Search results for "Integra"

showing 10 items of 5314 documents

"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 8" 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- --> K2*(1430) K with statistical errors only.

E+ E- --> K2*(1430)- K+Strange production1.92-3.0E+ E- ScatteringIntegrated Cross SectionExclusiveE+ E- --> K2*(1430)+ K-Cross SectionSIGE+ E- --> K2*(1430)0 KS
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"Table 2" of "Study of the muon pair production at center-of-mass energies from 20-GeV to 136-GeV with the ALEPH detector"

1997

Inclusive analysis from evvents with no specific selection of hard ISR.

E+ E- --> MU+ MU- (GAMMAS)Di-Muon ProductionAsymmetry MeasurementE+ E- ScatteringIntegrated Cross Section136.2ExclusiveCross SectionSIGMuon productionASYM
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"Table 1" of "Study of the muon pair production at center-of-mass energies from 20-GeV to 136-GeV with the ALEPH detector"

1997

Exlclusive analysis from events with hard ISR.

E+ E- --> MU+ MU- GAMMA (GAMMAS)Di-Muon ProductionAsymmetry MeasurementE+ E- ScatteringIntegrated Cross SectionExclusiveCross SectionSIGMuon productionASYM88.2-93.0
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