Search results for "Quantum Fluctuation"

showing 10 items of 92 documents

Reply to "Comment on 'Dispersion Interaction between Two Hydrogen Atoms in a Static Electric Field' "

2020

In their Comment on our Letter Dispersion Interaction between Two Hydrogen Atoms in a Static Electric Field, P. P. Abrantes et al. address one of the main points discussed in our Letter, that is, the possibility to manipulate interatomic interactions through an external static electric field. In our Letter, we have shown that the interaction between two ground-state atoms can be significantly modified, exploiting an external static electric field, and even turned from attractive to repulsive, depending on the strength of the external field and the geometrical configu- ration. In their Comment, Abrantes et al. point out that it is the electrostatic contribution between the electric dipoles i…

PhysicsSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciHydrogenGeneral Physics and Astronomychemistry.chemical_elementQuantum fluctuationsHydrogen BondingCasimir-Polder interactionMolecular physicschemistryElectricityElectric fieldDispersion (optics)Dispersion interactionHydrogen
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Dynamical Casimir-Polder energy between an excited- and a ground-state atom.

2004

We consider the Casimir-Polder interaction between two atoms, one in the ground state and the other in its excited state. The interaction is time-dependent for this system, because of the dynamical self-dressing and the spontaneous decay of the excited atom. We calculate the dynamical Casimir-Polder potential between the two atoms using an effective Hamiltonian approach. The results obtained and their physical meaning are discussed and compared with previous results based on a time-independent approach which uses a non-normalizable dressed state for the excited atom.

PhysicsSpontaneous decayCondensed Matter::Quantum GasesQuantum Physicsquantum fluctuationsFOS: Physical sciencesquantum electrodynamicExcimerAtomic and Molecular Physics and OpticsCasimir effectsymbols.namesakeQuantum mechanicsExcited stateAtomsymbolsPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsAtomic physicsvan der Waals forceHamiltonian (quantum mechanics)Ground stateDynamical Casimir-Polder forceQuantum Physics (quant-ph)
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Quantum order by disorder in the Kitaev model on a triangular lattice

2015

We identify and discuss the ground state of a quantum magnet on a triangular lattice with bond-dependent Ising-type spin couplings, that is, a triangular analog of the Kitaev honeycomb model. The classical ground-state manifold of the model is spanned by decoupled Ising-type chains, and its accidental degeneracy is due to the frustrated nature of the anisotropic spin couplings. We show how this subextensive degeneracy is lifted by a quantum order-by-disorder mechanism and study the quantum selection of the ground state by treating short-wavelength fluctuations within the linked cluster expansion and by using the complementary spin-wave theory. We find that quantum fluctuations couple next-n…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Topological degeneracyFOS: Physical sciencesCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCondensed Matter Physics; Electronic Optical and Magnetic MaterialsCondensed Matter - Strongly Correlated ElectronsQuantum mechanicsElectronicHexagonal latticeOptical and Magnetic MaterialsGround stateDegeneracy (mathematics)QuantumQuantum fluctuationCluster expansionSpin-½Physical Review B
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Superconductivity in one dimension

2008

Superconducting properties of metallic nanowires can be entirely different from those of bulk superconductors because of the dominating role played by thermal and quantum fluctuations of the order parameter. For superconducting wires with diameters below $ \sim 50$ nm quantum phase slippage is an important process which can yield a non-vanishing wire resistance down to very low temperatures. Further decrease of the wire diameter, for typical material parameters down to $\sim 10$ nm, results in proliferation of quantum phase slips causing a sharp crossover from superconducting to normal behavior even at T=0. A number of interesting phenomena associated both with quantum phase slips and with …

PhysicsSuperconductivityCondensed matter physicsCondensed Matter - SuperconductivityPhysicsNanowireGeneral Physics and AstronomyFOS: Physical sciencesPersistent currentParity (physics)Superconductivity (cond-mat.supr-con)Condensed Matter::SuperconductivityThermalddc:530SlippageQuantumQuantum fluctuation
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Multimode squeezing of frequency combs

2006

We have developed a full multimode theory of a synchronously pumped type-I optical parametric oscillator. We calculate the output quantum fluctuations of the device and find that, in the degenerate case (coincident signal and idler set of frequencies), significant squeezing is obtained when one approaches threshold from below for a set of well-defined ``supermodes,'' or frequency combs, consisting of a coherent linear superposition of signal modes of different frequencies which are resonant in the cavity.

