Search results for "dijet production"
showing 10 items of 348 documents
"Table 33" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detec…
2013
The mean number of jets as a function of the rapidity difference between the boundary jets for boundary jets that have a mean transverse momentum in the range [150,180] GeV . Data are shown for the dijet Forward/Backward selection with a dijet veto energy, Q0, set equal to the mean transverse momentum of the boundary jets.
"Table 34" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detec…
2013
The mean number of jets as a function of the rapidity difference between the boundary jets for boundary jets that have a mean transverse momentum in the range [180,210] GeV . Data are shown for the dijet Forward/Backward selection with a dijet veto energy, Q0, set equal to the mean transverse momentum of the boundary jets.
"Table 32" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detec…
2013
The mean number of jets as a function of the rapidity difference between the boundary jets for boundary jets that have a mean transverse momentum in the range [120,150] GeV . Data are shown for the dijet Forward/Backward selection with a dijet veto energy, Q0, set equal to the mean transverse momentum of the boundary jets.
"Table 35" of "Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detec…
2013
The mean number of jets as a function of the rapidity difference between the boundary jets for boundary jets that have a mean transverse momentum in the range [210,240] GeV . Data are shown for the dijet Forward/Backward selection with a dijet veto energy, Q0, set equal to the mean transverse momentum of the boundary jets.
"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.
"Table 7" 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 Exclusive jet multiplicity, M(jj)>350, Dy(jj) >3.0. The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.
"Table 14" 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 pT(2nd jet)/pT(leading jet)). The first (sys) error is the uncorrelated systematic error and the second the correlated systematic error.