Search results for "Number"

showing 10 items of 3939 documents

An improved limit for Γee of X(3872) and Γee measurement of ψ(3686)

2015

Using the data sets taken at center-of-mass energies above 4 GeV by the BESIII detector at the BEPCII storage ring, we search for the reaction e(+)e(-) -> gamma(ISR) X(3872) -> gamma(ISR)pi(+ ...

PhysicsPhysics::General PhysicsNuclear and High Energy PhysicsParticle physicsPhotonPhysics::Instrumentation and Detectors010308 nuclear & particles physicsBranching fractionAstrophysics::High Energy Astrophysical PhenomenaDetectorQuantum number01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentStatistical analysisLimit (mathematics)Nuclear Experiment010306 general physicsStorage ringX(3872)Physics Letters B
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Reply to Comment on Measurement of quantum states of neutrons in the Earth's gravitational field

2003

Physical review / D 68(10), 108702 (2003). doi:10.1103/PhysRevD.68.108702

PhysicsPhysics::General PhysicsNuclear and High Energy PhysicsQuantum geometry03.65.TaThermal quantum field theory010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]Quantum dynamicsQuantum numberquantum theory53001 natural sciencesGeneral Relativity and Quantum CosmologyQuantization (physics)Gravitational fieldQuantum stateQuantum mechanics0103 physical sciencesQuantum gravityddc:530010306 general physics
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Turbulence structure and budgets in curved pipes

2013

Abstract Turbulent flow in curved pipes was investigated by Direct Numerical Simulation. Three curvatures δ (pipe radius a /curvature radius c ) were examined: δ  = 0 (straight pipe), simulated for validation and comparison purposes; δ  = 0.1; and δ  = 0.3. The friction velocity Reynolds number (based on the pipe radius a ) was 500 in all cases, yielding bulk Reynolds numbers of ∼17,000, ∼15,000 and ∼12,000 for δ  = 0, 0.1 and 0.3, respectively. The computational domain was ten pipe radii in length and was resolved by up to 20 × 10 6 hexahedral finite volumes. The time step was chosen equal to a wall time unit; 1 Large Eddy TurnOver Time (LETOT) was thus resolved by 500 time steps and simul…

PhysicsPlug flowGeneral Computer ScienceTurbulenceDirect Numerical SimulationGeneral EngineeringDirect numerical simulationCurved pipeReynolds numberLaminar flowMechanicsCurved pipe;Direct Numerical Simulation;Turbulence budget;Turbulent flowCurvatureVortexTurbulent flowPhysics::Fluid Dynamicssymbols.namesakeClassical mechanicsTurbulence budgetsymbolsShear velocitySettore ING-IND/19 - Impianti Nucleari
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Phase Equilibria of Lattice Polymers from Histogram Reweighting Monte Carlo Simulations

1998

Histogram-reweighting Monte Carlo simulations were used to obtain polymer / solvent phase diagrams for lattice homopolymers of chain lengths up to r=1000 monomers. The simulation technique was based on performing a series of grand canonical Monte Carlo calculations for a small number of state points and combining the results to obtain the phase behavior of a system over a range of temperatures and densities. Critical parameters were determined from mixed-field finite-size scaling concepts by matching the order parameter distribution near the critical point to the distribution for the three-dimensional Ising universality class. Calculations for the simple cubic lattice (coordination number z…

PhysicsPolymers and PlasticsStatistical Mechanics (cond-mat.stat-mech)Coordination numberOrganic ChemistryMonte Carlo methodThermodynamicsFOS: Physical sciencesRenormalization groupCondensed Matter - Soft Condensed MatterInorganic ChemistryVirial coefficientCritical point (thermodynamics)Lattice (order)Materials ChemistrySoft Condensed Matter (cond-mat.soft)Ising modelScalingCondensed Matter - Statistical Mechanics
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On the application of canonical perturbation theory to floppy molecules

2000

International audience; Canonical perturbation theory (CPT) is a powerful tool in the field of molecular physics. It consists of a series of coordinate transformations aimed at rewriting the Hamiltonian in a simpler form without modifying the geometry of the phase space. The major achievement of CPT is the straightforward derivation of relations between the physically meaningful parameters of potential energy surfaces and the coefficients of the so-called effective Hamiltonians. While most of the studies performed up to date deal with surfaces expanded in polynomial series around a single minimum, CPT has also been applied to mixed polynomial/trigonometric expansions in the treatment of tor…

