Search results for "Z0"

showing 10 items of 712 documents

"Table 7" of "Determination of $alpha_{s}$ in second order {QCD} from hadronic $Z$ decays"

1992

The energy-energy correlation EEC as a function of the correlation angle CHI.

InclusiveZ ProductionE+ E- --> HADRONSE+ E- ScatteringExclusive91.2E+ E- --> Z0 XEEC
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"Table 3" of "Measurement of inclusive jet cross-sections in Z/gamma*(---> e+ e-) + jets production in p anti-p collisions at s**(1/2) = 1.96-TeV"

2007

Total cross section for .GE.3JET.

InclusiveZ ProductionElectron productionPBAR P --> Z0 .GE.3JET XIntegrated Cross SectionPBAR P --> GAMMA* .GE.3JET XJet ProductionCross SectionSIG1960.0
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"Table 4" of "Measurement of the ratios of the Z/G* + >= n jet production cross sections to the total inclusive Z/G* cross section in ppbar collis…

2008

Number of observed events per 5 GeV bin for the >=3Jet sample. Data read from plots.

InclusiveZ ProductionElectron productionPBAR P --> Z0 .GE.3JET XJet ProductionN1960.115
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"Table 1" of "First measurement of sigma (p anti-p ---> Z) . Br (Z ---> tau tau) at s**(1/2) = 1.96- TeV"

2005

Measured cross section times branching ratio.

InclusiveZ ProductionIntegrated Cross SectionExclusivePBAR P --> Z0 XCross SectionTau productionSIG1960.0PBAR P --> TAU+ TAU-
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"Table 44" of "Studies of quantum chromodynamics with the ALEPH detector"

1997

Mean Multiplicities. Where a second systematic error is given, this is due to the uncertainty in the extrapolation to X = 0. Note that the ETA and ETAPRIMEvalues are for X > 0.1.

InclusiveZ ProductionStrange productionElectron productionE+ E- ScatteringE+ E- --> HADRON X91.2E+ E- --> Z0 XMULT
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"Table 1" of "Measurement of sigma(p anti-p ---> Z + X) Br(Z ---> tau+tau-) at s**(1/2) = 1.96-TeV"

2008

Measured cross section times branching ratio to TAU+ TAU-.

InclusiveZ Productionmental disordersIntegrated Cross SectionHigh Energy Physics::ExperimentPBAR P --> Z0 XCross SectionTau productionSIG1960.0
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General conservation law for a class of physics field theories

2019

In this paper we form a general conservation law that unifies a class of physics field theories. For this we first introduce the notion of a general field as a formal sum differential forms on a Minkowski manifold. Thereafter, we employ the action principle to define the conservation law for such general fields. By construction, particular field notions of physics, such as electric field strength, stress, strain etc. become instances of the general field. Hence, the differential equations that constitute physics field theories become also instances of the general conservation law. Accordingly, the general field and the general conservation law together correspond to a large class of physics…

Mathematics - Differential GeometryDifferential Geometry (math.DG)FOS: MathematicsFOS: Physical sciencesMathematical Physics (math-ph)Mathematical Physics53Z05 58Z05 58J45
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Multiplicity fluctuations in hadronic final states from the decay of the Z0

1992

An analysis of the fluctuations in the phase space distribution of hadrons produced in the decay of 78829 Z0 has been carried out, using the method of factorial moments. The high statistics collected by the DELPHI experiment at LEP during 1990 allowed studies of the event sample both globally and in intervals of p(t) and multiplicity, and for different jet topologies and for single jets. A large contribution to the factorial moments of the one-dimensional data on rapidity with respect to the event axis comes from hard gluons. Details of factorial moments in two and three dimensions are presented. Influences of resonance decays have been studied by Monte Carlo simulation: one-dimensional fac…

