Çetin, Serkant Ali (Dogus Author)The differential cross section for the process Z/γ * → ℓℓ (ℓ = e, μ) as a function of dilepton invariant mass is measured in pp collisions at √s = 7 TeV at the LHC using the ATLAS detector. The measurement is performed in the e and μ channels for invariant masses between 26 GeV and 66 GeV using an integrated luminosity of 1.6 fb -1 collected in 2011 and these measurements are combined. The analysis is extended to invariant masses as low as 12 GeV in the muon channel using 35 pb-1 of data collected in 2010. The cross sections are determined within fiducial acceptance regions and corrections to extrapolate the measurements to the full kinematic range are provided. Next-to-next-to-leading- order QCD predictions...
The differential cross section for the process Z/�� * ��� ������ (��� = e, ��) as a function of dile...
See paper for full list of authors - 32 pages plus author list (53 pages total), 7 figures, 13 table...
The differential cross section for the process Z/γ (∗) → ℓℓ (ℓ = e, μ) as a function of dilepton inv...
The differential cross section for the process Z/γ ∗ → ℓℓ (ℓ = e, μ) as a function of dilepton invar...
The differential cross section for the process Z/γ * → ℓℓ (ℓ = e, μ) as a function of dilepton invar...
The differential cross section for the process Z/gamma* to l l (l = e, μ) as a function of dilepton ...
The differential cross section for the process Z/γ ∗ → ℓℓ (ℓ = e, μ) as a function of dilepton invar...
The differential cross section for the process Z/\u3b3 * \u2192 \u2113\u2113 (\u2113 = e, \u3bc) as ...
The differential cross section for the process Z/\u3b3 * \u2192 \u2113\u2113 (\u2113 = e, \u3bc) as ...
The differential cross section for the process Z/gamma* -> ll (l = e, mu) as a function of dilepton ...
The differential cross section for the process Z/�� * ��� ������ (��� = e, ��) as a function of dile...
See paper for full list of authors - 32 pages plus author list (53 pages total), 7 figures, 13 table...
The differential cross section for the process Z/γ (∗) → ℓℓ (ℓ = e, μ) as a function of dilepton inv...
The differential cross section for the process Z/γ ∗ → ℓℓ (ℓ = e, μ) as a function of dilepton invar...
The differential cross section for the process Z/γ * → ℓℓ (ℓ = e, μ) as a function of dilepton invar...
The differential cross section for the process Z/gamma* to l l (l = e, μ) as a function of dilepton ...
The differential cross section for the process Z/γ ∗ → ℓℓ (ℓ = e, μ) as a function of dilepton invar...
The differential cross section for the process Z/\u3b3 * \u2192 \u2113\u2113 (\u2113 = e, \u3bc) as ...
The differential cross section for the process Z/\u3b3 * \u2192 \u2113\u2113 (\u2113 = e, \u3bc) as ...
The differential cross section for the process Z/gamma* -> ll (l = e, mu) as a function of dilepton ...
The differential cross section for the process Z/�� * ��� ������ (��� = e, ��) as a function of dile...
See paper for full list of authors - 32 pages plus author list (53 pages total), 7 figures, 13 table...
The differential cross section for the process Z/γ (∗) → ℓℓ (ℓ = e, μ) as a function of dilepton inv...