Search results for "Z Production"
showing 10 items of 244 documents
"Table 1" of "Search for the production of a long-lived neutral particle decaying within the ATLAS hadronic calorimeter in association with a $Z$ bos…
2018
The product of acceptance and efficiency for all signal MC samples.
"Table 14" of "Charged particle multiplicity distributions in restricted rapidity intervals in Z0 hadronic decays."
1992
Multiplicity moments in central rapidity intervals.. CQ is defined as MEAN(MULT**Q)/MEAN(MULT)**Q.
"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.
"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.
"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.
"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.
"Table 24" of "Measurement of the production cross section of jets in association with a Z boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLA…
2015
The distribution of DR (jj). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.
"Table 22" of "Measurement of the production cross section of jets in association with a Z boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLA…
2015
The distribution of M(jj). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.
"Table 23" of "Measurement of the production cross section of jets in association with a Z boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLA…
2015
The distribution of DPhi (jj). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.
"Table 8" of "Measurement of the production cross section of jets in association with a Z boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS…
2015
The distribution of Ratio of successive exclusive jet multiplicities, M(jj)>350, Dy(jj) >3.0. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.