Search results for "quantum gases"

showing 10 items of 650 documents

Finite-size scaling of the quark condensate in quenched lattice QCD

1999

We confront the finite volume and small quark mass behaviour of the scalar condensate, determined numerically in quenched lattice QCD using Neuberger fermions, with predictions of quenched chiral perturbation theory. We find that quenched chiral perturbation theory describes the numerical data well, allowing us to extract the infinite volume, chiral limit scalar condensate, up to a multiplicative renormalization constant.

QuarkPhysicsCondensed Matter::Quantum GasesNuclear and High Energy PhysicsChiral perturbation theoryFinite volume methodHigh Energy Physics::LatticeScalar (mathematics)High Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciencesParticle Physics - LatticeFermionLattice QCDRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)ScalingMathematical physics
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One-Loop Self Energy and Renormalization of the Speed of Light for some Anisotropic Improved Quark Actions

2000

One-loop corrections to the fermion rest mass M_1, wave function renormalization Z_2 and speed of light renormalization C_0 are presented for lattice actions that combine improved glue with clover or D234 quark actions and keep the temporal and spatial lattice spacings, a_t and a_s, distinct. We explore a range of values for the anisotropy parameter \chi = a_s/a_t and treat both massive and massless fermions.

QuarkPhysicsCondensed Matter::Quantum GasesNuclear and High Energy PhysicsWave function renormalizationParticle physicsHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesFermionRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeSelf-energyLattice gauge theoryInvariant mass
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Time-dependent resonance interaction energy between two entangled atoms under nonequilibrium conditions

2018

We consider the time-dependent resonance interaction energy between two identical atoms, one in the ground state and the other in an excited state, and interacting with the vacuum electromagnetic field, during a nonequilibrium situation such as the dynamical atomic self-dressing process. We suppose the two atoms prepared in a correlated, symmetric or antisymmetric, state. Since the atoms start from a nonequilibrium conditions, their interaction energy is time dependent. We obtain, at second order in the atom-field coupling, an analytic expression for the time-dependent resonance interaction energy between the atoms. We show that this interaction vanishes when the two atoms are outside the l…

Resonance interaction Casimir-Polder effect non equilibrium systems.High Energy Physics - TheoryCondensed Matter::Quantum GasesElectromagnetic fieldPhysicsQuantum PhysicsField (physics)Antisymmetric relationFOS: Physical sciencesNon-equilibrium thermodynamicsInteraction energy01 natural sciencesResonance (particle physics)010305 fluids & plasmasHigh Energy Physics - Theory (hep-th)Excited state0103 physical sciencesPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsAtomic physicsQuantum Physics (quant-ph)010306 general physicsGround statePhysical Review A
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Tunable Polarons in Bose-Einstein Condensates

2017

A toolbox for the quantum simulation of polarons in ultracold atoms is presented. Motivated by the impressive experimental advances in the area of ultracold atomic mixtures, we theoretically study the problem of ultracold atomic impurities immersed in a Bose-Einstein condensate mixture (BEC). The coupling between impurity and BEC gives rise to the formation of polarons whose mutual interaction can be effectively tuned using an external laser driving a quasi-resonant Raman transition between the BEC components. Our scheme allows one to change the effective interactions between polarons in different sites from attractive to zero. This is achieved by simply changing the intensity and the frequ…

ScienceFOS: Physical sciencesQuantum simulatorPolaron01 natural sciencesSettore FIS/03 - Fisica Della MateriaArticle010305 fluids & plasmaslaw.inventionsymbols.namesakeImpurityUltracold atomlaw/dk/atira/pure/subjectarea/asjc/10000103 physical sciencesPhysics::Atomic PhysicsGeneral010306 general physicsCondensed Matter::Quantum GasesPhysicsQuantum PhysicsMultidisciplinaryCondensed Matter::OtherPolaronsQRLaser3. Good healthCoupling (physics)Quantum Gases (cond-mat.quant-gas)symbolsMultidisciplinary ultracold atoms polaronsMedicine-----Atomic physicsCondensed Matter - Quantum GasesQuantum Physics (quant-ph)Raman spectroscopyBose–Einstein condensateScientific Reports
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Isotope dependence of the Zeeman effect in lithium-like calcium

2016

The magnetic moment μ of a bound electron, generally expressed by the g-factor μ=−g μB s ħ−1 with μB the Bohr magneton and s the electron's spin, can be calculated by bound-state quantum electrodynamics (BS-QED) to very high precision. The recent ultra-precise experiment on hydrogen-like silicon determined this value to eleven significant digits, and thus allowed to rigorously probe the validity of BS-QED. Yet, the investigation of one of the most interesting contribution to the g-factor, the relativistic interaction between electron and nucleus, is limited by our knowledge of BS-QED effects. By comparing the g-factors of two isotopes, it is possible to cancel most of these contributions an…

