Search results for "76"

showing 10 items of 2584 documents

"Table 1" of "Net-Charge Fluctuations in Pb-Pb collisions at \surds_NN = 2.76 TeV"

2013

The measured NU(+-DYN) as a function of the centrality of the collisions, expressed as the number of participating nucleons, for two values of midrapidity range.

Nonlinear Sciences::Chaotic DynamicsInclusive2760.0CORRNuclear TheoryNuclear ExperimentPB PB --> CHARGED X
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"Table 1" of "Measurement of transverse energy at midrapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV"

2016

$\langle $d$E_{\mathrm T}/$d$\eta \rangle / (\langle N_{\mathrm{part}}/2\rangle)$ versus $N_{\mathrm{part}}$, $\langle $d$E_{\mathrm T}/$d$\eta \rangle / (\langle N_{\mathrm{quark}}/2\rangle)$, and $\epsilon\tau$ versus $N_{\mathrm{part}}$ at midrapidity calculated from the tracking detectors,.

Nonlinear Sciences::Chaotic DynamicsInclusiveMathematics::Functional AnalysisMathematics::Group Theory2760.0High Energy Physics::LatticeHigh Energy Physics::PhenomenologyPB PB --> CHARGED X
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"Table 3" of "Measurement of transverse energy at midrapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV"

2016

$\langle $d$E_{\mathrm T}/$d$\eta \rangle$/$\langle $d$N_{\mathrm{ch}}/$d$\eta \rangle$ versus $N_{part}$.

Nonlinear Sciences::Chaotic DynamicsInclusiveMathematics::Functional AnalysisMathematics::Group Theory2760.0High Energy Physics::LatticeHigh Energy Physics::PhenomenologyPB PB --> CHARGED X
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"Table 4" of "Suppression of $\Lambda(1520)$ resonance production in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV"

2018

$\langle p_{\rm T} \rangle$ of $\Lambda$(1520) (sum of particle and anti-particle states) at midrapidity as a function of $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle^{1/3}$. The uncertainty 'syst,uncorrelated' indicates the systematic uncertainty after removing the contributions common to all centrality classes

Nonlinear Sciences::Chaotic DynamicsInclusiveMathematics::Functional AnalysisMathematics::Group Theory2760.0PB PB --> LAMBDA_BAR(1520) XHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyCharge Particle Multiplicty DependencePB PB --> LAMBDA(1520) X
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"Table 2" of "Inclusive J/psi production in pp collisions at sqrt(s) = 2.76 TeV"

2016

The $\sqrt{s}$-dependence of $\langle p_{\rm T}\rangle$ for inclusive J/$\psi$ production (forward rapidity).

Nonlinear Sciences::Chaotic DynamicsInclusiveMathematics::Functional AnalysisMathematics::Group TheoryP P --> J/PSI XProton-Proton Scattering2.76-7.0High Energy Physics::LatticeHigh Energy Physics::PhenomenologyMEAN(PT)Muon productionJ/Psi
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"Table 1" of "Measurements of the Nuclear Modification Factor for Jets in Pb+Pb Collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV with the ATLAS Detect…

2015

The $\langle T_{\mathrm{AA}} \rangle $ and $\langle N_{\mathrm{part}} \rangle$ values and their uncertainties in each centrality bin.

Nonlinear Sciences::Chaotic DynamicsInclusiveMathematics::Functional AnalysisMathematics::Group TheoryPB PB --> X2760.0High Energy Physics::LatticeHigh Energy Physics::PhenomenologyN
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The extrabasinal elements in Lower Pennsylvanian floras of the Maritime Provinces, Canada: Description of Adiantites, Pseudadiantites and Rhacopterid…

2021

Adiantites adiantoide s (Lindley and Hutton) Kidston, Pseudadiantites sessilis (Roehl) Gothan and Pseudadiantites rhomboideus (Ettingshausen) comb. nov. are figured and described as well as Rhacopteridium speciosum (Ettingshausen) Hirmer, as part of a revision of lower Pennsylvanian floras of Nova Scotia. These species show a foliar branching structure which is described as "pseudopinnate" as against the fully planated pinnate structure of the Palaeozoic fern and pteridosperm fronds. Their systematic affinity is unknown. A discussion is presented of the genera A diantites, Pseudadiantites, Aneimites , Palaeopteridium , and Triphyllopteris , and the problematic nature of the history of Adian…