Nuclear and High Energy PhysicsFactorialParticle physicsE+E ANNIHILATIONLUND MONTE-CARLOMonte Carlo methodPartonMULTIPARTICLE PRODUCTION01 natural sciences7. Clean energyJET FRAGMENTATIONNuclear physicsParticle decayRAPIDITY DISTRIBUTIONS0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RapidityZ0010306 general physicsParton showerHIGH-ENERGY COLLISIONSQuantum chromodynamicsPhysics010308 nuclear & particles physicsLUND MONTE-CARLO; HIGH-ENERGY COLLISIONS; E+E ANNIHILATION; MULTIPARTICLE PRODUCTION; RAPIDITY DISTRIBUTIONS; INTERMITTENCY ANALYSIS; JET FRAGMENTATION; Z0; QCD; SIMULATIONQCDINTERMITTENCY ANALYSISGluonSIMULATIONHigh Energy Physics::ExperimentFísica nuclearParticle Physics - Experiment
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Measurements of the Lineshape of the $Z^{0}$ and Determination of Electroweak Parameters from its Hadronic and Leptonic Decays

1994

Abstract: During the LEP running periods in 1990 and 1991 DELPHI has accumulated approximately 450000 Z0 decays into hadrons and charged leptons. The increased event statistics coupled with improved analysis techniques and improved knowledge of the LEP beam energies permit significantly better measurements of the mass and width of the Z0 resonance. Model independent fits to the cross sections and leptonic forward-backward asymmetries yield the following Z0 parameters: the mass and total width M(Z) = 91.187 +/- 0.009 GeV, GAMMA(Z) = 2.486 +/- 0.012 GeV, the hadronic and leptonic partial widths GAMMA(had) = 1.725 +/- 0.012GeV, GAMMA(l) = 83.01 +/- 0.52 MeV, the invisible width GAMMA(inv) = 51…

Nuclear and High Energy PhysicsParticle physicsElectron–positron annihilationLEP-SLC ENERGIESElementary particle01 natural sciences7. Clean energyPartícules (Física nuclear)PHYSICSNuclear physicsBHABHA SCATTERINGParticle decay0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RADIATIVE-CORRECTIONSLEP-SLC ENERGIES; RADIATIVE-CORRECTIONS; BHABHA SCATTERING; MASS CORRECTIONS; PHYSICS010306 general physicsDetectors de radiacióDELPHIBhabha scatteringPhysics010308 nuclear & particles physicsPhysicsDELPHI; Z0 resonance; mass corrections; radiative correctionsMathematics::History and OverviewHigh Energy Physics::PhenomenologyElectroweak interactionWeinberg angleMASS CORRECTIONSradiative correctionsZ0 resonanceHiggs bosonHigh Energy Physics::ExperimentParticle Physics - ExperimentLepton
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A search for neutral higgs particles in Z$^0$ decays

1992

Abstract The search in DELPHI data for neutral Higgs bosons is described. No candidate for the Standard Model Higgs is seen in Z0 decays to H 0 ν ν , H 0 μ + μ − or H0τ+τ− after selections that proved efficient for finding simulated H0. One remaining candidate for Z0 → H0e+e− is consistent with background. Together with our earlier studies, these results restrict the H0 mass to be above 38 GeV/c2 at the 95% confidence level. No signal is found for decays of Minimal Supersymmetric Standard Model neutral Higgs bosons to τ+τ−. Limits are obtained for their decays to produce four jets.

Nuclear and High Energy PhysicsParticle physicsElectron–positron annihilationSTANDARD MODEL01 natural sciencesLower limitStandard ModelNuclear physicsPHYSICSLIMITS0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsBosonPhysicsMASS SCALAR BOSONLIGHT SCALAR010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyZ0 DECAYE+E COLLISIONSSupersymmetrySUPERSYMMETRIC MODELSLEPNUCLEAR DECAYHiggs bosonHigh Energy Physics::ExperimentFísica nuclearMASS SCALAR BOSON; Z0 DECAY; SUPERSYMMETRIC MODELS; STANDARD MODEL; E+E COLLISIONS; NUCLEAR DECAY; LIGHT SCALAR; LIMITS; LEP; PHYSICSParticle Physics - ExperimentMinimal Supersymmetric Standard Model
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