Search results for "inclusive"

showing 10 items of 5972 documents

Handicap et inclusion scolaire au Cameroun : ce qu'en disent les enseignants ?

2019

International audience; Fondée sur le principe de l'égalité des chances et sur les valeurs humaines d'équité et du respect des différences, l'inclusion scolaire s'attache « à la façon de transformer les systèmes éducatifs et d'améliorer la qualité de l'éducation à tous les niveaux et dans tous les environnements, de manière à s'adapter à la diversité des apprenants et à promouvoir la réussite scolaire » (UNESCO, 2008). Elle est prescrite comme une injonction internationale quels que soient les contextes, elle implique un changement de paradigme dans lequel les conditions de réussite dépendent de la capacité de l'école à s'adapter à la diversité du public qu'elle accueille (Dyson et al., 199…

HandicapéCameroun[SHS.EDU]Humanities and Social Sciences/Education[SHS.EDU] Humanities and Social Sciences/EducationÉlèvePerceptionÉducation inclusiveEnseignant
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Education inclusive en Afrique subsaharienne

2013

L'éducation inclusive est identifiée comme une des stratégies permettant la réalisation de l'éducation pour tous. Mais dans les contextes où il existe une pluralité de problèmes éducatifs à régler, est-il possible d'inclure dans le système scolaire tous les groupes exposés à la marginalisation et à l'exclusion scolaire au travers des plans nationaux d'éducation ? Comment assurer la prise en compte des besoins éducatifs particuliers des enfants handicapés ? Cet ouvrage aborde ces questions en s'appuyant sur le cas de l'Afrique subsaharienne.

Handicapé[SHS.EDU]Humanities and Social Sciences/Education[SHS.EDU] Humanities and Social Sciences/EducationÉducation pour tousÉlève[ SHS.EDU ] Humanities and Social Sciences/EducationIntégration scolaireÉducation inclusiveBesoin éducatifAfrique subsaharienne
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Dynamics of the caring family

2003

When several individuals simultaneously provide for offspring, as in families, the effort of any one individual will depend on the efforts of the other family members. This conflict of interest among family members is made more complicated by their relatedness because relatives share genetic interest to some degree. The conflict resolution will also be influenced by the differences in reproductive value between breeders and helpers. Here, we calculate evolutionarily stable provisioning efforts in families with up to two helpers. We explicitly consider that the behavioral choices are made in a life-history context, and we also consider how group sizes change dynamically; this affects, for ex…

Hereditycooperative breedingContext (language use)provisioning effortsBiologymedicine.disease_causeModels BiologicalNesting BehaviorConflict PsychologicalCooperative breedingConflict resolutionHereditymedicineAnimalsESSFamilyCooperative Behaviorevolutionary conflict.Ecology Evolution Behavior and SystematicsEcologyEcologyReproductionInclusive fitnessProvisioningFeeding BehaviorBiological EvolutionStepfamilyfamily dynamicsReproductive valueload lighteningEnergy MetabolismSocial psychology
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Inclusive D-Meson Production at the LHC

2012

I present predictions for the inclusive production of $D$ mesons at the CERN LHC in the general-mass variable-flavor-number scheme at next-to-leading order. Numerical results are compared to data where available, and uncertainties to scale variations, parton distribution functions and charm mass are discussed. I point out that measurements at large rapidity have the potential to pin down models of intrinsic charm.

High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CERN LHC Collmass [charm]PhysicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesHigh Energy Physics::ExperimentNuclear Experimentdistribution function [parton]numerical calculationsinclusive production [D]1 [higher-order]
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Measurement of CP asymmetry in D 0 → K - K + and D 0 → π - πdecays

2014

Time-integrated $CP$ asymmetries in $D^0$ decays to the final states $K^- K^+$ and $\pi^- \pi^+$ are measured using proton-proton collisions corresponding to $3\mathrm{\,fb}^{-1}$ of integrated luminosity collected at centre-of-mass energies of $7\mathrm{\,Te\kern -0.1em V}$ and $8\mathrm{\,Te\kern -0.1em V}$. The $D^0$ mesons are produced in semileptonic $b$-hadron decays, where the charge of the accompanying muon is used to determine the initial flavour of the charm meson. The difference in $CP$ asymmetries between the two final states is measured to be \begin{align} \Delta A_{CP} = A_{CP}(K^-K^+)-A_{CP}(\pi^-\pi^+) = (+0.14 \pm 0.16\mathrm{\,(stat)} \pm 0.08\mathrm{\,(syst)})\% \ . \nonu…

