Search results for " Production"

showing 10 items of 5274 documents

"Table 3" of "Production of charmed mesons in Z decays"

1995

The DSYS error is due to the error in the branching ratio.

E+ E- --> HADRONSE+ E- --> Z0Integrated Cross Section91.2Cross SectionSIGInclusiveCharm productionE+ E- ScatteringE+ E- --> D- XExclusiveHigh Energy Physics::ExperimentE+ E- --> D+ XR measurement
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"Table 13" of "Studies of quantum chromodynamics with the ALEPH detector"

1997

Measure n-jet rates using the Durham cluster algorithm as a function of thejet-resolution parameter YCUT.

E+ E- --> HADRONSE+ E- --> Z0Integrated Cross Section91.2E+ E- --> 2JET XJet ProductionCross SectionSIGInclusiveDijet ProductionE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentR measurementComputer Science::Distributed Parallel and Cluster Computing
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"Table 15" of "Studies of quantum chromodynamics with the ALEPH detector"

1997

Measure n-jet rates using the Durham cluster algorithm as a function of thejet-resolution parameter YCUT.

E+ E- --> HADRONSE+ E- --> Z0Integrated Cross Section91.2E+ E- --> 4JET XJet ProductionCross SectionSIGInclusiveE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentR measurementComputer Science::Distributed Parallel and Cluster Computing
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"Table 16" of "Studies of quantum chromodynamics with the ALEPH detector"

1997

Measure n-jet rates using the Durham cluster algorithm as a function of thejet-resolution parameter YCUT.

E+ E- --> HADRONSE+ E- --> Z0Integrated Cross Section91.2Jet ProductionCross SectionSIGInclusiveE+ E- --> 5JET XE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentR measurementComputer Science::Distributed Parallel and Cluster Computing
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"Table 2" of "Production of charmed mesons in Z decays"

1995

The DSYS error is due to the error in the branching ratio.

E+ E- --> HADRONSE+ E- --> Z0Integrated Cross SectionE+ E- --> D*(2010)- X91.2E+ E- --> D*(2010)+ XCross SectionSIGInclusiveCharm productionE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentR measurement
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"Table 7" of "Measurements of e+ e- ---> K+ K- eta, K+ K- pi0 and K0(s) K+- pi-+ cross- sections using initial state radiation events"

2008

Isovector (I=1) component of the cross section for E+ E- --> K*(892) K with statistical errors only.

E+ E- --> K*(892)0 KSE+ E- --> K*(892)+ K-1.4-2.92Strange productionE+ E- --> K*(892)- K+E+ E- ScatteringIntegrated Cross SectionExclusiveCross SectionSIG
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"Table 6" of "Measurements of e+ e- ---> K+ K- eta, K+ K- pi0 and K0(s) K+- pi-+ cross- sections using initial state radiation events"

2008

Isoscalar (I=0) component of the cross section for E+ E- --> K*(892) K with statistical errors only.

E+ E- --> K*(892)0 KSE+ E- --> K*(892)+ K-Strange productionE+ E- --> K*(892)- K+E+ E- Scattering1.4-3.08Integrated Cross SectionExclusiveCross SectionSIG
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"Table 8" of "The $e^+ e^-\to 2(\pi^+\pi^-)\pi^0$, 2(\pi^+\pi^-)\eta$, $K^+ K^-\pi^+\pi^-\pi^0$ and $K^+ K^-\pi^+\pi^-\eta$ Cross Sections Measured w…

2007

Measured cross section for E+ E- --> K+ K- PI+ PI- PI0 with statistical errors only.

E+ E- --> K+ K- PI+ PI- PI0Strange productionE+ E- ScatteringIntegrated Cross SectionExclusiveCross SectionSIG1.613-4.487
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"Table 5" of "Production of K0 and Lambda in hadronic Z decays"

1994

Errors are dominantly systematic.

E+ E- --> K0 XE+ E- --> LAMBDA XE+ E- --> KS KS XStrange productionE+ E- --> KL XE+ E- --> LAMBDABAR LAMBDABAR XE+ E- --> Z091.2E+ E- --> LAMBDABAR KS XMULTInclusiveE+ E- --> LAMBDA LAMBDA XE+ E- ScatteringE+ E- --> LAMBDA LAMBDABAR XExclusiveE+ E- --> LAMBDA KS XE+ E- --> KS XE+ E- --> LAMBDABAR X
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"Table 7" of "Production of K0 and Lambda in hadronic Z decays"

1994

Numerical values supplied by P. Reeves.

E+ E- --> K0 XE+ E- --> LAMBDA XInclusiveSingle Differential Cross SectionStrange productionE+ E- --> Z0Rapidity DependenceE+ E- ScatteringExclusive91.2DSIG/DYRAPE+ E- --> LAMBDABAR X
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