PhysicsSuperposition principleOpticsMulti-mode optical fiberbusiness.industryCoincidentOptical parametric oscillatorPhysics::OpticsbusinessSignalOptical parametric amplifierAtomic and Molecular Physics and OpticsQuantum fluctuationPhysical Review A
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Squeezing induced by spontaneous rotational symmetry breaking

2009

In this communication we study in depth the phenomenon of quadrature squeezing generated via spontaneous rotational symmetry breaking discussed for the first time in [1]. The idea can be put in short as follows. Consider a degenerate optical parametric oscillator (DOPO) tuned to the first family of transverse modes at the signal frequency, and having perfectly spherical mirrors. When pumped above threshold with a Gaussian beam and within a classical description, it is easy to show that a TEM 10 mode with an arbitrary orientation (measured by θ at Fig. 1) emerges at the subharmonic, hence breaking the rotational symmetry of the system in the transverse plane. Quantum effects are then quite i…

PhysicsTransverse planeAngular momentumUncertainty principleQuantum mechanicsQuantum noiseDegenerate energy levelsRotational symmetryQuantum fluctuationGaussian beam
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Beam Energy Scan of Specific Heat Through Temperature Fluctuations in Heavy Ion Collisions

2016

Temperature fluctuations may have two distinct origins, first, quantum fluctuations that are initial state fluctuations, and second, thermodynamical fluctuations. We discuss a method of extracting the thermodynamic temperature from the mean transverse momentum of pions, by using controllable parameters such as centrality of the system, and range of the transverse momenta. Event-by-event fluctuations in global temperature over a large phase space provide the specific heat of the system. We present Beam Energy Scan of specific heat from data, AMPT and HRG model prediction. Experimental results from NA49, STAR, PHENIX, PHOBOS and ALICE are combined to obtain the specific heat as a function of …

Physicsthermodynamical fluctuationHistory010308 nuclear & particles physicsbeam energy scanheavy ion collisionsThermal fluctuationsThermodynamic temperature01 natural sciencesComputer Science ApplicationsEducationNuclear physicsTransverse planePionLattice (order)Phase space0103 physical sciences010306 general physicsNuclear ExperimentQuantum fluctuationEvent generator
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New quantum Monte Carlo formulation for modeling trans-polyacetylene properties: specific heat calculation

2004

Abstract In this paper we propose a new hybridization scheme for numerical simulation based on the determinantal quantum Monte Carlo and analytical model to treat the vibration mode of one-dimensional trans -polyacetylene chain. We use both of the extended Hubbard model (EHM) and Peierls–Hubbard model to compute the specific heat for different assumptions. For both the two models, our results indicate that the behavior of the specific heat is characterized by a maximum. We also introduce the effect of dimerization through Peierls–Hubbard model. In this case it is found that the specific heat magnitude is slightly more important when compared to specific heat value found with the EHM case. M…

Polymers and PlasticsComputer simulationHubbard modelChemistryQuantum Monte CarloOrganic ChemistryMonte Carlo methodSize consistency and size extensivityMaterials ChemistryCondensed Matter::Strongly Correlated ElectronsSolitonStatistical physicsGround stateQuantum fluctuationPolymer
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Plasmon mass scale and quantum fluctuations of classical fields on a real time lattice

2018

Classical real-time lattice simulations play an important role in understanding non-equilibrium phenomena in gauge theories and are used in particular to model the prethermal evolution of heavy-ion collisions. Above the Debye scale the classical Yang-Mills (CYM) theory can be matched smoothly to kinetic theory. First we study the limits of the quasiparticle picture of the CYM fields by determining the plasmon mass of the system using 3 different methods. Then we argue that one needs a numerical calculation of a system of classical gauge fields and small linearized fluctuations which correspond to quantum fluctuations, in a way that keeps the separation between the two manifest. We demonstra…

QC1-999hep-latFOS: Physical sciencesplasmafysiikka114 Physical sciences01 natural sciencessymbols.namesakeHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)LinearizationLattice (order)0103 physical sciencesGauge theory010306 general physicsQuantum fluctuationPlasmonplasmaParticle Physics - PhenomenologyDebyePhysicsta114010308 nuclear & particles physicsplasma physicsPhysicsGaussHigh Energy Physics - Lattice (hep-lat)hep-phParticle Physics - LatticeoscillationHigh Energy Physics - PhenomenologyClassical mechanicsQuasiparticlesymbols
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General Linearized Theory of Quantum Fluctuations around Arbitrary Limit Cycles

2017

The theory of Gaussian quantum fluctuations around classical steady states in nonlinear quantum-optical systems (also known as standard linearization) is a cornerstone for the analysis of such systems. Its simplicity, together with its accuracy far from critical points or situations where the nonlinearity reaches the strong coupling regime, has turned it into a widespread technique, which is the first method of choice in most works on the subject. However, such a technique finds strong practical and conceptual complications when one tries to apply it to situations in which the classical long-time solution is time dependent, a most prominent example being spontaneous limit-cycle formation. H…

Quantum PhysicsVan der Pol oscillatorGaussianFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesSymmetry (physics)Òptica quàntica010305 fluids & plasmasNonlinear systemsymbols.namesakeLinearizationQuantum mechanics0103 physical sciencessymbolsSymmetry breakingStatistical physicsLimit (mathematics)Quantum Physics (quant-ph)010306 general physicsQuantum fluctuationMathematicsPhysical Review Letters
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