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[PDF] Top 20 Measurement of the differential cross-sections of prompt and non-prompt production of $J/\psi $ and $\psi (2\mathrm {S})$ in $pp$ collisions at $\sqrt{s} = 7$ and 8 TeV with the ATLAS detector

Has 10000 "Measurement of the differential cross-sections of prompt and non-prompt production of $J/\psi $ and $\psi (2\mathrm {S})$ in $pp$ collisions at $\sqrt{s} = 7$ and 8 TeV with the ATLAS detector" found on our website. Below are the top 20 most common "Measurement of the differential cross-sections of prompt and non-prompt production of $J/\psi $ and $\psi (2\mathrm {S})$ in $pp$ collisions at $\sqrt{s} = 7$ and 8 TeV with the ATLAS detector".

Measurement of the differential cross-sections of prompt and non-prompt production of $J/\psi $ and $\psi (2\mathrm {S})$ in $pp$ collisions at $\sqrt{s} = 7$ and 8 TeV with the ATLAS detector

Measurement of the differential cross-sections of prompt and non-prompt production of $J/\psi $ and $\psi (2\mathrm {S})$ in $pp$ collisions at $\sqrt{s} = 7$ and 8 TeV with the ATLAS detector

... K.K. Temming 49 , D. Temple 144 , H. Ten Kate 31 , P.K. Teng 153 , J.J. Teoh 120 , F. Tepel 175 , S. Terada 68 , K. Terashi 157 , J. Terron 84 , S. Terzo 103 , M. Testa 48 , R.J. Teuscher 160 ,l , T. ... See full document

61

Measurement of differential cross sections for the production of a pair of isolated photons in pp collisions at $\sqrt{s}=7\,\text {TeV} $

Measurement of differential cross sections for the production of a pair of isolated photons in pp collisions at $\sqrt{s}=7\,\text {TeV} $

... The prompt-prompt template is built from events where the pileup energy density matches that of the event to be fitted, and where the two random cone directions are ... See full document

43

Measurement of the production cross section of prompt $J/\psi$ mesons in association with a $W^\pm$ boson in $pp$ collisions at $\sqrt{s} =$ 7 TeV with the ATLAS detector

Measurement of the production cross section of prompt $J/\psi$ mesons in association with a $W^\pm$ boson in $pp$ collisions at $\sqrt{s} =$ 7 TeV with the ATLAS detector

... C. Gay 169 , G. Gaycken 21 , E.N. Gazis 10 , P. Ge 33d ,n , Z. Gecse 169 , C.N.P. Gee 130 , D.A.A. Geerts 106 , Ch. Geich-Gimbel 21 , K. Gellerstedt 147a ,147b , C. Gemme 50a , A. Gemmell 53 , M.H. Genest 55 , S. ... See full document

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Measurement of the differential cross sections for top quark pair production as a function of kinematic event variables in pp collisions at $\sqrt s$=7 and 8 TeV

Measurement of the differential cross sections for top quark pair production as a function of kinematic event variables in pp collisions at $\sqrt s$=7 and 8 TeV

... p 2 T , where the sum is over all additional final-state partons in the matrix ...element. The effect of varying the renormalization and factorization scales ... See full document

25

Measurement of J/ψ and ψ(2S) Prompt Double-Differential Cross Sections in pp Collisions at $\sqrt{s}$=7  TeV

Measurement of J/ψ and ψ(2S) Prompt Double-Differential Cross Sections in pp Collisions at $\sqrt{s}$=7  TeV

... collected with triggers specifically designed for this purpose, including a sample enriched in dimuons from J/ψ decays where a muon is combined with an- other track and the pair ... See full document

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Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector

Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector

... immersed in a 2 T axial magnetic field provided by an encompassing thin superconducting solenoid, is located nearest to the beam pipe and comprises a high-granularity pixel detec- tor, a ... See full document

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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 ... See full document

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Measurement of $W^{\pm}$ and $Z$-boson production cross sections in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

Measurement of $W^{\pm}$ and $Z$-boson production cross sections in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