PhysicsPolynomial010304 chemical physics[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]General Physics and AstronomyQuantum number01 natural sciencesPotential energyNonlinear systemsymbols.namesakeClassical mechanics[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Phase spaceSaddle point0103 physical sciencessymbolsPerturbation theory (quantum mechanics)Physical and Theoretical Chemistry010306 general physicsHamiltonian (quantum mechanics)[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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High Reynolds number Navier-Stokes solutions and boundary layer separation induced by a rectilinear vortex array

2008

Numerical solutions of Prandtl’s equation and Navier Stokes equations are considered for the two dimensional flow induced by an array of periodic rec- tilinear vortices interacting with an infinite plane. We show how this initial datum develops a separation singularity for Prandtl equation. We investigate the asymptotic validity of boundary layer theory considering numerical solu- tions for the full Navier Stokes equations at high Reynolds numbers.

PhysicsPrandtl numberMathematical analysisMathematics::Analysis of PDEsReynolds numberNon-dimensionalization and scaling of the Navier–Stokes equationsunsteady separationReynolds equationPhysics::Fluid DynamicsFlow separationsymbols.namesakeBoundary layerPrandtl equation interactive viscous–inviscid equation.Navier Stokes solutionsymbolszero viscosity limitNavier–Stokes equationsReynolds-averaged Navier–Stokes equationsSettore MAT/07 - Fisica Matematica
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Kr369660 –Low- Z Boundary of the Island of Deformation at N=60

2017

Prompt γ-ray spectroscopy of the neutron-rich $^{96}$Kr, produced in transfer- and fusion-induced fission reactions, has been performed using the combination of the Advanced Gamma Tracking Array and the VAMOS++ spectrometer. A second excited state, assigned to $J^π$ = $4^+$, is observed for the first time, and a previously reported level energy of the first 2+ excited state is confirmed. The measured energy ratio R4/2 = E($4^+$)/E($2^+$) = 2.12(1) indicates that this nucleus does not show a well-developed collectivity contrary to that seen in heavier N = 60 isotones. This new measurement highlights an abrupt transition of the degree of collectivity as a function of the proton number at Z = …

PhysicsProton010308 nuclear & particles physicsFissionGeneral Physics and Astronomy01 natural sciencesAtomic orbitalExcited stateNeutron number0103 physical sciencesQuadrupoleAtomic numberAtomic physicsNuclear Experiment010306 general physicsSpectroscopyPhysical Review Letters
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Evolution of proton single-particle states in neutron-rich Sb isotopes beyond N=82

2020

11 pags., 8 figs., 2 tabs.

PhysicsProtonIsotope010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaNuclear structure[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Structure7. Clean energy01 natural sciencesBeta decayNuclear physicsNeutron numberExcited state0103 physical sciencesNeutronNuclear Experiment010306 general physicsExcitationPhysical Review C
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Projections and isolated points of parts of the spectrum

2018

‎‎In this paper‎, ‎we relate the existence of certain projections‎, ‎commuting with a bounded linear operator $T\in L(X)$ acting on Banach space $X$‎, ‎with the generalized Kato decomposition of $T$‎. ‎We also relate the existence of these projections with some properties of the quasi-nilpotent part $H_0(T)$ and the analytic core $K(T)$‎. ‎Further results are given for the isolated points of some parts of the spectrum‎.

PhysicsPure mathematics47A11‎Algebra and Number Theory‎localized SVEP‎‎spectrum‎47A53‎Spectrum (functional analysis)Banach spaceLocalized SVEPKato decompositionBounded operator47A10SpectrumCore (graph theory)Decomposition (computer science)‎47A55Analysis
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Multiple Noncommutative Tori and Hopf Algebras

2001

We derive the Kac-Paljutkin finite-dimensional Hopf algebras as finite fibrations of the quantum double torus and generalize the construction for quantum multiple tori.

PhysicsPure mathematicsAlgebra and Number TheoryFOS: Physical sciencesTorusMathematics - Rings and AlgebrasMathematical Physics (math-ph)Hopf algebraNoncommutative geometry16W30 57T05Rings and Algebras (math.RA)Mathematics::Quantum AlgebraMathematics - Quantum AlgebraFOS: MathematicsQuantum Algebra (math.QA)Mathematics::Symplectic GeometryQuantumMathematical PhysicsCommunications in Algebra
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