ScienceGeneral Physics and Astronomychemistry.chemical_elementElectron01 natural sciencesGeneral Biochemistry Genetics and Molecular BiologyArticle010305 fluids & plasmasIonBohr magnetonsymbols.namesakeRecoilNuclear magnetic resonance0103 physical sciencesPhysics::Atomic Physics010306 general physicsSpin (physics)Nuclear ExperimentPhysicsCondensed Matter::Quantum GasesMultidisciplinaryZeeman effectMagnetic momentQGeneral ChemistrychemistrysymbolsLithiumddc:500Präzisionsexperimente - Abteilung BlaumAtomic physicsNature Communications
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Seed‐Layer‐Free Atomic Layer Deposition of Highly Uniform Al 2 O 3 Thin Films onto Monolayer Epitaxial Graphene on Silicon Carbide

2019

Atomic layer deposition (ALD) is the method of choice to obtain uniform insulating films on graphene for device applications. Owing to the lack of out-of-plane bonds in the sp(2) lattice of graphene, nucleation of ALD layers is typically promoted by functionalization treatments or predeposition of a seed layer, which, in turn, can adversely affect graphene electrical properties. Hence, ALD of dielectrics on graphene without prefunctionalization and seed layers would be highly desirable. In this work, uniform Al2O3 films are obtained by seed-layer-free thermal ALD at 250 degrees C on highly homogeneous monolayer (1L) epitaxial graphene (EG) (amp;gt;98% 1L coverage) grown on on-axis 4H-SiC(00…

SiCMaterials sciencePhysics::Opticslaw.inventionchemistry.chemical_compoundAtomic layer depositionlawLattice (order)MonolayerPhysics::Atomic and Molecular ClustersSilicon carbidePhysics::Chemical PhysicsThin filmCondensed Matter::Quantum Gasesatomic force microscopybusiness.industryAtomic force microscopyGrapheneMechanical EngineeringCondensed Matter Physicsepitaxial graphenechemistryMechanics of Materialsatomic layer depositionOptoelectronicsatomic force microscopy; atomic layer deposition; epitaxial graphene; SiCEpitaxial graphenebusinessDen kondenserade materiens fysikAdvanced Materials Interfaces
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Experimental Realization of a Dirac Monopole through the Decay of an Isolated Monopole

2017

We experimentally observe the decay dynamics of deterministically created isolated monopoles in spin-1 Bose-Einstein condensates. As the condensate undergoes a change between magnetic phases, the isolated monopole gradually evolves into a spin configuration hosting a Dirac monopole in its synthetic magnetic field. We characterize in detail the Dirac monopole by measuring the particle densities of the spin states projected along different quantization axes. Importantly, we observe the spontaneous emergence of nodal lines in the condensate density that accompany the Dirac monopole. We also demonstrate that the monopole decay accelerates in weaker magnetic field gradients.

Spin statesmagneetitHigh Energy Physics::LatticeQC1-999Magnetic monopoleFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciences010305 fluids & plasmasQuantization (physics)Atomic and Molecular Physics0103 physical sciences010306 general physicskvanttifysiikkamagnetsSpin-½PhysicsCondensed Matter::Quantum Gasesta114PhysicsMagnetic field gradientMagnetic fieldQuantum Gases (cond-mat.quant-gas)quantum physicsQuantum electrodynamicsParticleCondensed Matter - Quantum GasesRealization (systems)Physical Review X
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Use of supercritical CO2 and N2 as dissolved gases for the atomization of ethanol and water

2012

Supercritical dissolved gas atomization (SDGA) is an atomization process in which a gas at temperatures and pressures above the critical point is used as the atomizing medium. The concept of SDGA has been applied mainly using CO 2 as atomizing gas in various processes developed for the production of fine particles of pharmaceuticals, polymers, and chemical products and for the atomization of fuels. In this work, SDGA, using ethanol and water as the liquids to be atomized, has been experimentally studied. The spray characteristics, in terms of droplet size and distribution, have been investigated using a laser diffraction analyzer. Ethanol has been chosen due to the large miscibility with CO…

