Search results for "DSI"
showing 10 items of 1457 documents
"Table 5" of "Measurement of the differential cross sections for isolated direct photon pair production in $p \bar p$ collisions at $\sqrt{s} = 1.96$…
2013
The measured differential distribution in the two-photon mass for |azimuthal angle separation| < PI/2;.
"Table 8" of "Measurement of the differential cross sections for isolated direct photon pair production in $p \bar p$ collisions at $\sqrt{s} = 1.96$…
2013
The measured differential distribution in the two-photon mass for |azimuthal angle separation| > PI/2;.
"Table 1" of "Measurement of the differential cross sections for isolated direct photon pair production in $p \bar p$ collisions at $\sqrt{s} = 1.96$…
2013
The measured differential distribution in the two-photon mass;.
"Table 2" of "Measurements of normalized differential cross-sections for ttbar production in pp collisions at sqrt(s) = 7 TeV using the ATLAS detecto…
2016
Normalized differential cross-sections for the mass of the ttbar system. The cross-section in each bin is given as the integral of the normalized differential cross-section over the bin width, divided by the bin width. The calculation of the cross-sections in the last bins includes events falling outside of the bin edges, and the normalization is done within the quoted bin width. The full covariance matrice is provided in Table 6 below.
"Table 8" of "Measurement of ZZ production in pp collisions at sqrt(s)=7 TeV and limits on anomalous ZZZ and ZZgamma couplings with the ATLAS detecto…
2014
Normalized ZZ fiducial cross section (multiplied by 10^6 for readability) in bins of the transverse mass of the ZZ system for the 2l2nu channel. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties.
"Table 7" of "Measurement of ZZ production in pp collisions at sqrt(s)=7 TeV and limits on anomalous ZZZ and ZZgamma couplings with the ATLAS detecto…
2014
Normalized ZZ fiducial cross section (multiplied by 10^6 for readability) in bins of the mass of the ZZ system for the 4l channel. The first systematic uncertainty is detector systematics, the second is background systematic uncertainties.
"Table 7" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."
2000
Oblateness O.
"Table 2" of "Precise study of the Z/gamma* boson transverse momentum distribution in ppbar collisions using a novel technique"
2011
The measured PHI* distributions for the dimuon events corrected back to the particle level. The distributions are normalised to unity inidividually for each abs(yrap) bin and channel.
"Table 7" of "Measurement of $Z / \gamma^\ast +jet+X$ angular distributions in $p \bar{p}$ collisions at $\sqrt{s}=1.96$ TeV"
2009
Individual percentage contributions to the systematic error for the binning in PHI(P=3)-PHI(P=4) for Z/GAMMA* transverse momentum > 25 GeV.
"Table 2" of "Measurement of $Z / \gamma^\ast +jet+X$ angular distributions in $p \bar{p}$ collisions at $\sqrt{s}=1.96$ TeV"
2009
Differential cross section in bins of PHI(P=3)-PHI(P=4) for Z/GAMMA* transverse momentum > 45 GeV.