• No results found

[PDF] Top 20 Luminosity determination in pp collisions at root s=7 TeV using the ATLAS detector at the LHC

Has 10000 "Luminosity determination in pp collisions at root s=7 TeV using the ATLAS detector at the LHC" found on our website. Below are the top 20 most common "Luminosity determination in pp collisions at root s=7 TeV using the ATLAS detector at the LHC".

Luminosity determination in pp collisions at root s=7 TeV using the ATLAS detector at the LHC

Luminosity determination in pp collisions at root s=7 TeV using the ATLAS detector at the LHC

... In contrast, the track-counting luminosities obtained using the three track selections defined in Sect. 3.2 exhibit a noticeable relative non-linearity (Fig. 16(a)). The pattern is consistent with that observed in ... See full document

72

Luminosity determination in pp collisions at √s = 8 TeV using the ATLAS detector at the LHC

Luminosity determination in pp collisions at √s = 8 TeV using the ATLAS detector at the LHC

... the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Ger- many), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Taiwan), RAL (UK) and BNL ... See full document

45

Improved luminosity determination in pp collisions at √s=7 TeV using the ATLAS detector at the LHC

Improved luminosity determination in pp collisions at √s=7 TeV using the ATLAS detector at the LHC

... FCal luminosity determinations do not de- pend upon event counting, but rather upon measuring detec- tor currents that are proportional to the total particle flux in specific regions of the ...Tile ... See full document

40

Search for pair production of massive particles decaying into three quarks with the ATLAS detector in √s=7 TeV pp collisions at the LHC

Search for pair production of massive particles decaying into three quarks with the ATLAS detector in √s=7 TeV pp collisions at the LHC

... Several triggers are used to select events for the signal and control regions studied for this analysis channel. In each case, the triggers are intended to select jets with at least 30 GeV of transverse momentum. This ... See full document

43

Search for a heavy narrow resonance decaying to eμ, eτ, or μτ with the ATLAS detector in √s=7 TeV pp collisions at the LHC

Search for a heavy narrow resonance decaying to eμ, eτ, or μτ with the ATLAS detector in √s=7 TeV pp collisions at the LHC

... The dominant sources of systematic uncertainty for the back- ground predictions arise from the statistical uncertainty on the W + jets and multijet background determinations from data, a 10% uncertainty on extrapolation ... See full document

19

Search for strong gravity in multijet final states produced in pp collisions at root s=13 TeV using the ATLAS detector at the LHC

Search for strong gravity in multijet final states produced in pp collisions at root s=13 TeV using the ATLAS detector at the LHC

... Since black holes and string balls are expected to decay predominantly to quarks and gluons, the search is simplified by considering only jets. The analysis uses jets of hadrons, as well as misidentified jets arising ... See full document

38

Search for contact interactions in dilepton events from pp collisions at root s=7 TeV with the ATLAS detector

Search for contact interactions in dilepton events from pp collisions at root s=7 TeV with the ATLAS detector

... A. Macchiolo 99 , B. Maˇcek 74 , J. Machado Miguens 124a , R. Mackeprang 35 , R.J. Madaras 14 , W.F. Mader 43 , R. Maenner 58c , T. Maeno 24 , P. Mättig 174 , S. Mättig 41 , L. Magnoni 29 , E. Magradze 54 , Y. ... See full document

19

Measurement of event-shape observables in Z→ℓ+ℓ- events in pp collisions at √s=7 TeV with the ATLAS detector at the LHC

Measurement of event-shape observables in Z→ℓ+ℓ- events in pp collisions at √s=7 TeV with the ATLAS detector at the LHC

... the LHC at √ s = 13 ...the LHC, as well as the support staff from our institutions with- out whom ATLAS could not be operated ...the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF ... See full document

40

Measurement of the isolated diphoton cross section in pp collisions at √s=7 TeV with the ATLAS detector

Measurement of the isolated diphoton cross section in pp collisions at √s=7 TeV with the ATLAS detector

... the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated ...the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 ... See full document

29

Search for the Dimuon Decay of the Higgs Boson in pp Collisions at root s=13 TeV with the ATLAS Detector

Search for the Dimuon Decay of the Higgs Boson in pp Collisions at root s=13 TeV with the ATLAS Detector

... R. M. Barnett, 16 Z. Barnovska-Blenessy, 36a A. Baroncelli, 136a G. Barone, 25 A. J. Barr, 122 L. Barranco Navarro, 170 F. Barreiro, 85 J. Barreiro Guimarães da Costa, 35a R. Bartoldus, 145 A. E. Barton, 75 P. Bartos, ... See full document

