Search results for "STRANGE"

showing 10 items of 551 documents

"Table 4" of "Measurement of the g p -> K^0 Sigma^+ reaction with the Crystal Ball/TAPS detectors at the Mainz Microtron"

2014

The recoil polarization of the SIGMA+ for photon energy 1275, 1325, 1375 and 1425 MeV.

GAMMA P --> K0 SIGMA+POLPhotoproductionStrange productionPolarizationNuclear TheoryPhysics::Accelerator PhysicsExclusivePhysics::Atomic PhysicsNuclear Experiment
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"Table 3" of "Measurement of the g p -> K^0 Sigma^+ reaction with the Crystal Ball/TAPS detectors at the Mainz Microtron"

2014

The recoil polarization of the SIGMA+ for photon energy 1125, 1175 and 1225 MeV.

GAMMA P --> K0 SIGMA+POLPhotoproductionStrange productionPolarizationNuclear TheoryPhysics::Accelerator PhysicsExclusivePhysics::Atomic PhysicsNuclear Experiment
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"Table 2" of "Measurement of the g p -> K^0 Sigma^+ reaction with the Crystal Ball/TAPS detectors at the Mainz Microtron"

2014

The differential cross section for photon energies 1275, 1325, 1375 and 1425 MeV.

GAMMA P --> K0 SIGMA+Single Differential Cross SectionPhotoproductionStrange productionNuclear TheoryPhysics::Accelerator PhysicsExclusiveNuclear ExperimentDSIG/DOMEGA
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"Table 1" of "Measurement of the g p -> K^0 Sigma^+ reaction with the Crystal Ball/TAPS detectors at the Mainz Microtron"

2014

The differential cross section for photon energies 1125, 1175 and 1225 MeV.

GAMMA P --> K0 SIGMA+Single Differential Cross SectionPhotoproductionStrange productionNuclear TheoryPhysics::Accelerator PhysicsExclusiveNuclear ExperimentDSIG/DOMEGA
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Do Uncertainty and Fuzziness Present Themselves (and Behave) in the Same Way in Hard and Human Sciences?

2010

In the present paper the question whether uncertainty and fuzziness present themselves and behave in the same way (or not) in hard and human sciences will be briefly discussed. This problem came out from the attempt to answer the question asked by Lotfi Zadeh on the (apparent) strangeness of a very limited use of fuzzy sets in human sciences.

Hard and soft scienceSettore INF/01 - Informaticabusiness.industryUncertainty fuzziness hard sciences human sciences two cultures use of formal methods in human sciences.Fuzzy setHuman scienceArtificial intelligenceStrangenessType-2 fuzzy sets and systemsbusinessMathematics
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Core-collapse supernova simulations in one and two dimensions: comparison of codes and approximations

2018

We present spherically symmetric (1D) and axisymmetric (2D) supernova simulations for a convection-dominated 9 Msun and a 20 Msun progenitor that develops violent activity by the standing-accretion-shock instability (SASI). We compare in detail the Aenus-Alcar code, which uses fully multidimensional two-moment neutrino transport with an M1 closure, with a ray-by-ray-plus (RbR+) version of this code and with the Prometheus-Vertex code that employs RbR+ two-moment transport with a Boltzmann closure. Besides testing consequences of ignored non-radial neutrino-flux components in the RbR+ approximation, we also discuss the influence of various transport ingredients applied or not applied in rece…

High Energy Astrophysical Phenomena (astro-ph.HE)Physics010308 nuclear & particles physicsScatteringAdvectionAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesAstronomy and AstrophysicsStrangenessType II supernova01 natural sciencesInstabilityComputational physicsSupernovaAstrophysics - Solar and Stellar AstrophysicsSpace and Planetary Science0103 physical sciencesRadiative transferNeutrinoAstrophysics - High Energy Astrophysical Phenomena010303 astronomy & astrophysicsSolar and Stellar Astrophysics (astro-ph.SR)Monthly Notices of the Royal Astronomical Society
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Determination of the Chiral Couplings L10 and C87 from Semileptonic τ Decays

2008

Using recent precise hadronic tau-decay data on the V-A spectral function, and general properties of QCD such as analyticity, the operator product expansion and chiral perturbation theory, we get accurate values for the QCD chiral order parameters L_10^r(M_rho) and C_87^r(M_rho). These two low-energy constants appear at order p^4 and p^6, respectively, in the chiral perturbation theory expansion of the V-A correlator. At order p^4 we obtain L_10^r(M_rho) = -(5.22\pm 0.06)10^{-3}. Including in the analysis the two-loop (order p^6) contributions, we get L_10^r(M_rho) = -(4.06\pm 0.39)10^{-3} and C_87^r(M_rho) = (4.89\pm 0.19)10^{-3}GeV^{-2}. In the SU(2) chiral effective theory, the correspon…

High Energy Physics - Lattice (hep-lat)Spectral functionsFOS: Physical sciencesFísicaPerturbation theoryLow-energy constantsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeStrange quark massQCD predictionsHigh Energy Physics::ExperimentUs-vertical-barHadronic width
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Multiquark description of the D-sJ(2860) and D-sJ(2700)

2009

Within a theoretical framework that accounts for all open-charm mesons, including the D-0*(2308), the D-sJ*(2317), and the D-sJ(2460), we analyze the structure and explore possible quantum number assignments for the D-sJ(2860) and the D-sJ(2700) mesons reported by BABAR and Belle Collaborations. The open-charm sector is properly described if considered as a combination of conventional quark-antiquark states and four-quark components. All negative parity and 2(+) states can be understood in terms only of q (q) over bar components, however the description of the 0(+) and 1(+) mesons is improved whenever the mixing between two- and four-quark configurations is included. We analyze all possible…

High Energy Physics::PhenomenologyCharm mesonsFísicaHigh Energy Physics::ExperimentCharm-strange mesonsquark models
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Rapidity correlations in Lambda baryon and proton production in hadronic Z0 decays

1998

In an analysis of multihadronic events recorded at LEP by DELPHI in the years 1992 through 1994, charged hadrons are identified using the measurement of their energy loss and their Cherenkov angle. Rapidity correlations of \La-\La, proton-proton, and \La-proton pairs are compared. The agreement with the string and cluster fragmentation models is tested. For those pairs that frame a meson in terms of rapidity the compensation of strangeness is studied. For \La{}$\overline{\mathrm{p}}$ pairs the additional correlation with respect to charged kaons is analysed.

IMAGING CHERENKOV DETECTOR; DELPHIParticle physicsNuclear and High Energy PhysicsMesonElectron–positron annihilationHadronNuclear TheoryStrangenessLambdaLambda baryon01 natural sciencesPartícules (Física nuclear)Nuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Rapidity010306 general physicsNuclear ExperimentDELPHIPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyLARGE ELECTRON POSITRON COLLIDERIMAGING CHERENKOV DETECTORLarge Electron–Positron ColliderPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentParticle Physics - Experiment
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"Table 3" of "Long-range angular correlations of $\rm \pi$, K and p in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

2013

The Fourier coefficients V2(2PC,sub) extracted for charged kaons as a function of PT from the correlation in the 0-20% multiplicity class after subraction of the correlation from the 60-100% event class.

Inclusive5020.0P PB --> K+ XStrange productionCORRP PB --> K- X
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