Search results for " Order"

showing 10 items of 827 documents

An algebraic approach to the Tavis-Cummings problem

2002

An algebraic method is introduced for an analytical solution of the eigenvalue problem of the Tavis-Cummings (TC) Hamiltonian, based on polynomially deformed su(2), i.e. su_n(2), algebras. In this method the eigenvalue problem is solved in terms of a specific perturbation theory, developed here up to third order. Generalization to the N-atom case of the Rabi frequency and dressed states is also provided. A remarkable enhancement of spontaneous emission of N atoms in a resonator is found to result from collective effects.

PhysicsCondensed Matter::Quantum GasesQuantum PhysicsFOS: Physical sciencesAtomic and Molecular Physics and Opticssymbols.namesakeResonatorThird orderQuantum mechanicssymbolsSpontaneous emissionPhysics::Atomic PhysicsAlgebraic numberHamiltonian (quantum mechanics)Algebraic methodQuantum Physics (quant-ph)Eigenvalues and eigenvectorsRabi frequency
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Magnetic order in the heavy fermion system Ce(Cu1−xNix)2Ge2

1990

Abstract The magnetic phase diagram of the heavy fermion (HF) systems Ce(Cu 1−x Ni x ) 2 Ge 2 is discussed utilizing results of transport, thermodynamic and neutron-scattering measurements. While the Kondo temperature increases monotonically with x, a complex x-dependence is found for the Neel temperature, associated with a transition from local-moment to itinerant HF magnetism.

PhysicsCondensed matter physicsMagnetismMagnetic orderMonotonic functionCondensed Matter PhysicsMagnetic phase diagramElectronic Optical and Magnetic MaterialsHeavy fermionOrder (group theory)Condensed Matter::Strongly Correlated ElectronsElectrical and Electronic EngineeringNéel temperatureMagnetic impurityPhysica B: Condensed Matter
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Asymptotic structure factor and power-law tails for phase ordering in systems with continuous symmetry.

1991

We compute the asymptotic structure factor ${\mathit{S}}_{\mathbf{k}}$(t) [=L(t${)}^{\mathit{d}}$g(kL(t)), where L(t) is a time-dependent characteristic length scale and d is the dimensionality] for a system with a nonconserved n-component vector order parameter quenched into the ordered phase. The well-known Ohta-Jasnow-Kawasaki-Yalabik-Gunton result is recovered for n=1. The scaling function g(x) has the large-x behavior g(x)\ensuremath{\sim}${\mathit{x}}^{\mathrm{\ensuremath{-}}(\mathit{d}+\mathit{n})}$, which includes Porod's law (for n=1) as a special case.

PhysicsContinuous symmetryPhase (matter)Phase orderingGeneral Physics and AstronomyOrder (ring theory)Function (mathematics)Structure factorPower lawScalingMathematical physicsPhysical review letters
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Implementing consistent NLO factorization in single inclusive forward hadron production

2017

Single inclusive forward hadron production in high-energy hadron collisions can provide an important test of the Color Glass Condensate picture at small $x$. Recent studies of this process at next-to-leading order have led to problematic results, with cross sections becoming negative at large transverse momenta. We study a new formulation of this quantity proposed recently by Iancu et al. We show that it leads to physical results up to large transverse momenta at fixed coupling. Taking into account running coupling effects in a way that is consistent with existing DIS calculations still poses a challenge.

PhysicsCouplingsingle inclusive hadron productionParticle physicseducation05 social sciencesHadronFOS: Physical sciences020207 software engineering02 engineering and technology114 Physical sciencesColor-glass condensateHigh Energy Physics - PhenomenologyTransverse planeHigh Energy Physics - Phenomenology (hep-ph)Factorization0202 electrical engineering electronic engineering information engineeringProduction (economics)0501 psychology and cognitive sciencesNuclear Experiment050107 human factorsnext-to-leading order cross section
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Exotic magnetism in the alkali sesquioxidesRb4O6andCs4O6

2009

Among the various alkali oxides the sesquioxides ${\text{Rb}}_{4}{\text{O}}_{6}$ and ${\text{Cs}}_{4}{\text{O}}_{6}$ are of special interest. Electronic-structure calculations using the local spin-density approximation predicted that ${\text{Rb}}_{4}{\text{O}}_{6}$ should be a half-metallic ferromagnet, which was later contradicted when an experimental investigation of the temperature-dependent magnetization of ${\text{Rb}}_{4}{\text{O}}_{6}$ showed a low-temperature magnetic transition and differences between zero-field-cooled and field-cooled measurements. Such behavior is known from spin glasses and frustrated systems. ${\text{Rb}}_{4}{\text{O}}_{6}$ and ${\text{Cs}}_{4}{\text{O}}_{6}$ c…

PhysicsCrystallographyCharge orderingMagnetizationSpin glassUnpaired electronCondensed matter physicsMagnetismValencyCrystal structureCondensed Matter PhysicsAntibonding molecular orbitalElectronic Optical and Magnetic MaterialsPhysical Review B
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Compact Topological Quantum Groups

1995

Using vector spaces topologies we unify the different models of quantum groups. Duality and reflexivity are built in. The Drinfeld deformation can be extended to the distributions on a simple compact Lie group and dually to the infinitely differentiable functions. The topological quantum double is similarly defined and a uniqueness result is obtained.

