A measurement of the Drell-Yan differential cross section at low invariant mass is presented in the di-muon channel. A 1.64 pb$^{-1}$ dataset of $\sqrt{s}=7$ TeV proton-proton collision data collected by the ATLAS experiment at the LHC is used. The measurement is made in an invariant mass range of $26 < M_{\mu\mu} < 66$ GeV where $M_{\mu\mu}$ is the invariant mass of the muon pair. A review of the relevant theoretical physics and the ATLAS detector is made. The analysis is described with particular attention paid to the determination of the isolation efficiency corrections for the Monte Carlo and the estimate of the multijet background. The fiducial differential cross section is calculated with a statistical uncertainty that varies between ...
LHC proton-proton collisions at a centre of mass energy of √s = 7 TeV were observed in 2011. From...
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...
PhDA measurement of the Drell-Yan di fferential cross section at low invariant mass is presented in ...
The differential cross section for the process Z/gamma* -> ll (l = e, mu) as a function of dilept...
The low mass Drell-Yan di-muon process is investigated with the ATLAS detector at the LHC, in order ...
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...
Çetin, Serkant Ali (Dogus Author)The differential cross section for the process Z/γ * → ℓℓ (ℓ = e, μ...
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 ...
LHC proton-proton collisions at a centre of mass energy of √s = 7 TeV were observed in 2011. From...
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...
PhDA measurement of the Drell-Yan di fferential cross section at low invariant mass is presented in ...
The differential cross section for the process Z/gamma* -> ll (l = e, mu) as a function of dilept...
The low mass Drell-Yan di-muon process is investigated with the ATLAS detector at the LHC, in order ...
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...
Çetin, Serkant Ali (Dogus Author)The differential cross section for the process Z/γ * → ℓℓ (ℓ = e, μ...
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 ...
LHC proton-proton collisions at a centre of mass energy of √s = 7 TeV were observed in 2011. From...
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...