Search results for "DSI"

showing 10 items of 1457 documents

"Table 28" of "Measurement of top quark pair differential cross-sections in the dilepton channel in $pp$ collisions at $\sqrt{s}$ = 7 and 8 TeV with …

2017

Statistical bin-to-bin correlations in the normalized $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 8 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

InclusiveDSIG/DMProton-Proton ScatteringDifferential Cross SectionHigh Energy Physics::PhenomenologyTopTop ProductionHigh Energy Physics::ExperimentP P --> TOP TOPBAR X
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"Table 31" of "Measurement of top quark pair differential cross-sections in the dilepton channel in $pp$ collisions at $\sqrt{s}$ = 7 and 8 TeV with …

2017

Statistical bin-to-bin correlations in the absolute $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 7 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

InclusiveDSIG/DMProton-Proton ScatteringDifferential Cross SectionHigh Energy Physics::PhenomenologyTopTop ProductionHigh Energy Physics::ExperimentP P --> TOP TOPBAR X
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"Table 34" of "Measurement of top quark pair differential cross-sections in the dilepton channel in $pp$ collisions at $\sqrt{s}$ = 7 and 8 TeV with …

2017

Statistical bin-to-bin correlations in the absolute $t\bar t$ differential cross-sections for $t\bar t$ system mass $m_{t\bar t}$ at $\sqrt{s}$ = 8 TeV. The off-diagonal correlations mainly due to bin migrations in unfolding and the normalization condition.

InclusiveDSIG/DMProton-Proton ScatteringDifferential Cross SectionHigh Energy Physics::PhenomenologyTopTop ProductionHigh Energy Physics::ExperimentP P --> TOP TOPBAR X
researchProduct

"Table 6" of "Measurements of normalized differential cross-sections for ttbar production in pp collisions at sqrt(s) = 7 TeV using the ATLAS detecto…

2016

Bin-wise full covariance matrices for the normalized differential cross-sections of the mass of the ttbar system. The elements of the covariance matrices are in units of TeV$^{-2}$.

InclusiveDSIG/DMProton-Proton ScatteringHigh Energy Physics::PhenomenologyStatistics::MethodologyHigh Energy Physics::ExperimentP P --> TOP TOPBAR X
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"Table 19" of "Measurements of $W^\pm Z$ production cross sections in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector and limits on ano…

2016

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

InclusiveDSIG/DMTWZ8000.0Proton-Proton ScatteringZ ProductionDifferential Cross SectionAstrophysics::Cosmology and Extragalactic AstrophysicsW ProductionP P --> W+ Z0 X
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"Table 34" of "Measurements of $W^\pm Z$ production cross sections in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector and limits on ano…

2016

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

InclusiveDSIG/DMTWZ8000.0Proton-Proton ScatteringZ ProductionDifferential Cross SectionP P --> (W+ + W-) Z0 XAstrophysics::Cosmology and Extragalactic Astrophysics
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"Table 18" of "Measurements of $W^\pm Z$ production cross sections in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector and limits on ano…

2016

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

InclusiveDSIG/DMTWZ8000.0Proton-Proton ScatteringZ ProductionDifferential Cross SectionP P --> (W+ + W-) Z0 XAstrophysics::Cosmology and Extragalactic Astrophysics
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"Table 20" of "Measurements of $W^\pm Z$ production cross sections in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector and limits on ano…

2016

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

InclusiveDSIG/DMTWZ8000.0Proton-Proton ScatteringZ ProductionDifferential Cross SectionP P --> W- Z0 XAstrophysics::Cosmology and Extragalactic AstrophysicsW Production
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"Table 4" of "First Measurement of the Muon Neutrino Charged Current Single Pion Production Cross Section on Water with the T2K Near Detector"

2016

Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $p_\mu$ in the reduced phase-space of $p_{\pi^+} > 200$ MeV/$c$, $p_\mu > 200$ MeV/c, $\cos(\theta_{\pi^+}) > 0.3$ and $\cos(\theta_\mu) > 0.3$.

InclusiveDSIG/DPDifferential Cross SectionDeep Inelastic ScatteringCharged CurrentNUMU NUCLEON --> MU- PI+ XMuon Production
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"Table 2" of "First Measurement of the Muon Neutrino Charged Current Single Pion Production Cross Section on Water with the T2K Near Detector"

2016

Unfolded $\nu_\mu$ CC1$\pi^+$ differential cross section as a function of $p_\pi$ in the reduced phase-space of $p_{\pi^+} > 200$ MeV/$c$, $p_\mu > 200$ MeV/c, $\cos(\theta_{\pi^+}) > 0.3$ and $\cos(\theta_\mu) > 0.3$.

InclusiveDSIG/DPDifferential Cross SectionDeep Inelastic ScatteringCharged CurrentNUMU NUCLEON --> MU- PI+ XMuon Production
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