Search results for "Cross Section"

showing 10 items of 3111 documents

"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
researchProduct

"Table 5" 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 gluon-gluon fusion Higgs boson production cross section times ditau branching fraction as a function of the Higgs boson mass.

Condensed Matter::Quantum GasesInclusiveP P --> TAU+ TAU- X13000.0Proton-Proton ScatteringHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyIntegrated Cross SectionHigh Energy Physics::ExperimentCross SectionNuclear ExperimentSIGHiggs
researchProduct

"Table 5" 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 gluon-gluon fusion Higgs boson production cross section times ditau branching fraction as a function of the Higgs boson mass.

Condensed Matter::Quantum GasesInclusiveP P --> TAU+ TAU- X13000.0Proton-Proton ScatteringHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyIntegrated Cross SectionHigh Energy Physics::ExperimentCross SectionNuclear ExperimentSIGHiggs
researchProduct

"Table 5" 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 gluon-gluon fusion Higgs boson production cross section times ditau branching fraction as a function of the Higgs boson mass.

Condensed Matter::Quantum GasesInclusiveP P --> TAU+ TAU- X13000.0Proton-Proton ScatteringHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyIntegrated Cross SectionHigh Energy Physics::ExperimentCross SectionNuclear ExperimentSIGHiggs
researchProduct

"Table 5" 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 gluon-gluon fusion Higgs boson production cross section times ditau branching fraction as a function of the Higgs boson mass.

Condensed Matter::Quantum GasesInclusiveP P --> TAU+ TAU- X13000.0Proton-Proton ScatteringHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyIntegrated Cross SectionHigh Energy Physics::ExperimentCross SectionNuclear ExperimentSIGHiggs
researchProduct

"Table 30" 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 HT for events with one or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionDSIG/DHTPBAR P --> W+ JETS XPBAR P --> W- JETS XJet Production1960.0W Production
researchProduct

"Table 32" 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 HT for events with three or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionDSIG/DHTPBAR P --> W+ JETS XPBAR P --> W- JETS XJet Production1960.0W Production
researchProduct

"Table 33" 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 HT for events with four or more jets produced in association with a W boson. First uncertainty is statistical, second uncertainty is systematic.

Condensed Matter::Quantum GasesInclusiveSingle Differential Cross SectionDSIG/DHTPBAR P --> W+ JETS XPBAR P --> W- JETS XJet Production1960.0W Production
researchProduct

"Table 31" 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 HT 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 GasesInclusiveSingle Differential Cross SectionDijet ProductionDSIG/DHTPBAR P --> W+ JETS XPBAR P --> W- JETS XJet Production1960.0W Production
researchProduct

"Table 10" 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 lepton pseudorapidity 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 GasesInclusiveSingle Differential Cross SectionDijet ProductionHigh Energy Physics::PhenomenologyPBAR P --> W+ JETS XPBAR P --> W- JETS XHigh Energy Physics::ExperimentDSIG/DETARAPJet Production1960.0W Production
researchProduct