PhysicsDuality (mathematics)Topological orderTopological ringLie groupCompact quantum groupQuantum topologyTopologySymmetry protected topological orderTopological entropy in physics
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Simulating long-distance entanglement in quantum spin chains by superconducting flux qubits

2014

We investigate the performance of superconducting flux qubits for the adiabatic quantum simulation of long distance entanglement (LDE), namely a finite ground-state entanglement between the end spins of a quantum spin chain with open boundary conditions. As such, LDE can be considered an elementary precursor of edge modes and topological order. We discuss two possible implementations which simulate open chains with uniform bulk and weak end bonds, either with Ising or with XX nearest-neighbor interactions. In both cases we discuss a suitable protocol for the adiabatic preparation of the ground state in the physical regimes featuring LDE. In the first case the adiabatic manipulation and the …

PhysicsFlux qubitQuantum PhysicsFOS: Physical sciencesQuantum simulatorQuantum entanglementSquashed entanglementAdiabatic quantum computationAtomic and Molecular Physics and OpticsCondensed Matter - Other Condensed MatterQuantum electrodynamicsQuantum mechanicsTopological orderQuantum Physics (quant-ph)Adiabatic processSuperconducting quantum computingOther Condensed Matter (cond-mat.other)
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On the convergence of perturbative coupled cluster triples expansions:Error cancellations in the CCSD(T) model and the importance of amplitude relaxa…

2015

Recently, we proposed a novel Lagrangian-based perturbation series-the CCSD(T-n) series-which systematically corrects the coupled cluster singles and doubles (CCSD) energy in orders of the Møller-Plesset fluctuation potential for effects due to triple excitations. In the present study, we report numerical results for the CCSD(T-n) series up through fourth order which show the predicted convergence trend throughout the series towards the energy of its target, the coupled cluster singles, doubles, and triples (CCSDT) model. Since effects due to the relaxation of the CCSD singles and doubles amplitudes enter the CCSD(T-n) series at fourth order (the CCSD(T-4) model), we are able to separate th…

PhysicsGeneral Physics and AstronomyPerturbation (astronomy)T-modelCoupled clusterFourth orderAmplitudeClassical mechanicsPhysics::Atomic and Molecular ClustersPerturbation theory (quantum mechanics)Physical and Theoretical ChemistryTotal energyTriplet statePhysics::Chemical PhysicsMathematical physics
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Topological Phases in Planar Electrodynamics

2001

This section is meant to be an extension of Chap. 31 on the quantal Berry phases. In particular, we are interested in studying the electromagnetic interaction of particles with a nonzero magnetic moment in \(D = 2 + 1\) dimensions and of translational invariant configurations of \((D = 3 + 1)\)-dimensional charged strings with a nonzero magnetic moment per unit length. The whole discussion is based on our article in Physical Review D44, 1132 (1991).

PhysicsGeometric phaseMagnetic momentFractional quantum Hall effectTopological orderGauge theoryQuantum Hall effectSymmetry protected topological orderTopological quantum numberMathematical physics
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Direct perturbation theory in terms of energy derivatives: Fourth-order relativistic corrections at the Hartree–Fock level

2011

In this work, the quantum-chemical treatment of relativistic effects by means of direct perturbation theory is extended from its lowest order, DPT2, to the next higher order, DPT4. The required theory is given in terms of energy derivatives with the DPT4 energy correction defined as the corresponding second derivative with respect to the relativistic perturbation parameter λ(rel) = c(2) and c as the speed of light. To facilitate the implementation in standard quantum-chemical program packages, a general formulation of DPT starting from a nonrelativistic Lagrangian is developed, thereby expanding both wave function and operators in terms of λ(rel). The corresponding expressions, which incorp…

PhysicsHartree–Fock methodGeneral Physics and AstronomyPerturbation (astronomy)symbols.namesakeFourth orderModels ChemicalQuantum electrodynamicssymbolsQuantum TheoryPhysical and Theoretical ChemistryRelativistic quantum chemistryWave functionHyperfine structureSoftwareLagrangianSecond derivativeThe Journal of Chemical Physics
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