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CMS beam spot center coordinates for collisions at 13 TeV.Data were taken with CMS magnet at 3.8 T (black dots), 2.8 T (green dots) or 0 T (red dots). The error bars indicate the statistical uncertainty from the fit. |
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Comparison of the primary vertex resolution in Y vs pT sum of the associated tracks for four different data taking: 7 TeV (50 ns), 8 TeV (50 ns), 13 TeV (50 and 25 ns).
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Data (black dots) and simulation (light blue rectangles) tracking efficiency for muons coming from the Z decay as a function of the absolute pseudorapidity(top), the phi (center) and the number of primary vertexes(bottom) of the probe muon. |
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Data (dots) and simulation (rectangles) tracking efficiency for muons as a function of the transverse momentum of the probe muon for tracks reconstructed with tracker info only in purple as well as the tracks reconstructed with tracker and muon seeded in blue and black. |
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The D0 -> K3π decay has a complex structure due to the interference of different intermediate states in two or three bodies that could affect the final efficiency. The previous analysis considered it as systematics uncertainty, we used a strategy to correct the final measurement. We have to assign the proper efficiency to each event. The kinematics of a spin-0 particle decaying in a four-body final state are fully described by five invariant quantities. We choose the square of five invariant sub-mass: sij = (pi + pj)2 where pi,j is the particle momentum. Finally we define the function F(x)=m0+m1s1+m2s2+m3s3+m4s4+m5s5, a linear combination of the sub-mass states, that well describes the efficiency. Each event in the Nk3𝜋 final state is then weighted with the quantity 1/F. Comparison between the value of the function F(x) bin by bin (black) and the reconstruction efficiency in Monte Carlo sample (red). |
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ΔM=M^{D*}-M^{D0} distributions for Kπ (top) and K3π (bottom) for data, stream ZeroBias. The fitted shapes in blue well describe data point for both signal (solid) and background (dashed). |
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The ratio of tracking relative efficiencies for charged pions, as a function of the minimum D*% candidates pT threshold, is shown in three different pseudorapidity regions: barrel (top), transition (center) and endcap (bottom). |