20

Measurement of the ZZ Production Cross Section in pp Collisions at root s=13 TeV with the ATLAS Detector

Measurement of the ZZ Production Cross Section in pp Collisions at root s=13 TeV with the ATLAS Detector

... In pp collisions at a center-of-mass energy of p ffiffiffi s ¼ 13 TeV, ZZ production is dominated by quark-antiquark (q q) interactions, with an ¯ Oð10%Þ contribution from loop-induced gluon-gluon ... See full document

19

Search for high mass dilepton resonances in pp collisions at root s = 8 TeV with the ATLAS detector

Search for high mass dilepton resonances in pp collisions at root s = 8 TeV with the ATLAS detector

... In the context of models with extra dimensions, semi- classical black holes can be formed at a collider if the available energy is well above the higher-dimensional Planck scale [32,33]. Such black holes would then decay ... See full document

31

Search for third generation scalar leptoquarks in pp collisions at √s=7 TeV with the ATLAS detector

Search for third generation scalar leptoquarks in pp collisions at √s=7 TeV with the ATLAS detector

... accurate determination of the normalisation factors compared to the event-counting method employed in the electron channel, and the normalisation factor uncertainty for the muon channel is correspondingly smaller ... See full document

41

Measurement of isolated photon pair production in pp collisions at √s=7 TeV with the ATLAS detector

Measurement of isolated photon pair production in pp collisions at √s=7 TeV with the ATLAS detector

... the detector-level selection criteria divided by the number of generated events satisfying the equivalent truth-level criteria, thus correcting for reconstructed events with true photons failing the acceptance ... See full document

43

Search for dilepton resonances in pp collisions at √s=7 TeV with the ATLAS detector

Search for dilepton resonances in pp collisions at √s=7 TeV with the ATLAS detector

... the ATLAS experiment in pp collisions at p ffiffiffi s ¼ 7 TeV at the Large Hadron Collider and correspond to a total integrated luminosity of ...1.83 TeV on the ... See full document

20

Measurement of the W-boson mass in pp collisions at root s=7 TeV with the ATLAS detector

Measurement of the W-boson mass in pp collisions at root s=7 TeV with the ATLAS detector

... F. Lo Sterzo 153 , E.M. Lobodzinska 45 , P. Loch 7 , F.K. Loebinger 87 , K.M. Loew 25 , A. Loginov 179,∗ , T. Lohse 17 , K. Lohwasser 45 , M. Lokajicek 129 , B.A. Long 24 , J.D. Long 169 , R.E. Long 75 , L. Longo ... See full document

86

Search for a heavy particle decaying into an electron and a muon with the ATLAS detector in √s=7 TeV pp collisions at the LHC

Search for a heavy particle decaying into an electron and a muon with the ATLAS detector in √s=7 TeV pp collisions at the LHC

... An e resonance can be generated in models containing a heavy neutral gauge boson with nondiagonal lepton flavor couplings Z 0 [24]. Very stringent limits on the com- bination of the mass and the coupling to ee and e of ... See full document

19

Measurement of the W-boson mass in pp collisions at root s=7 TeV with the ATLAS detector

Measurement of the W-boson mass in pp collisions at root s=7 TeV with the ATLAS detector

... S. L. Barnes 36c , B. M. Barnett 133 , R. M. Barnett 16 , Z. Barnovska-Blenessy 36a , A. Baroncelli 136a , G. Barone 25 , A. J. Barr 122 , L. Barranco Navarro 170 , F. Barreiro 85 , J. Barreiro Guimarães da Costa ... See full document

61

Search for Dilepton Resonances in pp Collisions at √s=7  TeV with the ATLAS Detector

Search for Dilepton Resonances in pp Collisions at √s=7  TeV with the ATLAS Detector

... the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated ...the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden),CC-IN2P3 ... See full document

19

Measurement of the W-boson mass in pp collisions at root s=7 TeV with the ATLAS detector

Measurement of the W-boson mass in pp collisions at root s=7 TeV with the ATLAS detector

... V. Chernyatin 27,* , E. Cheu 7 , L. Chevalier 138 , V. Chiarella 50 , G. Chiarelli 126a,126b , G. Chiodini 76a , A. S. Chisholm 32 , A. Chitan 28b , Y. H. Chiu 172 , M. V. Chizhov 68 , K. Choi 64 , A. R. ... See full document

14

Show all 10000 documents...