Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead lead collisions at root S NN=2 76 TeV with the ATLAS detector

s = 7 and 8 TeV in the Compact Muon Solenoid experiment at the LHC, using data samples corresponding to integrated luminosities of up to 5.1 fb − 1 at 7 TeV and 5.3 fb − 1 at 8 TeV.

56: Also at KFKI Research Institute for Particle and Nuclear Physics, Budapest, Hungary 57: Also at Kyungpook National University,

For PbPb collisions, an additional sys- tematic uncertainty is assessed by taking the difference between applying and not applying the correction for different values of R AA

The parametrisation of the interpolating functions φ k (m b ) describing the dependence of the differential b-jet shapes with the b-quark mass is done using second-order polynomials

The nc 2 {4, ΣE T } in ultra-central collisions calculated for charged particles as a function of centrality (left panel), ΣE T (middle panel), and N ch rec (right panel) with

These searches are dubbed resonant, since they allow to directly probe B(Υ → γa) in a model-independent way, regardless of the non-resonant contribution from figure 1. Searches

41: Also at Adiyaman University, Adiyaman, Turkey 42: Also at Izmir Institute of Technology, Izmir, Turkey 43: Also at The University of Iowa, Iowa City, USA 44: Also at

59: Also at KFKI Research Institute for Particle and Nuclear Physics, Budapest, Hungary 60: Also at Kyungpook National University,