Search results for "Sigma"

showing 10 items of 346 documents

"Table 2" of "Measurement of the polarization of Lambda0, anti-Lambda0, Sigma+ and Xi- produced in a Sigma- beam of 330-GeV/c"

1995

Target Consisted of a copper and a carbon block arranged side by side.

POLInclusiveStrange productionSIGMA- CU --> XI- XPolarizationSIGMA- C --> XI- XExclusiveSIGMA- NUCLEUS --> X XI-
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"Table 3" of "Measurement of the polarization of Lambda0, anti-Lambda0, Sigma+ and Xi- produced in a Sigma- beam of 330-GeV/c"

1995

Target Consisted of a copper and a carbon block arranged side by side.

POLInclusiveStrange productionSIGMA- CU --> XI- XPolarizationSIGMA- C --> XI- XExclusiveSIGMA- NUCLEUS --> X XI-
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"Table 1" of "Measurement of the polarization of Lambda0, anti-Lambda0, Sigma+ and Xi- produced in a Sigma- beam of 330-GeV/c"

1995

Target Consisted of a copper and a carbon block arranged side by side.

POLStrange productionSIGMA- C --> XI- XSIGMA- CU --> SIGMA+ XSIGMA- C --> LAMBDABAR XSIGMA- C --> LAMBDA XSIGMA- CU --> LAMBDABAR XInclusiveSIGMA- CU --> LAMBDA XSIGMA- NUCLEUS --> LAMBDABAR XSIGMA- CU --> XI- XPolarizationSIGMA- C --> SIGMA+ XSIGMA- NUCLEUS --> LAMBDA XExclusiveSIGMA- NUCLEUS --> X XI-SIGMA- NUCLEUS --> SIGMA+ X
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Measurement of the ZZ cross-section in e(+)e(-) interactions at 183-189 GeV

2001

Measurements of on-shell ZZ production are described, using data collected by DELPHI in 1997 and 1998, at centre-of-mass energies sqrt(s) = 182.6 GeV and 188.6 GeV respectively. Results obtained in each of the final states q qbar q qbar, mu+mu- q qbar, e+e- q qbar, nu nubar q qbar, l+l-l+l-, and nu nubar l+l- are presented. The measured cross-sections for on-shell ZZ production via the tree-level doubly-resonant graphs (NC02) are: sigma_{NC02}(182.6 GeV) = 0.38 +- 0.18 (stat) +- 0.04 (syst) pb, sigma_{NC02}(188.6 GeV) = 0.60 +- 0.13 (stat) +- 0.07 (syst) pb. They are consistent with the Standard Model expectations of 0.25 pb and 0.65 pb at each energy.

Particle physicsNuclear and High Energy PhysicsCOLLISIONSLOWEST ORDER CALCULATIONSPAIR PRODUCTIONENERGIESMONTE-CARLO SIMULATIONFOS: Physical sciences2-PHOTON PROCESSES01 natural sciencesPartícules (Física nuclear)Standard ModelHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)LEP2SEARCH0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]PROGRAM010306 general physicsQCDELPHIPhysics010308 nuclear & particles physicsPhysicsSigmaMONTE-CARLO SIMULATION; LOWEST ORDER CALCULATIONS; PAIR PRODUCTION; 2-PHOTON PROCESSES; ROOT-S=183 GEV; COLLISIONS; PROGRAM; LEP2; ENERGIES; SEARCHLARGE ELECTRON POSITRON COLLIDERPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSFísica nuclearParticle Physics - ExperimentROOT-S=183 GEV
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Measurement of e+ e- → DD cross sections at the ψ(3770) resonance

2018

Chinese physics / C High energy physics and nuclear physics C 42(8), 083001 (2018). doi:10.1088/1674-1137/42/8/083001

Particle physicsNuclear and High Energy PhysicsMesoncharm mesonsElectron–positron annihilation01 natural sciencesResonance (particle physics)530BESIII/BEPCIIlaw.inventionHigh Energy Physics - ExperimentNOlaw0103 physical sciencesddc:530010306 general physicsColliderInstrumentationDECAY LIBRARY TAUOLAPhysicsLuminosity (scattering theory)Annihilation010308 nuclear & particles physicsSigmacross sectionsAstronomy and AstrophysicsBESIII/BEPCII; charm mesons; cross sections; Nuclear and High Energy Physics; Instrumentation; Astronomy and AstrophysicsHigh Energy Physics::ExperimentBar (unit)
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Measurement of e+e−→π+π−ψ(3686) from 4.008 to 4.600 GeV and observation of a charged structure in the π±ψ(3686) mass spectrum

2018

We study the process e(+)e(-) -> p(+)p(-)psi(3686) using 5.1 fb(-1) of data collected at 16 center-of-mass energy (root s) points from 4.008 to 4.600 GeV by the BESIII detector operating at the BEPCII collider. The measured Born cross sections for e(+)e(-) -> p(+)p(-)psi(3686) are consistent with previous results, but with much improved precision. A fit to the cross section shows contributions from two structures: the first has M = 4209.5 +/- 7.4 +/- 1.4 MeV/c(2) and Gamma = 80.1 +/- 24.6 +/- 2.9 MeV, and the second has M = 4383.8 +/- 4.2 +/- 0.8 MeV/c(2) and Gamma = 84.2 +/- 12.5 +/- 2.1 MeV, where the first errors are statistical and the second systematic. The lower-mass resonance is obse…

