[PDF] Top 20 Measurement of the charged-particle multiplicity inside jets from $\sqrt{s}=8$ TeV $pp$ collisions with the ATLAS detector
Has 10000 "Measurement of the charged-particle multiplicity inside jets from $\sqrt{s}=8$ TeV $pp$ collisions with the ATLAS detector" found on our website. Below are the top 20 most common "Measurement of the charged-particle multiplicity inside jets from $\sqrt{s}=8$ TeV $pp$ collisions with the ATLAS detector".
Measurement of the charged-particle multiplicity inside jets from $\sqrt{s}=8$ TeV $pp$ collisions with the ATLAS detector
... Given the jet p T , the charged particle multiplicity inside jets does not vary significantly with ...that the solution to Eq. 1 reproduces the quark ... See full document
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Measurement of the prompt J/ $\psi $ pair production cross-section in pp collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
... acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, ... See full document
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Measurement of charged-particle distributions sensitive to the underlying event in $ \sqrt{s}=13 $ TeV proton-proton collisions with the ATLAS detector at the LHC
... acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, ... See full document
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Measurement of isolated-photon pair production in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
... on the Z boson mass peak [ 25 ], and the determination of the pseudorapidities is optimized using the technique described in ...benefit from the fine segmentation of ... See full document
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Measurement of the production cross section of jets in association with a Z boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector
... on the jet energy scale (JES), determined from the combination of methods based on MC and in-situ techniques used to determine the scale, constitutes the dominant component ... See full document
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Measurement of the $ZZ$ Production Cross Section in $pp$ Collisions at $\sqrt{s}$ = 13 TeV with the ATLAS Detector
... Studying the production of pairs of Z bosons in proton- proton (pp) interactions at the Large Hadron Collider (LHC) tests the electroweak sector of the standard ... See full document
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Measurement of the Soft-Drop Jet Mass in pp Collisions at $\sqrt{s} = 13$ TeV with the ATLAS Detector
... Herwig++ particle-level (left), and NLO+NLL(+NP) [ 15 ] and LO+NNLL [ 17 , 18 ] theory predictions ...(right). The LO+NNLL calculation does not have non-perturbative (NP) corrections; the region ... See full document
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Measurement of the total cross section from elastic scattering in pp collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
... inclusive-OR of the two sides was used to define an event with activity in the ...detector. The luminosity is determined with the event-counting method based on ... See full document
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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 TeV using ... See full document
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Measurement of the azimuthal anisotropy for charged particle production in $\sqrt{s_{NN}}=2.76$ TeV lead-lead collisions with the ATLAS detector
... m from the collision point, detecting neutrons and photons with |η| > ...one of the two minimum-bias trigger scintillator (MBTS) counters, covering ...side of the ... See full document
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Search for heavy Majorana neutrinos with the ATLAS detector in pp collisions at $ \sqrt{s}=8 $ TeV
... selection of events which contain a large number of fake and non-prompt ...electrons, the probabilities are measured in events with at least one jet and with exactly one ...is ... See full document
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Performance of pile-up mitigation techniques for jets in $pp$ collisions at $\sqrt{s}=8$ TeV using the ATLAS detector
... is the number of colliding bunch pairs in the LHC, f rev = ...is the revolution fre- quency [ 1 ], and σinelastic is the pp inelastic ...When the instantaneous luminosity ... See full document
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Search for heavy long-lived multi-charged particles in pp collisions at $\sqrt{s}=\;8$ TeV using the ATLAS detector
... The ATLAS detector [ 10 ] covers nearly the entire solid angle around the collision ...consists of an inner tracking detector (ID) comprising a silicon pixel ... See full document
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Measurement of the top quark mass using charged particles in pp collisions at $\sqrt s =$ 8 TeV
... colored particle that decays before forming a color-neutral state through hadronization and thus presents a unique opportunity to directly probe the properties of color ...determinations of ... See full document
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Analysis of events with $b$-jets and a pair of leptons of the same charge in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
... contributions from two categories: i) events where one or more jets are misidentified as leptons, or which contain non-prompt leptons, and ii) events that contain two leptons of opposite charge, ... See full document
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Measurement of the double-differential high-mass Drell-Yan cross section in pp collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
... . The measurements are listed to- gether with the statistical (δ stat ), systematic (δ sys ) and total (δ tot ) ...addition the contributions from the individual correlated (cor) ... See full document
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Measurement of the cross section for the production of a $W$ boson in association with $b^-$ jets in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
... A measurement is presented of the cross section for the production of a W boson with one or two b-jets in proton-proton collisions at a centre-of-mass energy ... See full document
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Search for the electroweak production of supersymmetric particles in $\sqrt{s}$=8 TeV $pp$ collisions with the ATLAS detector
... leptons from a W or Z boson, a prompt tau, or a SUSY particle decay; “fake” leptons can originate from a misidentified light-flavor quark or gluon jet (referred to as “light flavor”); “non- prompt ” ... See full document
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Search for high-mass dilepton resonances in pp collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
... consists of layers of silicon pixel and mi- crostrip detectors and a straw-tube transition-radiation tracker having coverage within |η| < ...2.0. The ID is im- mersed in a 2 T magnetic field ... See full document
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High-$E_{\rm T}$ isolated-photon plus jets production in $pp$ collisions at $\sqrt s=$ 8 TeV with the ATLAS detector
... functions of (a) E T γ , (b) p T jet1 , (c) m γ −jet1 and (d) | cos θ ∗ |. The NLO QCD predictions from J ETPHOX corrected for hadronisation and underlying-event effects and using the CT10 PDF ... See full document
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