Nova scotiaFrondPaleozoicbiologyPaleontologybiology.organism_classificationQE701-760PaleontologyGeographyHabitatPennsylvanianFernflora pennsylvanian namurian westphalian nova scotia extrabasinal.PalaeogeographySpanish Journal of Palaeontology
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The first large-scale shell-model calculation of the two-neutrino double beta decay of $^{76}$Ge to the excited states in $^{76}$Se

2022

Large-scale shell-model calculations were carried out for the half-lives and branching ratios of the $2\nu\beta\beta$ decay of $^{76}$Ge to the ground state and the lowest three excited states $2_1^+$, $0_2^+$ and $2_2^+$ in $^{76}$Se. In total, the wave functions of more than 10,000 intermediate $1^+$ states in $^{76}$As were calculated in a three-step procedure allowing an efficient use of the available computer resources. In the first step, 250 lowest states, below some 5 MeV of excitation energy, were calculated without truncations within a full major shell $0f_{5/2}-1p-0g_{9/2}$ for both protons and neutrons. The wave functions of the rest of the states, up to some 30 MeV, were compute…

Nuclear Theory (nucl-th)Nuclear and High Energy PhysicsNuclear Theorymatrix elementsshell modelneutriinotdouble-beta decayFOS: Physical scienceshiukkasfysiikkaydinfysiikka76Geexcited states
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Irradiation induced defects in fluorine doped silica

2008

International audience; The role of fluorine doping in the response to UV pulsed laser and c radiation of silica preforms and fibers was studied using electron spin resonance (ESR) spectroscopy. Exposure to radiation mainly generates E0 centers, with the same effectiveness in fibers and in preforms. The E'concentration in F-doped silica fibers is found to increase with UV energy fluence till a saturation value, consistently with a precursor conversion process. These results show the fluorine role in reducing the strained Si–O bonds thus improving the radiation hardness of silica, also after drawing process.

Nuclear and High Energy Physics[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics]Optical fiberMaterials scienceOptical fiberDopingchemistry.chemical_elementSilicaPhotochemistryCrystallographic defectSilica irradiation effects fluorine dopinglaw.inventionNuclear magnetic resonancechemistrylawElectron spin resonanceHalogenPACS: 71.55.Jv; 61.72.Ww; 76.30.Mi; 61.80.Ed; 61.80.BaFluorineDefectsIrradiationElectron paramagnetic resonanceSpectroscopyInstrumentationFluorine doping
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Numerical analysis of the Oseen-type Peterlin viscoelastic model by the stabilized Lagrange-Galerkin method, Part II: A linear scheme

2017

This is the second part of our error analysis of the stabilized Lagrange-Galerkin scheme applied to the Oseen-type Peterlin viscoelastic model. Our scheme is a combination of the method of characteristics and Brezzi-Pitk\"aranta's stabilization method for the conforming linear elements, which leads to an efficient computation with a small number of degrees of freedom especially in three space dimensions. In this paper, Part II, we apply a semi-implicit time discretization which yields the linear scheme. We concentrate on the diffusive viscoelastic model, i.e. in the constitutive equation for time evolution of the conformation tensor a diffusive effect is included. Under mild stability condi…

Numerical AnalysisApplied MathematicsComputationNumerical analysisDegrees of freedom (statistics)010103 numerical & computational mathematicsNumerical Analysis (math.NA)01 natural sciences010101 applied mathematicsComputational MathematicsNonlinear systemMethod of characteristicsModeling and SimulationConvergence (routing)FOS: MathematicsApplied mathematicsTensorMathematics - Numerical Analysis65M12 76A05 65M60 65M250101 mathematicsGalerkin methodAnalysisMathematics
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