Particle physicsPhotonMesonElectron–positron annihilationGeneral Physics and AstronomyDalitz plot01 natural sciencesResonance (particle physics)law.inventionMomentumNuclear physicslaw0103 physical sciencesPiIntermediate stateInvariant massBorn approximationNuclear Experiment010306 general physicsColliderQuantum chromodynamicsPhysicsLuminosity (scattering theory)Linear polarization010308 nuclear & particles physicsSigmaMagnetic fieldAntimatterIsospinMass spectrumHigh Energy Physics::ExperimentAtomic physicsPhysical Review D
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Evidence for Muon Neutrino Oscillation in an Accelerator-Based Experiment

2005

We present results for muon neutrino oscillation in the KEK to Kamioka (K2K) long-baseline neutrino oscillation experiment. K2K uses an accelerator-produced muon neutrino beam with a mean energy of 1.3 GeV directed at the Super-Kamiokande detector. We observed the energy dependent disappearance of muon neutrino, which we presume have oscillated to tau neutrino. The probability that we would observe these results if there is no neutrino oscillation is 0.0050% (4.0 sigma).

Particle physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaGeneral Physics and AstronomyFOS: Physical sciencesddc:500.201 natural sciences7. Clean energyHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesMuon neutrino010306 general physicsNeutrino oscillationPhysicsTamura Norio010308 nuclear & particles physicsOscillationDetectorHigh Energy Physics::PhenomenologySigmaFísicaSolar neutrino problemK2K experimentPhysics::Accelerator Physics田村 詔生High Energy Physics::ExperimentBeam (structure)
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Rosenbluth Separation of the π^{0} Electroproduction Cross Section.

2016

We present deeply virtual $\pi^0$ electroproduction cross-section measurements at $x_B$=0.36 and three different $Q^2$--values ranging from 1.5 to 2 GeV$^2$, obtained from experiment E07-007 that ran in the Hall A at Jefferson Lab. The Rosenbluth technique was used to separate the longitudinal and transverse responses. Results demonstrate that the cross section is dominated by its transverse component, and thus is far from the asymptotic limit predicted by perturbative Quantum Chromodynamics. An indication of a non-zero longitudinal contribution is provided by the interference term $\sigma_{LT}$ also measured. Results are compared with several models based on the leading twist approach of G…

Particle physicslongitudinalinterferenceGeneral Physics and Astronomyparton: distribution functionPartonhard exclusive electroproduction; mesons[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesHigh Energy Physics - ExperimentNuclear physicspi: distribution amplitudegeneralized parton distribution: transversityPiondeep inelastic scattering0103 physical scienceshard exclusive electroproduction[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]quantum chromodynamics: perturbation theory010306 general physicsNuclear ExperimentNuclear ExperimentmesonsQuantum chromodynamicsPhysics010308 nuclear & particles physicsscattering amplitudemomentum transferSigmanucleon: generalized parton distributionScattering amplitudetransverseDistribution (mathematics)Amplitudepi0: electroproductiontwistHigh Energy Physics::ExperimentNucleonchannel cross section: measuredJefferson Labexperimental resultsPhysical review letters
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Sigmatisma korekcija 5 – 6 gadīgiem bērniem

2017

Maģistra darba nosaukums: „Sigmatisma korekcija 5 – 6 gadīgiem bērniem”. Darba autore: Liene Mačevska. Darba zinātniskā vadītāja: Dr. paed. profesore Sarmīte Tūbele. Darba saturs: 136 lappuses, 5 attēli, 10 tabulas, 18 pielikumi. Pētījuma mērķis: teorētiski izpētīt, pamatot un praktiski pārbaudīt dažādas sigmatisma korekcijas metodes 5 – 6 gadīgiem bērniem, lai veicinātu pareizu skaņu (svelpeņu, šņāceņu) izrunu. Pētījuma hipotēze: sigmatisma korekcija 5 – 6 gadīgiem bērniem norit veiksmīgi, ja: 1.tiek ņemtas vērā bērna attīstības īpatnības; 2.tiek izmantotas atbilstošas koriģējoši attīstošās metodes (vingrinājumi). Pētījuma teorētiskajā daļā, analizējot zinātnisko literatūru, autore aprakst…

Pedagoģijaskaņu izrunas traucējumipirmsskolasigmatismsrunas un valodas attīstība5 – 6 gadīgi bērni
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"K0S0_dcs02" of "$K^+\Lambda$ and $K^+\Sigma^0$ photoproduction with fine center-of-mass energy resolution"

2022

Excitation function at cos(Theta_K+)cm = -0.7

PhotoproductionGAMMA P --> K+ SIGMA0Exclusive
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