... M. LeBlanc 169 , T. LeCompte 6 , F. Ledroit-Guillon 57 , C.A. Lee 27 , S.C. Lee 152 , L. Lee 1 , G. Lefebvre 82 , M. Lefebvre 169 , F. Legger 101 , C. Leggett 16 , A. Lehan 76 , G. Lehmann Miotto 32 , X. Lei 7 , ... See full document

21

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

... level cross sections, which must be corrected for non- perturbative effects to be compared with ...ators. The corrections are derived by using PYTHIA 6.425 with the AUET2B ... See full document

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Measurement of top quark pair differential cross-sections in the dilepton channel in $pp$ collisions at $\sqrt{s}$ = 7 and 8 TeV with ATLAS

Measurement of top quark pair differential cross-sections in the dilepton channel in $pp$ collisions at $\sqrt{s}$ = 7 and 8 TeV with ATLAS

... The ATLAS detector 1 is a general-purpose, cylindrically symmetric detector with a barrel and two endcap ...components. The inner detector (ID) is closest to ... 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

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 ... See full document

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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

... pions in the ψ(2S) → J/ψ π + π − decay are reconstructed by taking all pairs of the remaining oppositely charged tracks with p T > ...GeV and |η| < 2.5 and ... See full document

58

Measurement of differential $J/\psi$ production cross sections and forward-backward ratios in p + Pb collisions with the ATLAS detector

Measurement of differential $J/\psi$ production cross sections and forward-backward ratios in p + Pb collisions with the ATLAS detector

... Measurements of differential cross-sections for Jproduction in p+Pb collisions ats N N = ...5.02 TeV at the LHC with ... See full document

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Measurement of $D^{*\pm}$, $D^\pm$ and $D_s^\pm$ meson production cross sections in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Measurement of $D^{*\pm}$, $D^\pm$ and $D_s^\pm$ meson production cross sections in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... combinations with m(Kπ π ) − m(Kπ) < 153 MeV are removed. The background from D + s → φπ + , with φ → K + K − , is suppressed by rejecting any three-track D + candidate comprised of ... 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

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, ... See full document

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Measurement of diffraction dissociation cross sections in pp collisions at $\sqrt{s}$ = 7 TeV

Measurement of diffraction dissociation cross sections in pp collisions at $\sqrt{s}$ = 7 TeV

... organized in eleven sections and two appendices. The CMS detector is described in Section ...presents the Monte Carlo (MC) simulations used in the analysis. ... See full document

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Measurement of the differential cross-section of $B^{+}$ meson production in pp collisions at $\sqrt{s}$ = 7 TeV at ATLAS

Measurement of the differential cross-section of $B^{+}$ meson production in pp collisions at $\sqrt{s}$ = 7 TeV at ATLAS

... b-hadron production cross-section has been predicted with next-to-leading-order (NLO) accuracy for more than twenty years [ 1 , 2 ] and more recently it has been predicted with ... See full document

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Measurement of the $ t\overline{t}W $ and $ t\overline{t}Z $ production cross sections in pp collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector

Measurement of the $ t\overline{t}W $ and $ t\overline{t}Z $ production cross sections in pp collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector

... S. Jakobsen 30 , T. Jakoubek 127 , J. Jakubek 128 , D.O. Jamin 114 , D.K. Jana 79 , E. Jansen 78 , R. Jansky 62 , J. Janssen 21 , M. Janus 54 , G. Jarlskog 81 , N. Javadov 65,b , T. Jav˚urek 48 , L. ... See full document

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Measurements of integrated and differential cross sections for isolated photon pair production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

Measurements of integrated and differential cross sections for isolated photon pair production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

... J. Jimenez Pena 170 , S. Jin 35a , A. Jinaru 28b , O. Jinnouchi 159 , H. Jivan 147c , P. Johansson 141 , K.A. Johns 7 , C.A. Johnson 64 , W.J. Johnson 140 , K. Jon-And 148a,148b , R.W.L. Jones ... See full document

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Observation and measurements of the production of prompt and non-prompt $J/\psi$ mesons in association with a $Z$ boson in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

Observation and measurements of the production of prompt and non-prompt $J/\psi$ mesons in association with a $Z$ boson in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

... surrounds the calorimet- ers and consists of three large air-core superconducting magnets (each with eight coils), which generate a toroidal magnetic ...field. The MS is instrumented ... See full document

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