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[PDF] Top 20 Measurement of the $\Lambda_b$ polarization and angular parameters in $\Lambda_b\to J/\psi\, \Lambda$ decays from pp collisions at $\sqrt{s}=$ 7 and 8 TeV

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Measurement of the $\Lambda_b$ polarization and angular parameters in $\Lambda_b\to J/\psi\, \Lambda$ decays from pp collisions at $\sqrt{s}=$ 7 and 8 TeV

Measurement of the $\Lambda_b$ polarization and angular parameters in $\Lambda_b\to J/\psi\, \Lambda$ decays from pp collisions at $\sqrt{s}=$ 7 and 8 TeV

... DATA AND SIMULATED EVENTS We use data collected with a trigger designed for events containing a J=ψ meson decaying to two muons that form a displaced vertex relative to the mean ... See full document

20

Measurement of the production cross-section of $\psi(2S) \to J/\psi ( \to \mu^{+} \mu^{-}) \pi^{+} \pi^{-}$ in pp collisions at $ \sqrt{s} $ = 7 TeV at ATLAS

Measurement of the production cross-section of $\psi(2S) \to J/\psi ( \to \mu^{+} \mu^{-}) \pi^{+} \pi^{-}$ in pp collisions at $ \sqrt{s} $ = 7 TeV at ATLAS

... models of prompt ψ(2S) production vary significantly in their predictions of overall rate and kinematic ...found to describe the data satisfactorily across the full range ... See full document

58

Measurement of the X(3872) production cross section via decays to J/psi pi pi in pp collisions at sqrt(s) = 7 TeV

Measurement of the X(3872) production cross section via decays to J/psi pi pi in pp collisions at sqrt(s) = 7 TeV

... The measurement is found to be stable with respect to variations of the pseudo-proper-decay- length requirement between 50 and 250 ...Application of the same ... See full document

35

Measurement of $\tau$ polarization in $W -> \tau \nu$ decays with the ATLAS detector in pp collisions at sqrt(s) = 7 TeV

Measurement of $\tau$ polarization in $W -> \tau \nu$ decays with the ATLAS detector in pp collisions at sqrt(s) = 7 TeV

... contained in a 2 T magnetic field providing charged particle position and momentum measurements, a calorimeter system for en- ergy measurements of charged and neutral particles, and a ... See full document

25

Angular analysis of $B^0_d \rightarrow K^{*}\mu^+\mu^-$ decays in $pp$ collisions at $\sqrt{s}= 8$ TeV with the ATLAS detector

Angular analysis of $B^0_d \rightarrow K^{*}\mu^+\mu^-$ decays in $pp$ collisions at $\sqrt{s}= 8$ TeV with the ATLAS detector

... vetoed to remove any potential contamination from the φ(1020) ...resonance. The remaining data with q 2 ∈ [0.04, 6.0] GeV 2 are analysed in order to extract the signal ... See full document

47

Angular analysis of the decay $B^0 \to K^{*0} \mu^+ \mu^-$ from pp collisions at $\sqrt  s = 8$ TeV

Angular analysis of the decay $B^0 \to K^{*0} \mu^+ \mu^-$ from pp collisions at $\sqrt s = 8$ TeV

... used in the analysis accommodates cases in which the kaon and pion charges are correctly and incorrectly ...Both of these contributions are treated as signal. The ... See full document

36

Observation of the decay $B^+ \to \psi(2S) \phi(1020) K^+$ in pp collisions at $\sqrt s =$ 8 TeV

Observation of the decay $B^+ \to \psi(2S) \phi(1020) K^+$ in pp collisions at $\sqrt s =$ 8 TeV

... production at the CERN LHC and the high luminosity of the accelerator provide the possibility to study rare B meson ...reported the likely presence of ... See full document

28

Measurement of the mass of the top quark in decays with a $J/\psi$ meson in pp collisions at 8 TeV

Measurement of the mass of the top quark in decays with a $J/\psi$ meson in pp collisions at 8 TeV

... erator, and the MLM prescription [18] is used for matching of matrix-element jets to parton ...showers. The Lund string model [19] is used for the simulation of the ... See full document

36

Measurements of $\psi(2S)$ and $X(3872) \to J/\psi\pi^+\pi^-$ production in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector

Measurements of $\psi(2S)$ and $X(3872) \to J/\psi\pi^+\pi^-$ production in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector

... a measurement of the di fferential cross sections for the production of ψ(2S ) and X(3872) states in the decay channel J/ψπ + π − is performed, using ...−1 ... See full document

42

Combined Measurement of the Higgs Boson Mass in $pp$ Collisions at $\sqrt{s}=7$ and 8 TeV with the ATLAS and CMS Experiments

Combined Measurement of the Higgs Boson Mass in $pp$ Collisions at $\sqrt{s}=7$ and 8 TeV with the ATLAS and CMS Experiments

