Search results for "Inclusive"

showing 10 items of 5972 documents

"Table 6" 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 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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"Table 2" of "Search for stable hadronising squarks and gluinos with the ATLAS experiment at the LHC"

2012

Distribution of the observed BETA values in the Tile Calorimeter plus the simulated background and model estimates for three gluino masses.

Inclusiveanimal structuresgenetic structuresProton-Proton ScatteringPhysics::Instrumentation and DetectorsHigh Energy Physics::Phenomenology7000.0High Energy Physics::ExperimentP P --> CHARGED XNP P --> R-HADRON X
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"Table 6" of "Final COMPASS results on the deuteron spin-dependent structure function $g_1^{\rm d}$ and the Bjorken sum rule"

2017

Normalisations of the different data sets used in the QCD fit.

Inclusivel n --> l XComputer Science::Logic in Computer ScienceHigh Energy Physics::LatticeSpin Dependent Structure FunctionHigh Energy Physics::Phenomenologyl P --> l XDeep Inelastic ScatteringQCD fitHigh Energy Physics::ExperimentNLOl D --> l X
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"Table 5" of "Final COMPASS results on the deuteron spin-dependent structure function $g_1^{\rm d}$ and the Bjorken sum rule"

2017

Parameters of two solutions of the QCD fit. The assumed functional form at $Q^2_0 = 1 ($GeV$/c)^2$ is $q(x) = \eta x^\alpha (1-x)^\beta (1 + \gamma x)/N$ where N is the normalisation. The parametrisation is used for the singlet and gluon helicity distribution and the two non-singlet distributions $\Delta q_3$ and $\Delta q_8$.

Inclusivel n --> l XSpin Dependent Structure FunctionHigh Energy Physics::Phenomenologyl P --> l XDeep Inelastic ScatteringQCD fitHigh Energy Physics::ExperimentNLOl D --> l X
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