Search results for "Jet Production"
showing 10 items of 2071 documents
"Table 2" of "Search for Quark Contact Interactions in Dijet Angular Distributions in pp Collisions at sqrt(s) = 7 TeV Measured with the ATLAS Detect…
2010
CHI distribution for mass bin 520 to 800 GeV.
"Table 1" of "Search for Quark Contact Interactions in Dijet Angular Distributions in pp Collisions at sqrt(s) = 7 TeV Measured with the ATLAS Detect…
2010
CHI distribution for mass bin 340 to 520 GeV.
"Table 1" of "The scale dependence of the hadron multiplicity in quark and gluon jets and a precise determination of C(A)/C(F)."
1999
Charged multiplicity in events with a hard photon, as a function of the apparent centre-of-mass energy (SQRT(S)) of the hadronic system. The errors shown are statistical only.
"Table 2" of "The scale dependence of the hadron multiplicity in quark and gluon jets and a precise determination of C(A)/C(F)."
1999
Charged multiplicity in symmetric three jet events as function of the opening angle between the low energetic jets, THETA1. Jets are defined from charged and neutral particles using the DURHAM algorithm. The errors shown are statistical only.
"Table 11" of "Measurement of the forward-backward asymmetry in the distribution of leptons in $t\bar{t}$ events in the lepton+jets channel"
2014
Observed ASYMFB(LEPTON) at production level for the "lepton + >= 4 jets, >= 2 b-tags" channel.
"Table 2" of "Energy dependence of the differences between the quark and gluon jet fragmentation"
1998
Durham and JADE algoritms were used.
"Table 9" of "Search for Massive Colored Scalars in Four-Jet Final States in sqrt{s}=7 TeV proton-proton collisions with the ATLAS Detector"
1970
The observed 95% CL upper bounds on scalar pair production cross-section as a function of the scalar particle mass.
"Table 26" 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 in the gap as a function of the mean transverse momentum of the boundary jets for boundary jets that have a rapidity difference in the range [1,2], using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.
"Table 29" 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 in the gap as a function of the mean transverse momentum of the boundary jets for boundary jets that have a rapidity difference in the range [4,5], using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.
"Table 28" 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 in the gap as a function of the mean transverse momentum of the boundary jets for boundary jets that have a rapidity difference in the range [3,4], using a jet veto Q0 = 20 GeV. Data are shown for two dijet selections: (i) the dijet system is defined as the two leading-pT jets in the event (ii) the dijet system is defined as the most forward-backward jets in the event.