effects might complicate the detection of different phases. Since one-dimensional systems have been shown to be very promising candidates to observe FFLO states, we apply our results als…

ComputationFOS: Physical sciencesradiation pressure01 natural sciences010305 fluids & plasmaslaser coolingfermion systemsLattice (order)Laser coolingQuantum mechanicsCondensed Matter::Superconductivity0103 physical sciencesoptical lattices010306 general physicsPhysicsCondensed Matter::Quantum GasesOptical latticeCondensed matter physicsBCS theoryBCS theoryAtomic and Molecular Physics and OpticsCondensed Matter - Other Condensed MatterRadiation pressureQuasiparticleFermi gasOther Condensed Matter (cond-mat.other)
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Realistic investigations of correlated electron systems with LDA + DMFT

2006

Conventional band structure calculations in the local density approximation (LDA) [1–3] are highly successful for many materials, but miss important aspects of the physics and energetics of strongly correlated electron systems, such as transition metal oxides and f-electron systems displaying, e.g., Mott insulating and heavy quasiparticle behavior. In this respect, the LDA + DMFT approach which merges LDA with a modern many-body approach, the dynamical mean-field theory (DMFT), has proved to be a breakthrough for the realistic modeling of correlated materials. Depending on the strength of the electronic correlation, a LDA + DMFT calculation yields the weakly correlated LDA results, a strong…

Condensed Matter::Quantum GasesCondensed matter physicsHubbard modelElectronic correlationChemistryMott insulatorQuantum Monte CarloCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsQuasiparticleCondensed Matter::Strongly Correlated ElectronsStrongly correlated materialddc:530Metal–insulator transitionLocal-density approximation
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Roton-roton crossover in strongly correlated dipolar Bose-nonstnon condensates

2011

We study the pair correlations and excitations of a dipolar Bose gas layer. The anisotropy of the dipole-dipole interaction allows us to tune the strength of pair correlations from strong to weak perpendicular and weak to strong parallel to the layer by increasing the perpendicular trap frequency. This change is accompanied by a roton-roton crossover in the spectrum of collective excitations, from a roton caused by the head-to-tail attraction of dipoles to a roton caused by the side-by-side repulsion, while there is no roton excitation for intermediate trap frequencies. We discuss the nature of these two kinds of rotons and the relation to instabilities of dipolar Bose gases. In both regime…

Condensed Matter::Quantum GasesPhysicsCondensed matter physicsBose gasta114Condensed Matter::OtherGeneral Physics and AstronomyCondensed Matter::Mesoscopic Systems and Quantum Hall EffectRotonlaw.inventionDipolelawQuasiparticleElectric dipole transitionAnisotropyExcitationBose–Einstein condensatePhysical Review Letters
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Fermion Condensation in Finite Systems

2014

Here we consider another example of systems, in which fermion condensation takes place. These are what is called finite Fermi systems, i.e. systems with finite number of fermions, contrary to a solid, where the number of electrons is practically infinite. An example of a finite Fermi system is an atomic nucleus, having finite number of nucleons, protons and neutrons, which are fermions. Here we show that the fermion condensation manifests itself in finite Fermi systems as a forced merger of all, discreet for finite systems, single-particle levels, lying near the Fermi surface. On the first sight, this merger contradicts the standard Landau quasiparticle picture. Nevertheless, similar to inf…

Condensed Matter::Quantum GasesPhysicsFermion doublingTheoretical physicsAtomic nucleusQuasiparticleFermi surfaceFermionFermi liquid theoryLandau quantizationSpin-½
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The electron gas with short coherence length pairs: how to approach the stronger coupling limit?

2001

Abstract The attractive Hubbard model is investigated in 2D using a T -matrix approach. In a self-consistent calculation pairs as infinite lifetime Bosons only exist in the atomic limit and therefore a Fermi surface can be investigated also in the stronger coupling regime. A heavy quasiparticle peak with a weak dispersion crosses the Fermi surface at k F whereas light, single particle excitations do only exist far away from the Fermi surface. At low temperatures there seem to exist different self-consistent solutions. In one of them a pseudogap opens even in the integrated density of states. In the present work accurate k -dependent and k -integrated spectral quantities for a 2D finite latt…

Condensed Matter::Quantum GasesPhysicsHubbard modelCondensed matter physicsEnergy Engineering and Power TechnologyFermi surfaceCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCoherence lengthQuasiparticleDensity of statesCondensed Matter::Strongly Correlated ElectronsElectrical and Electronic EngineeringFermi gasPseudogapBosonPhysica C: Superconductivity
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Laser-induced collective excitations in a two-component Fermi gas

2002

We consider the linear density response of a two-component (superfluid) Fermi gas of atoms when the perturbation is caused by laser light. We show that various types of laser excitation schemes can be transformed into linear density perturbations, however, a Bragg spectroscopy scheme is needed for transferring energy and momentum into a collective mode. This makes other types of laser probing schemes insensitive for collective excitations and therefore well suited for the detection of the superfluid order parameter. We show that for the special case when laser light is coupled between the two components of the Fermi gas, density response is always absent in a homogeneous system.

Condensed Matter::Quantum GasesPhysicsLinear densityCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed Matter - SuperconductivityFOS: Physical sciencesEnergy–momentum relationLaserAtomic and Molecular Physics and Opticslaw.inventionSuperconductivity (cond-mat.supr-con)SuperfluiditylawMesoscale and Nanoscale Physics (cond-mat.mes-hall)QuasiparticleAtomic physicsFermi gasSpectroscopyExcitationPhysical Review A
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