Search results for "Z0"

showing 10 items of 712 documents

The Reasonable Effectiveness of Mathematical Deformation Theory in Physics

2019

This is a brief reminder, with extensions, from a different angle and for a less specialized audience, of my presentation at WGMP32 in July 2013, to which I refer for more details on the topics hinted at in the title, mainly deformation theory applied to quantization and symmetries (of elementary particles).

PhysicsHigh Energy Physics - TheoryDark matterDeformation theoryFOS: Physical sciencesElementary particleMathematical Physics (math-ph)[MATH] Mathematics [math]16. Peace & justiceTheoretical physicsQuantization (physics)53D55 81R50 17B37 53Z05 81S10 81V25 83C57High Energy Physics - Theory (hep-th)Homogeneous spaceAnti-de Sitter space[MATH]Mathematics [math]Mathematical Physics
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"Table 21" of "Measurement of the production cross section of jets in association with a Z boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLA…

2015

The distribution of Dy (jj). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.

Physics::Fluid DynamicsInclusiveDijet ProductionP P --> Z0 .GE.2JET XProton-Proton ScatteringZ Production7000.0High Energy Physics::ExperimentJet ProductionNuclear ExperimentMULT
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"Table 8" of "Measurement of the production cross section for Z/gamma* in association with jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS de…

2014

Jet differential cross section dsigma/dy as a function of the second-leading jet y corrected to the lepton common fiducial region and for QED radiation effects.

Physics::Fluid DynamicsInclusiveSingle Differential Cross SectionP P --> Z0 JET XP P --> GAMMA* JET XProton-Proton ScatteringZ ProductionAstrophysics::High Energy Astrophysical PhenomenaRapidity DependenceHigh Energy Physics::PhenomenologyHigh Energy Physics::ExperimentDSIG/DYRAPJet Production
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"Table 7" of "Measurement of the production cross section for Z/gamma* in association with jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS de…

2014

Jet differential cross section dsigma/dy as a function of the leading jet y corrected to the lepton common fiducial region and for QED radiation effects.

Physics::Fluid DynamicsInclusiveSingle Differential Cross SectionP P --> Z0 JET XP P --> GAMMA* JET XProton-Proton ScatteringZ ProductionAstrophysics::High Energy Astrophysical PhenomenaRapidity DependenceHigh Energy Physics::PhenomenologyHigh Energy Physics::ExperimentDSIG/DYRAPJet Production
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"Table 6" of "Measurement of the production cross section for Z/gamma* in association with jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS de…

2014

Inclusive jet differential cross section dsigma/dy corrected to the lepton common fiducial region and for QED radiation effects.

Physics::Fluid DynamicsInclusiveSingle Differential Cross SectionP P --> Z0 JET XP P --> GAMMA* JET XProton-Proton ScatteringZ ProductionRapidity DependenceHigh Energy Physics::PhenomenologyHigh Energy Physics::ExperimentDSIG/DYRAPJet Production
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"Table 2" of "A Precise Determination of the Number of Families With Light Neutrinos and of the $Z$ Boson Partial Widths"

1990

Calorimeter selection.

Physics::Instrumentation and DetectorsE+ E- --> HADRONSE+ E- --> Z0E+ E- ScatteringIntegrated Cross Section88.278-95.036ExclusiveHigh Energy Physics::ExperimentCross SectionR measurementSIG
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"Table 2" of "Measurement of electroweak parameters from Z decays into Fermion pairs"

1990

Hadronic cross section from the calorimeter selection trigger.

Physics::Instrumentation and DetectorsE+ E- --> HADRONSE+ E- --> Z0Nuclear TheoryHigh Energy Physics::PhenomenologyIntegrated Cross SectionCross SectionSIG88.227-95.036E+ E- ScatteringExclusiveHigh Energy Physics::ExperimentR measurementNuclear Experiment
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"Table 4" of "Search for dark matter in events with a hadronically decaying W or Z boson and missing transverse momentum in pp collisions at sqrt(s)=…

2014

Observed limits on the effective theory mass scale M* as a function of the dark matter mass M(chi) at 90% confidence-level from combined mono-W-boson and mono-Z-boson signals for various operators.

Quantitative Biology::Subcellular ProcessesCondensed Matter::Quantum GasesInclusive8000.0Proton-Proton ScatteringZ ProductionP P --> W- CHI CHIBAR XHigh Energy Physics::PhenomenologyP P --> Z0 CHI CHIBAR XMW ProductionP P --> W+ CHI CHIBAR X
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DETERMINATION OF ALPHA(S) FOR B-QUARKS AT THE Z(0) RESONANCE

1993

The strong coupling constant for b quarks has been determined, and its flavour independence, as predicted by QCD, investigated. The analysis involved events with lepton candidates selected from approximately 356 000 hadronic decays of the Z0, collected by the DELPHI detector at LEP in 1990 and 199 1. A method based on a direct comparison of the three-jet fraction in a b enriched sample, selected by requiring leptons with large momenta and transverse momenta, to that of the entire hadronic sample, illustrated the significant effect of the b quark mass on the multi-jet cross section, and verified the flavour independence of the strong coupling constant to an accuracy of +/- 6%. A second proce…

QuarkCHARMED MESONSNuclear and High Energy PhysicsParticle physicsHEAVY FLAVOR PRODUCTIONElectron–positron annihilationHigh Energy Physics::LatticeFRAGMENTATION FUNCTIONSFlavourHadron01 natural sciencesBottom quarkNuclear physicsMONTE-CARLO0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNuclear ExperimentZ DECAYSPhysicsCoupling constantQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyJET PRODUCTION-RATESQCDSTRING MODELHigh Energy Physics::ExperimentFísica nuclearHEAVY FLAVOR PRODUCTION; JET PRODUCTION-RATES; E+ E ANNIHILATION; Z0 RESONANCE; FRAGMENTATION FUNCTIONS; CHARMED MESONS; STRING MODEL; MONTE-CARLO; Z DECAYS; QCDE+ E ANNIHILATIONZ0 RESONANCEParticle Physics - ExperimentLepton
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A$_{FB}$ in the SMEFT: precision Z physics at the LHC

2021

We study the forward-backward asymmetry $A_{FB}$ in $pp \to \ell^+\ell^-$ at the Z peak within the Standard Model Effective Field Theory (SMEFT). We find that this observable provides per mille level constraints on the vertex corrections of the Z boson to quarks,which close a flat direction in the electroweak precision SMEFT fit. Moreover, we show that current $A_{FB}$ data is precise enough so that its inclusion in the fit improves significantly LEP bounds even in simple New Physics setups. This demonstrates that the LHC can compete with and complement LEP when it comes to precision measurements of the Z boson properties

QuarkNuclear and High Energy PhysicsParticle physicsp p: scatteringangular distribution: asymmetryPhysics beyond the Standard Modelmedia_common.quotation_subjectFOS: Physical sciencesQC770-79801 natural sciencesAsymmetryStandard ModelquarkZ0: productionHigh Energy Physics - Phenomenology (hep-ph)effective field theoryflat directionNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesEffective field theory010306 general physicsmedia_commonPhysicsLarge Hadron Colliderelectroweak interaction010308 nuclear & particles physicsprecision measurementnew physicsElectroweak interactionHigh Energy Physics::PhenomenologyObservableCERN LEP StorEffective Field Theoriescorrection: vertexHigh Energy Physics - Phenomenologyp p --> lepton+ lepton-CERN LHC Coll[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Beyond Standard ModelHigh Energy Physics::Experiment
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