• Nenhum resultado encontrado

[PDF] Top 20 Measurement of neutral strange particle production in the underlying event in proton-proton collisions at sqrt(s) = 7 TeV

Has 10000 "Measurement of neutral strange particle production in the underlying event in proton-proton collisions at sqrt(s) = 7 TeV" found on our website. Below are the top 20 most common "Measurement of neutral strange particle production in the underlying event in proton-proton collisions at sqrt(s) = 7 TeV".

Measurement of neutral strange particle production in the underlying event in proton-proton collisions at sqrt(s) = 7 TeV

Measurement of neutral strange particle production in the underlying event in proton-proton collisions at sqrt(s) = 7 TeV

... FAPESP); the Bulgarian Ministry of Education, Youth and Science; CERN; the Chinese Academy of Sciences, Ministry of Science and Technology, and National Natural Science Foundation ... See full document

35

Measurement of the t-tbar production cross section in the e-mu channel in proton-proton collisions at sqrt(s) = 7 and 8 TeV

Measurement of the t-tbar production cross section in the e-mu channel in proton-proton collisions at sqrt(s) = 7 and 8 TeV

... evaluating the quantity at three values λm = 0, 1, − 1, corresponding to the nominal value of the parameter and to ± 1 standard deviation (σ) ...sources of uncertainty, only one ... See full document

52

Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector

Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector

... C. Chen 64 , H. Chen 25 , K. Chen 148 , L. Chen 33d,i , S. Chen 33c , X. Chen 33f , Y. Chen 67 , H.C. Cheng 89 , Y. Cheng 31 , A. Cheplakov 65 , E. Cheremushkina 130 , R. Cherkaoui El Moursli 135e , V. Chernyatin 25,∗ , ... See full document

34

Measurement of $b$-hadron pair production with the ATLAS detector in proton-proton collisions at $\sqrt{s}=8$ TeV

Measurement of $b$-hadron pair production with the ATLAS detector in proton-proton collisions at $\sqrt{s}=8$ TeV

... consists of an inner tracking system, referred to as the inner detector, sur- rounded by a superconducting solenoid, electromagnetic and hadronic calorimeters and an external muon ...tracks in ... See full document

49

Measurement of the top quark pair production charge asymmetry in proton-proton collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector

Measurement of the top quark pair production charge asymmetry in proton-proton collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector

... and the efficiency of an event produced in the true bin t to be reconstructed in any bin ...r. The background in each bin is taken into account when computing L ... See full document

45

Measurement of the top quark pair production cross section in proton-proton collisions at $\sqrt(s) =$ 13 TeV

Measurement of the top quark pair production cross section in proton-proton collisions at $\sqrt(s) =$ 13 TeV

... simulation. The scaling from the SS control region in data to the signal region is performed using an extrapolation factor, extracted from MC simulation, given by the ratio of ... See full document

18

Exclusive photon-photon production of muon pairs in proton-proton collisions at $\sqrt{s}=7$ TeV

Exclusive photon-photon production of muon pairs in proton-proton collisions at $\sqrt{s}=7$ TeV

... 4.0 event generator [9, 10] is used to produce simulated samples of two-photon production of muon ...pairs. The generator uses full leading-order QED matrix elements, and the ... See full document

35

Observation of a diffractive contribution to dijet production in proton-proton collisions at $\sqrt{s}=7$ TeV

Observation of a diffractive contribution to dijet production in proton-proton collisions at $\sqrt{s}=7$ TeV

... fraction of the total inelastic proton-proton cross section at high energies is at- tributed to diffractive processes, characterised by the presence of a large ... See full document

35

Measurement of charged-particle event shape variables in $\sqrt{s}=7$ TeV proton-proton interactions with the ATLAS detector

Measurement of charged-particle event shape variables in $\sqrt{s}=7$ TeV proton-proton interactions with the ATLAS detector

... The measurement of charged-particle event shape variables is presented in inclusive inelastic pp collisions at a center-of-mass energy of 7 ... See full document

56

Measurement of the triple-differential cross section for photon+jets production in proton-proton collisions at $\sqrt{s}$=7 TeV

Measurement of the triple-differential cross section for photon+jets production in proton-proton collisions at $\sqrt{s}$=7 TeV

... bining the photon and QCD parton multiplicity tree-level matrix elements with a QCD+QED parton shower using the formalism given in ...from the photon fragmentation compo- nent, permitting a ... See full document

33

Measurement of the $Z Z$ production cross section and limits on anomalous neutral triple gauge couplings in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Measurement of the $Z Z$ production cross section and limits on anomalous neutral triple gauge couplings in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... to the observed number of events. The sys- tematic errors are included as nuisance ...parameters. The resulting limits for each coupling, determined assuming real couplings and with the ... See full document

18

Search for Monotop Signatures in Proton-Proton Collisions at $\sqrt s =$ 8 TeV

Search for Monotop Signatures in Proton-Proton Collisions at $\sqrt s =$ 8 TeV

... Extensions of theories beyond the standard model (BSM), such as those with universal extra dimensions [1] or supersymmetry [2, 3], predict the existence of neutral massive particles ... See full document

29

Search for resonant $t \bar t$ production in proton-proton collisions at $\sqrt s=$ 8  TeV

Search for resonant $t \bar t$ production in proton-proton collisions at $\sqrt s=$ 8  TeV

... parameters of 0.8 (CA8 jets) and 1.5 (CA15 jets) for the analyses at high and low values of the t¯t invariant mass, ...respectively. The CA algorithm has been chosen because ... See full document

35

Measurement of differential cross sections for Z boson production in association with jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Measurement of differential cross sections for Z boson production in association with jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... The particle-flow (PF) algorithm [43] is used to reconstruct the ...combines the infor- mation from the various elements of the CMS detector to reconstruct and identify ... See full document

51

Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... determine the calibration of each CASTOR channel relative to the ...to the last two longitudinal channels, which have detector noise levels very close to the muon ionization peak and ... See full document

30

Jet energy measurement and its systematic uncertainty in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Jet energy measurement and its systematic uncertainty in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... made in this analysis with respect to what is reported in ...]. The dead material uncertainty, which is large in ...to the systematic uncertainty reported in ...change in ... See full document

100

Measurement of electroweak production of a W boson and two forward jets in proton-proton collisions at $ \sqrt{s}=8 $ TeV

Measurement of electroweak production of a W boson and two forward jets in proton-proton collisions at $ \sqrt{s}=8 $ TeV

... from the combination of the tracker and the corresponding ECAL cluster information, and must pass electron identification requirements according to a multi- variate identification technique ... See full document

36

Measurement of charged particle spectra in minimum-bias events from proton–proton collisions at $\sqrt{s}=13\,\text {TeV} $

Measurement of charged particle spectra in minimum-bias events from proton–proton collisions at $\sqrt{s}=13\,\text {TeV} $

... study of the properties of particle production without any selection bias arising from re- quiring the presence of a hard scattering (a selection known as ”minimum bias”) ... See full document

38

Search for excited leptons in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Search for excited leptons in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... (SM) of particle physics is an extremely successful effective theory which has been ex- tensively tested over the past forty ...number of fundamental questions are left unanswered. In ... See full document

22

The performance of the CMS muon detector in proton-proton collisions at sqrt(s) = 7 TeV at the LHC

The performance of the CMS muon detector in proton-proton collisions at sqrt(s) = 7 TeV at the LHC

... within the chambers with a precision sufficient to set sharp transverse momentum (p T ) thresholds at the level-1 (L1) trigger level up to 100 GeV/c, and to tag the parent bunch crossing with ... See full document

101

Show all 10000 documents...