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[PDF] Top 20 Measurement of the flavour composition of dijet events in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Has 10000 "Measurement of the flavour composition of dijet events in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector" found on our website. Below are the top 20 most common "Measurement of the flavour composition of dijet events in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector".

Measurement of the flavour composition of dijet events in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Measurement of the flavour composition of dijet events in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... R. Bartoldus 143 , A.E. Barton 71 , V. Bartsch 149 , A. Basye 165 , R.L. Bates 53 , L. Batkova 144a , J.R. Batley 28 , A. Battaglia 17 , M. Battistin 30 , F. Bauer 136 , H.S. Bawa 143 ,e , S. Beale 98 , T. Beau 78 ... See full document

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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

... fitting the observed charged asymmetry distribution of single-track hadron- ically decaying τ candidates satisfying the full W → τ ν event selection to a linear combination of tem- plates ... See full document

25

Dijet production in $\sqrt{s}=$ 7 TeV $pp$ collisions with large rapidity gaps at the ATLAS experiment

Dijet production in $\sqrt{s}=$ 7 TeV $pp$ collisions with large rapidity gaps at the ATLAS experiment

... MES of Russia and NRC KI, Russian Feder- ation; JINR; MESTD, Serbia; MSSR, Slovakia; ARRS and MIZŠ, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SERI, SNSF and Cantons ... See full document

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Measurement of dijet cross sections in $pp$ collisions at 7 TeV centre-of-mass energy using the ATLAS detector

Measurement of dijet cross sections in $pp$ collisions at 7 TeV centre-of-mass energy using the ATLAS detector

... illustrate the sensitivity of the measurements to physics beyond the SM, the model of QCD plus contact interactions (CIs) [ 69 ] with left–left coupling and destructive ... See full document

74

Measurements of jet vetoes and azimuthal decorrelations in dijet events produced in $pp$ collisions at $\sqrt{s}=7\,\mathrm{TeV}$ using the ATLAS detector

Measurements of jet vetoes and azimuthal decorrelations in dijet events produced in $pp$ collisions at $\sqrt{s}=7\,\mathrm{TeV}$ using the ATLAS detector

... C.M. Lester 121 , M. Levchenko 122 , J. Levˆeque 5 , D. Levin 88 , L.J. Levinson 173 , M. Levy 18 , A. Lewis 119 , G.H. Lewis 109 , A.M. Leyko 21 , M. Leyton 41 , B. Li 33b,t , B. Li 84 , H. Li 149 , H.L. Li 31 , L. Li ... See full document

29

Measurement of kT splitting scales in W->lv events at sqrt(s)=7 TeV with the ATLAS detector

Measurement of kT splitting scales in W->lv events at sqrt(s)=7 TeV with the ATLAS detector

... A measurement of splitting scales, as defined by the k T clustering algorithm, is presented for final states containing a W boson produced in proton–proton collisions at a ... See full document

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Measurement of the production of a $W$ boson in association with a charm quark in $pp$ collisions at $\sqrt{s} =$ 7 TeV with the ATLAS detector

Measurement of the production of a $W$ boson in association with a charm quark in $pp$ collisions at $\sqrt{s} =$ 7 TeV with the ATLAS detector

... from the fitting procedure are dominated by the modelling of the shape of the signal ...templates. The main sources are the mass resolution and the amount ... See full document

74

Measurement of the $ZZ$ Production Cross Section in $pp$ Collisions at $\sqrt{s}$ = 13 TeV with the ATLAS Detector

Measurement of the $ZZ$ Production Cross Section in $pp$ Collisions at $\sqrt{s}$ = 13 TeV with the ATLAS Detector

... inclusive with respect to additional ...tion with two leptonically decaying Z bosons and a third hadronically decaying weak boson and contributions from double parton scattering are included in ... See full document

19

Search for lepton flavour violation in the emu continuum with the ATLAS detector in $\sqrt{s}=7$ TeV $pp$ collisions at the LHC

Search for lepton flavour violation in the emu continuum with the ATLAS detector in $\sqrt{s}=7$ TeV $pp$ collisions at the LHC

... The ATLAS detector [25] is a multi-purpose particle de- tector with a forward-backward symmetric cylindrical ge- ometry and almost 4π coverage in solid angle ...[26]. The inner ... See full document

19

Measurement of the Soft-Drop Jet Mass in pp Collisions at $\sqrt{s} = 13$  TeV with the ATLAS Detector

Measurement of the Soft-Drop Jet Mass in pp Collisions at $\sqrt{s} = 13$  TeV with the ATLAS Detector

... extended the search program for physics beyond the Standard Model at the Large Hadron ...Collider. The state-of-the-art tools have been mo- tivated by theoretical ... See full document

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Measurement of the high-mass Drell--Yan differential cross-section in pp collisions at sqrt(s)=7 TeV with the ATLAS detector

Measurement of the high-mass Drell--Yan differential cross-section in pp collisions at sqrt(s)=7 TeV with the ATLAS detector

... estimate the dijet and W +jets background are considered as ...cross-checks. The first of these is similar to the baseline method but uses fake rates derived from loosely selected ... See full document

21

Search for third generation scalar leptoquarks in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector

Search for third generation scalar leptoquarks in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector

... considered in this analysis are the production of W +jets, Z/γ ∗ +jets, t ¯t, single top quarks, boson pairs, and ...multi-jets. The W - and Z-boson processes are simulated using the ... See full document

43

Measurement of the forward-backward asymmetry of electron and muon pair-production in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector

Measurement of the forward-backward asymmetry of electron and muon pair-production in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector

... is the fine-structure constant, √ ˆs is the centre-of-mass energy of the quark and anti-quark, and θ is the angle between the lepton and the quark in ... See full document

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Measurement of the $t$-channel single top-quark production cross section in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Measurement of the $t$-channel single top-quark production cross section in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... acknowledge the support of ANPCyT, Ar- gentina; YerPhI, Armenia; ARC, Australia; BMWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; ... See full document

27

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

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

... for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated ...acknowledge the support of ... See full document

31

Dynamics of isolated-photon plus jet production in pp collisions at $\sqrt(s)=7$ TeV with the ATLAS detector

Dynamics of isolated-photon plus jet production in pp collisions at $\sqrt(s)=7$ TeV with the ATLAS detector

... acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWF and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, ... See full document

53

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

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

... calculations at the parton level are corrected to the particle level for the underlying event and for effects of fragmentation and of QED final-state radiation ...from the ... See full document

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Measurement of event-shape observables in $Z \rightarrow \ell ^{+} \ell ^{-}$ events in $pp$ collisions at $\sqrt{s}=$ 7 TeV with the ATLAS detector at the LHC

Measurement of event-shape observables in $Z \rightarrow \ell ^{+} \ell ^{-}$ events in $pp$ collisions at $\sqrt{s}=$ 7 TeV with the ATLAS detector at the LHC

... E. Gornicki 40 , A.T. Goshaw 46 , C. Gössling 44 , M.I. Gostkin 66 , C.R. Goudet 117 , D. Goujdami 135c , A.G. Goussiou 138 , N. Govender 145b , E. Gozani 152 , L. Graber 55 , I. Grabowska-Bold 39a , P.O.J. Gradin 164 , ... See full document

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Search for magnetic monopoles in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector

Search for magnetic monopoles in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector

... 2) The simulation un- derestimates the TRT occupancy in the data by up to 20%; therefore, the number of low-threshold hits (those unlikely to come from the monopole or ... See full document

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Measurement of the production cross section for Z/gamma* in association with jets in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Measurement of the production cross section for Z/gamma* in association with jets in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, ... See full document

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