Search results for "Cross Section"

showing 10 items of 3111 documents

"Table 25" of "Measurement of event shape and inclusive distributions at s**(1/2) = 130-GeV and 136-GeV."

1997

4-jet rate for the Jade Algorithm.

Computer Science::Multiagent SystemsE+ E- --> 4JET133.0Astrophysics::High Energy Astrophysical PhenomenaE+ E- ScatteringIntegrated Cross SectionExclusiveHigh Energy Physics::ExperimentJet ProductionCross SectionSIGComputer Science::Distributed Parallel and Cluster Computing
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"Table 26" of "Measurement of event shape and inclusive distributions at s**(1/2) = 130-GeV and 136-GeV."

1997

5-jet rate for the Jade Algorithm.

Computer Science::Multiagent SystemsE+ E- --> 5JET133.0Astrophysics::High Energy Astrophysical PhenomenaE+ E- ScatteringIntegrated Cross SectionExclusiveHigh Energy Physics::ExperimentJet ProductionCross SectionSIGComputer Science::Distributed Parallel and Cluster Computing
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"Table 1" of "Lowest Q**2 measurement of the gamma* p --> delta reaction: Probing the pionic contribution."

2006

Measured value of SIG(C=T) + EPS*SIG(C=L) as a function of the pion angle relative to the virtual photon direction.

ComputingMilieux_THECOMPUTINGPROFESSIONElectron productionNuclear TheoryIntegrated Cross SectionComputingMethodologies_IMAGEPROCESSINGANDCOMPUTERVISIONCross SectionSIGInformationSystems_MODELSANDPRINCIPLES7.950E-017.950E-01E- P --> E- PI0 PExclusiveInformationSystems_MISCELLANEOUS1.221ComputingMethodologies_COMPUTERGRAPHICSComputer Science::Cryptography and Security
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"Table 2" of "Measurement of inclusive K*(892)0, Phi(1020) and K*2(1430)0 production in hadronic Z decays."

1996

SIG in (1/SIG) is the total hadronic cross section. The erros are statistical ones. The cross sections SIG(C=A), SIG(C=B), and SIG(C=C) obtained with A) both kaons identified, B) at least one kaon identified, and C) without requiring kaon identification.

ComputingMilieux_THECOMPUTINGPROFESSIONGeneralLiterature_INTRODUCTORYANDSURVEYInformationSystems_INFORMATIONINTERFACESANDPRESENTATION(e.g.HCI)Nuclear Theory91.2DSIG/DXInclusiveSingle Differential Cross SectionInformationSystems_MODELSANDPRINCIPLESE+ E- --> PHI XE+ E- ScatteringHigh Energy Physics::ExperimentInformationSystems_MISCELLANEOUSNuclear ExperimentComputer Science::Cryptography and Security
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"Table 1" of "Measurement of inclusive K*(892)0, Phi(1020) and K*2(1430)0 production in hadronic Z decays."

1996

SIG in (1/SIG) is the total hadronic cross section. The statistical and systematic errors are combined quadratically.

ComputingMilieux_THECOMPUTINGPROFESSIONStrange productionGeneralLiterature_INTRODUCTORYANDSURVEYInformationSystems_INFORMATIONINTERFACESANDPRESENTATION(e.g.HCI)E+ E- --> K*(892)0 X91.2E+ E- --> K*BAR(892)0 XDSIG/DXInclusiveSingle Differential Cross SectionInformationSystems_MODELSANDPRINCIPLESE+ E- ScatteringInformationSystems_MISCELLANEOUSComputer Science::Cryptography and Security
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"Table 21" of "Search for supersymmetry in events with three leptons and missing transverse momentum in sqrt(s) = 7 TeV pp collisions with the ATLAS …

2012

The Systematic Uncertainty of the data (excluding the Monte Carlo) in signal region SR1 for the SUSY simplified model grid.

Condensed Matter::Materials ScienceProton-Proton ScatteringP P --> 3LEPTON JET(S) MMHigh Energy Physics::PhenomenologyIntegrated Cross SectionExclusiveSUSY7000.0Condensed Matter::Strongly Correlated ElectronsSupersymmetryJet ProductionCross SectionSIG
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"Table 23" of "Studies of W boson plus jets production in p\bar{p} collisions at sqrt(s)=1.96 TeV"

2013

Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of W boson pT for events with two or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesDijet ProductionInclusiveSingle Differential Cross SectionHigh Energy Physics::PhenomenologyPBAR P --> W+ JETS XPBAR P --> W- JETS XDSIG/DPTJet ProductionTransverse Momentum Dependence1960.0W Production
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"Table 6" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

2020

Observed and expected 95% CL upper limits on the b-associated Higgs boson production cross section times ditau branching fraction as a function of the boson mass.

Condensed Matter::Quantum GasesInclusiveP P --> TAU+ TAU- BQ BQBAR X13000.0Proton-Proton ScatteringHigh Energy Physics::PhenomenologyIntegrated Cross SectionHigh Energy Physics::ExperimentCross SectionSIGHiggs
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"Table 6" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

2020

Observed and expected 95% CL upper limits on the b-associated Higgs boson production cross section times ditau branching fraction as a function of the boson mass.

Condensed Matter::Quantum GasesInclusiveP P --> TAU+ TAU- BQ BQBAR X13000.0Proton-Proton ScatteringHigh Energy Physics::PhenomenologyIntegrated Cross SectionHigh Energy Physics::ExperimentCross SectionSIGHiggs
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"Table 6" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

2020

Observed and expected 95% CL upper limits on the b-associated Higgs boson production cross section times ditau branching fraction as a function of the boson mass.

Condensed Matter::Quantum GasesInclusiveP P --> TAU+ TAU- BQ BQBAR X13000.0Proton-Proton ScatteringHigh Energy Physics::PhenomenologyIntegrated Cross SectionHigh Energy Physics::ExperimentCross SectionSIGHiggs
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