Spray characteristicsGeneral Chemical EngineeringAnalytical chemistryMiscibilityLaser diffractionIndustrial and Manufacturing EngineeringPhysics::Fluid DynamicsGas to liquidschemistry.chemical_compoundAtomizing gas Dissolved gas Droplet sizes Fine particles Gas to liquids Laser diffraction Supercritical fluids Supercritical CO2Fine particlesCritical point (thermodynamics)Gas to liquidsPhysics::Atomic and Molecular ClustersChemical Engineering (all)Physics::Atomic PhysicsDissolved gasCondensed Matter::Quantum Gaseschemistry.chemical_classificationAtomizing gasSupercritical fluidsChemistry (all)Droplet sizesGeneral ChemistryPolymerSupercritical CO2Supercritical fluidCondensed Matter::Soft Condensed MatterSolventchemistryCarbon dioxide
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Measurements of Higgs boson production and couplings in diboson final states with the ATLAS detector at the LHC

2013

We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWF and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC and NSRF, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, DFG, HGF, MPG and AvH Foundation, Germany; GSRT and NSRF, Greece; ISF, MINERVA, GIF, DIP and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; BRF and RCN, Norway; MNiSW, Poland; GRICES and FCT, Portu…

Standard Modeldilepton: mass spectrumCiencias Físicas01 natural sciences7. Clean energySettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentHiggs particle: hadroproduction//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)vector boson: fusion[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]QCBosonPhysicsHIGGS BOSONLarge Hadron Collidervector boson: pair productiontransverse energy: missing-energy4. EducationATLAS experimentSettore FIS/01 - Fisica SperimentaleATLAS3. Good healthMassless particleCERN LHC CollHiggs particle: massPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs boson7000: 8000 GeV-cmsFísica nuclearAtlasLhcNeutrinoHiggs particle: decay modesParticle Physics - ExperimentCIENCIAS NATURALES Y EXACTASp p: scatteringNuclear and High Energy PhysicsParticle physicsmass spectrum: (4lepton)530 PhysicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2ATLASdetector; LHC; Higgsbosonproduction; diboson530Massless ParticlesNnlo QCDNuclear physics0103 physical sciencesFysikddc:530High Energy Physics010306 general physicsTransverse-MomentumCondensed Matter::Quantum GasesHiggs particle: couplingScience & Technologyhep-ex010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaQCD CorrectionsFermion//purl.org/becyt/ford/1.3 [https]Hadron CollidersDiboson ProductionAstronomíavector boson: leptonic decayHADRON-HADRON COLLISIONSProton-Proton CollisionsRoot-S=7 TevHiggs particle: hadroproduction ; Higgs particle: coupling ; vector boson: fusion ; p p: scattering ; CERN LHC Coll ; ATLAS ; Higgs particle: decay modes ; vector boson: pair production ; vector boson: leptonic decay ; mass spectrum: two-photon ; mass spectrum: (4lepton) ; dilepton: mass spectrum ; transverse energy: missing-energy ; Higgs particle: mass ; experimental results ; 7000: 8000 GeV-cmsExperimental High Energy PhysicsHigh Energy Physics::ExperimentCross-Sectionsmass spectrum: two-photonexperimental resultsLeptonBroken Symmetries
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Form factor approach to dynamical correlation functions in critical models

2012

We develop a form factor approach to the study of dynamical correlation functions of quantum integrable models in the critical regime. As an example, we consider the quantum non-linear Schr\"odinger model. We derive long-distance/long-time asymptotic behavior of various two-point functions of this model. We also compute edge exponents and amplitudes characterizing the power-law behavior of dynamical response functions on the particle/hole excitation thresholds. These last results confirm predictions based on the non-linear Luttinger liquid method. Our results rely on a first principles derivation, based on the microscopic analysis of the model, without invoking, at any stage, some correspon…

Statistics and ProbabilityHigh Energy Physics - TheoryIntegrable systemMinor (linear algebra)[PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph]FOS: Physical sciences01 natural sciencesGapless playbackLuttinger liquid0103 physical sciencesLieb–Liniger model[NLIN.NLIN-SI]Nonlinear Sciences [physics]/Exactly Solvable and Integrable Systems [nlin.SI]Statistical physics010306 general physicsQuantumMathematical PhysicsPhysicsQuantum PhysicsNonlinear Sciences - Exactly Solvable and Integrable Systems010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]Form factor (quantum field theory)Statistical and Nonlinear PhysicsMathematical Physics (math-ph)AmplitudeHigh Energy Physics - Theory (hep-th)Quantum Gases (cond-mat.quant-gas)Statistics Probability and UncertaintyExactly Solvable and Integrable Systems (nlin.SI)Quantum Physics (quant-ph)Condensed Matter - Quantum Gases
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