Search results for "Chaotic dynamics"

showing 10 items of 197 documents

"Table 4" of "Properties of jet fragmentation using charged particles measured with the ATLAS detector in $pp$ collisions at $\sqrt{s}=13$ TeV"

2020

$\langle \zeta \rangle$, central jet.

Nonlinear Sciences::Chaotic DynamicsMathematics::Functional AnalysisMathematics::Group Theory13000.0$\langle \zeta \rangle$High Energy Physics::LatticeHigh Energy Physics::PhenomenologyP P --> jet jet
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"2/NPART*" of "Centrality and pseudorapidity dependence of the charged-particle multiplicity density in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.4…

2019

Values of $2/\langle N_\mathrm{part} \rangle \langle \mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle$ and $2/\langle N_\mathrm{part} \rangle N^\mathrm{tot}_\mathrm{ch}$ in Xe--Xe collisions at $\sqrt{s_{_{\mathrm{NN}}}} = 5.44\,\mathrm{TeV}$ for the top 5$\%$ central collisions.

Nonlinear Sciences::Chaotic DynamicsMathematics::Functional AnalysisMathematics::Group TheoryHigh Energy Physics::LatticeHigh Energy Physics::Phenomenology5440.0XE XE --> CHARGED X2/NPART*
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"2/NPART*_VS_SCALED" of "Centrality and pseudorapidity dependence of the charged-particle multiplicity density in Xe-Xe collisions at $\sqrt{s_{\rm N…

2019

Values of $2/\langle N_\mathrm{part} \rangle \langle \mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle$ and $2/\langle N_\mathrm{part} \rangle N^\mathrm{tot}_\mathrm{ch}$ as a function of $(\langle N_\mathrm{part} \rangle -2)/(2A)$ in Xe--Xe collisions at $\sqrt{s_{_{\mathrm{NN}}}} = 5.44\,\mathrm{TeV}$.

Nonlinear Sciences::Chaotic DynamicsMathematics::Functional AnalysisMathematics::Group TheoryHigh Energy Physics::LatticeHigh Energy Physics::Phenomenology5440.0XE XE --> CHARGED X2/NPART*
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"2/NPART*VS" of "Centrality and pseudorapidity dependence of the charged-particle multiplicity density in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5…

2019

Values of $2/\langle N_\mathrm{part} \rangle \langle \mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle$ and $2/\langle N_\mathrm{part} \rangle N^\mathrm{tot}_\mathrm{ch}$ as a function of $\langle N_\mathrm{part} \rangle$ in Xe--Xe collisions at $\sqrt{s_{_{\mathrm{NN}}}} = 5.44\,\mathrm{TeV}$.

Nonlinear Sciences::Chaotic DynamicsMathematics::Functional AnalysisMathematics::Group TheoryHigh Energy Physics::LatticeHigh Energy Physics::Phenomenology5440.0XE XE --> CHARGED X2/NPART*
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"Table 1" of "Measurement of the t anti-t production cross-section in p anti-p collisions using dilepton events"

2008

TOP TOPBAR production cross section for top quark mass 175 GeV.

Nonlinear Sciences::Chaotic DynamicsNonlinear Sciences::Exactly Solvable and Integrable SystemsPBAR P --> TOP TOPBARIntegrated Cross SectionPhysics::Atomic and Molecular ClustersExclusiveHigh Energy Physics::ExperimentCross SectionSIG1960.0Computer Science::Computers and Society
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"Table 1" of "Measurement of the t anti-t production cross section in p anti-p collisions at s**(1/2) = 1.96-TeV"

2008

The combined result for the TOP TOPBAR production cross section at top quark mass of 175 GeV.. The second DSYS error is the uncertainty on the luminosity.

Nonlinear Sciences::Chaotic DynamicsNonlinear Sciences::Exactly Solvable and Integrable SystemsPBAR P --> TOP TOPBARIntegrated Cross SectionPhysics::Atomic and Molecular ClustersExclusiveHigh Energy Physics::ExperimentCross SectionSIG1960.0Computer Science::Computers and Society
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"Table 2" of "Measurement of the t anti-t production cross section in p anti-p collisions at s**(1/2) = 1.96-TeV"

2008

The cross section for TOP TOPBAR production at the world average top quark mass of 172.6 GeV.. Errors contain both statistics and systematics.

Nonlinear Sciences::Chaotic DynamicsNonlinear Sciences::Exactly Solvable and Integrable SystemsPBAR P --> TOP TOPBARIntegrated Cross SectionPhysics::Atomic and Molecular ClustersExclusiveHigh Energy Physics::ExperimentCross SectionSIG1960.0Computer Science::Computers and Society
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"Table 12" of "Search for light scalar top quark pair production in final states with two leptons with the ATLAS detector in sqrt(s) = 7 TeV proton-p…

2012

Distribution of the Jet Multiplicity for all events in the Top Control Region.

Nonlinear Sciences::Chaotic DynamicsNonlinear Sciences::Exactly Solvable and Integrable SystemsProton-Proton ScatteringAstrophysics::High Energy Astrophysical PhenomenaP P --> LEPTON+ LEPTON- JET(S) MMPhysics::Atomic and Molecular ClustersExclusiveTop7000.0Jet ProductionComputer Science::Computers and Society
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Spiking patterns emerging from wave instabilities in a one-dimensional neural lattice.

2003

The dynamics of a one-dimensional lattice (chain) of electrically coupled neurons modeled by the FitzHugh-Nagumo excitable system with modified nonlinearity is investigated. We have found that for certain conditions the lattice exhibits a countable set of pulselike wave solutions. The analysis of homoclinic and heteroclinic bifurcations is given. Corresponding bifurcation sets have the shapes of spirals twisting to the same center. The appearance of chaotic spiking patterns emerging from wave instabilities is discussed.

Nonlinear Sciences::Chaotic DynamicsNonlinear systemClassical mechanicsQuantitative Biology::Neurons and CognitionArtificial neural networkControl theoryLattice (order)ChaoticCountable setHomoclinic orbitNonlinear Sciences::Pattern Formation and SolitonsBifurcationMathematicsPhysical review. E, Statistical, nonlinear, and soft matter physics
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KAM Techniques for Time Dependent Quantum Systems

1995

We consider a spin 1/2 in constant magnetic field perturbed by a quasiperiodic time dependent magnetic field. We discuss its stability properties in terms of the spectrum of the corresponding quasienergy operator. Since the spectrum of the unperturbed problem is dense, there appear small denominators in the perturbation theory, corresponding to resonances. They are treated with a technique developped by L.H. Eliasson, based on a KAM iteration.

Nonlinear Sciences::Chaotic DynamicsOperator (physics)Quantum mechanicsQuasiperiodic functionSpectrum (functional analysis)Perturbation theoryConstant (mathematics)QuantumMathematicsMagnetic fieldSpin-½
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