... importance of the various sources of systematic uncertainty is further investigated by dividing the nuisance parameters into yet-finer groups, with each group associated with a specific ... See full document

47

Measurement of the WZ production cross section in pp collisions at $\sqrt{s} = 7$ and 8 $\,\text{TeV}$ and search for anomalous triple gauge couplings at $\sqrt{s} = 8\,\text{TeV} $

Measurement of the WZ production cross section in pp collisions at $\sqrt{s} = 7$ and 8 $\,\text{TeV}$ and search for anomalous triple gauge couplings at $\sqrt{s} = 8\,\text{TeV} $

... leptons from W and Z boson decays are mostly isolated from other final-state par- ticles in the ...Consequently, the selected leptons are required to be isolated ... See full document

44

Measurement of the prompt J/ $\psi $ pair production cross-section in pp collisions at $\sqrt{s} = 8$  TeV with the ATLAS detector

Measurement of the prompt J/ $\psi $ pair production cross-section in pp collisions at $\sqrt{s} = 8$  TeV with the ATLAS detector

... full and detailed description of the ATLAS detector can be found in ...]. The inner detector (ID) is composed of the pixel detector, the semiconductor tracker ... See full document

53

Measurement of the ratio $B(B^0_s \to J/\psi f_0(980))$ / $B(B^0_s \to J/\psi \phi(1020))$ in pp collisions at $\sqrt s$ = 7 TeV

Measurement of the ratio $B(B^0_s \to J/\psi f_0(980))$ / $B(B^0_s \to J/\psi \phi(1020))$ in pp collisions at $\sqrt s$ = 7 TeV

... support from the Marie-Curie programme and the European Re- search Council and EPLANET (European Union); the Leventis Foundation; the ...Foundation; the Alexander ... See full document

27

Measurement of prompt $J/\psi$ pair production in pp collisions at $ \sqrt{s} $ = 7 Tev

Measurement of prompt $J/\psi$ pair production in pp collisions at $ \sqrt{s} $ = 7 Tev

... efficiency to trigger and reconstruct J/ψ pair events relies on detector ...simulation. To evaluate the uncertainty event-based efficiency values are instead constructed from ... See full document

33

Measurement of the prompt $J/\psi$ and $\psi$(2S) polarizations in $pp$ collisions at $\sqrt{s}$ = 7 TeV

Measurement of the prompt $J/\psi$ and $\psi$(2S) polarizations in $pp$ collisions at $\sqrt{s}$ = 7 TeV

... colleagues in the CERN accelerator departments for the excellent perfor- mance of the LHC and thank the technical and administrative staffs at CERN ... See full document

49

Measurement of the $\Lambda_b$ cross section and the $_{\bar{\Lambda}_b}$ to $\Lambda_b$ ratio with $J/\Psi \Lambda$ decays in $pp$ collisions at $\sqrt{s}=7$ TeV

Measurement of the $\Lambda_b$ cross section and the $_{\bar{\Lambda}_b}$ to $\Lambda_b$ ratio with $J/\Psi \Lambda$ decays in $pp$ collisions at $\sqrt{s}=7$ TeV

... surements of B + [6], B 0 [7], and B 0 s [9] production cross sections also performed by the Compact Muon Solenoid (CMS) experiment at the LHC ...[18]. The ... See full document

33

Measurement of inclusive jet and dijet production in $pp$ collisions at $\sqrt{s}=7$ TeV using the ATLAS detector

Measurement of inclusive jet and dijet production in $pp$ collisions at $\sqrt{s}=7$ TeV using the ATLAS detector

... compared to the matched reconstructed spectrum from the Monte Carlo ...simulation. In the sec- ond step, the iterated unfolding matrix A ptcl,i reco,j is deter- ... See full document

54

Measurement of the mass difference between top quark and antiquark in pp collisions at $\sqrt{s} = 8$ TeV

Measurement of the mass difference between top quark and antiquark in pp collisions at $\sqrt{s} = 8$ TeV

... both in the data and simulation ...achieved at the reconstructed particle level with only weak pileup ...Jets in the data have an additional residual correction that is ... See full document

31

Searches for long-lived charged particles in pp collisions at $\sqrt{s}$=7 and 8 TeV

Searches for long-lived charged particles in pp collisions at $\sqrt{s}$=7 and 8 TeV

... recorded at collision energies of 7 and 8 ...only the inner tracker, a search with both the inner tracker and the muon system, a search with only the ... See full document

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Phenomenological MSSM interpretation of CMS searches in pp collisions at sqrt(s) = 7 and 8 TeV

Phenomenological MSSM interpretation of CMS searches in pp collisions at sqrt(s) = 7 and 8 TeV

... Hungary; the Department of Atomic Energy and the Department of Science and Technology, India; the Institute for Studies in Theoretical Physics and ... See full document

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