High Energy Physics::Lattice14.40.Lb01 natural sciencesLuminositySettore FIS/04 - Fisica Nucleare e SubnucleareFlavor physicsABSORPTIONPhysics::Chemical PhysicsNuclear ExperimentQCmedia_commonCharm physicsPhysicsHadronic decays of charmed mesonCharm physics; CP violation; Flavor physics; Hadron-Hadron ScatteringParticle physicsHadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified hadronCharge conjugation parity time reversal and other discrete symmetrieFIS/01 - FISICA SPERIMENTALECP violation13.25.FtSCATTERING-AMPLITUDEFísica nuclearLHCParticle physicsCharm physicNuclear and High Energy PhysicsMesonmedia_common.quotation_subjectLHCb - Abteilung HofmannHadronsAsymmetryREGENERATIONTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYSEARCH0103 physical sciencesPiSCATTERINGSCATTERING-AMPLITUDE; REGENERATION; ABSORPTION; SEARCHSDG 7 - Affordable and Clean Energy010306 general physicsLarge Hadron Collider (France and Switzerland)/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyMuonHadron-Hadron Scattering010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyGran Col·lisionador d'HadronsCharge (physics)LHCbFlavor physic11.30.ErHigh Energy Physics::ExperimentFísica de partículesExperiments13.85.NiCharmed mesons (|C|>0 B=0)FIS/04 - FISICA NUCLEARE E SUBNUCLEARE
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"Table 1" of "Investigation of the splitting of quark and gluon jets."

1998

Scaled energy distribution of charged hadrons produced in Quark jets in 'Y'topology 3-JET events.

High Energy Physics::LatticeAstrophysics::High Energy Astrophysical PhenomenaE+ E- --> Z0Nuclear TheoryHigh Energy Physics::Phenomenology91.2Jet ProductionE+ E- --> CHGD-HADRONS XDSIG/DXInclusiveSingle Differential Cross SectionE+ E- --> 3JETE+ E- ScatteringExclusiveHigh Energy Physics::Experiment
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"Table 3" of "Investigation of the splitting of quark and gluon jets."

1998

Scaled energy distribution of charged hadrons produced in Quark jets in 'Mercedes' topology 3-JET events.

High Energy Physics::LatticeAstrophysics::High Energy Astrophysical PhenomenaE+ E- --> Z0Nuclear TheoryHigh Energy Physics::Phenomenology91.2Jet ProductionE+ E- --> CHGD-HADRONS XDSIG/DXInclusiveSingle Differential Cross SectionE+ E- --> 3JETE+ E- ScatteringExclusiveHigh Energy Physics::Experiment
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"Table 1" of "Identified Charged Particles in Quark and Gluon Jets"

2003

Jet flavor tagging is used. (C=DUSCB), (C=DUSC), (C=UDS) mean quark-jet flavors. CONST(C=GLUON/JET) is the ratio gluon/jet for all charged particles. 'Y' events, mirror symmetric events, the angle between the most energetic jet and other two jets is 150 +- 15 deg.

High Energy Physics::LatticeAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryHigh Energy Physics::PhenomenologyE+ E- --> QUARK QUARKBAR GLUONQUARK --> PI- X91.2QUARK --> PI+ XMULTQUARKBAR --> PI- XInclusiveQUARKBAR --> PI+ XE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentGLUON --> PI+ XGLUON --> PI- XMULT/MULT
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"Table 4" of "Identified Charged Particles in Quark and Gluon Jets"

2003

Jet flavor tagging is used. (C=DUSCB), (C=DUSC), (C=UDS) mean quark-jet flavors. CONST(C=GLUON/JET) is the ratio gluon/jet for all charged particles. 'Y' events, mirror symmetric events, the angle between the most energetic jet and other two jets is 150 +- 15 deg.

High Energy Physics::LatticeAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryHigh Energy Physics::PhenomenologyE+ E- --> QUARK QUARKBAR GLUONQUARKBAR --> CHARGED X91.2MULTInclusiveGLUON --> CHARGED XQUARK --> CHARGED XE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentMULT/MULT
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"Table 3" of "The scale dependence of the hadron multiplicity in quark and gluon jets and a precise determination of C(A)/C(F)."

1999

Twice the difference of the multiplicity in three jet events and in qqbar events of comparable scale 2(N_3jet-N_qqbar). The three-jet event multiplicity isequal to the data of Fig. 3c), the qqbar-multiplicity is taken from a fit of th e e+e- data corrected for the varying b-quark contribution. This multiplicity can be identified with the multiplicity of a hypothetical gluon-gluon event. Thereis a normalization uncertainty (i.e. a scale independent constant) of the gluon -gluon event multiplicity which should not influence the slope of the gg-multiplicity with scale (see paper). The errors shown are statistical only.

High Energy Physics::LatticeE+ E- --> 2JET GAMMAE+ E- --> HADRONSE+ E- --> Z0High Energy Physics::PhenomenologyE+ E- --> CHARGED XJet ProductionMULTInclusiveDijet ProductionE+ E- --> 3JETE+ E- ScatteringExclusive0.216High Energy Physics::Experiment
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