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[PDF] Top 20 $ZZ \to \ell^{+}\ell^{-}\ell^{\prime +}\ell^{\prime -}$ cross-section measurements and search for anomalous triple gauge couplings in 13 TeV $pp$ collisions with the ATLAS detector

Has 10000 "$ZZ \to \ell^{+}\ell^{-}\ell^{\prime +}\ell^{\prime -}$ cross-section measurements and search for anomalous triple gauge couplings in 13 TeV $pp$ collisions with the ATLAS detector" found on our website. Below are the top 20 most common "$ZZ \to \ell^{+}\ell^{-}\ell^{\prime +}\ell^{\prime -}$ cross-section measurements and search for anomalous triple gauge couplings in 13 TeV $pp$ collisions with the ATLAS detector".

$ZZ \to \ell^{+}\ell^{-}\ell^{\prime +}\ell^{\prime -}$ cross-section measurements and search for anomalous triple gauge couplings in 13 TeV $pp$ collisions with the ATLAS detector

$ZZ \to \ell^{+}\ell^{-}\ell^{\prime +}\ell^{\prime -}$ cross-section measurements and search for anomalous triple gauge couplings in 13 TeV $pp$ collisions with the ATLAS detector

... The ATLAS detector [22,23] is a multipurpose particle detector with a cylindrical ...calorimeters, and muon chambers. The inner detector (ID) is immersed in ... See full document

39

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 the standard model (SM) at ... See full document

19

Measurement of inclusive and differential cross sections in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

Measurement of inclusive and differential cross sections in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

... measured cross section and a theoretical prediction is evaluated by computing a p-value based on the difference between the value of −2 ln Λ at the best-fit value and ... See full document

49

Measurement of $WW/WZ \to \ell \nu q q^{\prime}$ production with the hadronically decaying boson reconstructed as one or two jets in $pp$ collisions at $\sqrt{s}=8$ TeV with ATLAS, and constraints on anomalous gauge couplings

Measurement of $WW/WZ \to \ell \nu q q^{\prime}$ production with the hadronically decaying boson reconstructed as one or two jets in $pp$ collisions at $\sqrt{s}=8$ TeV with ATLAS, and constraints on anomalous gauge couplings

... T. Klapdor-Kleingrothaus 51 , M.H. Klein 92 , M. Klein 77 , U. Klein 77 , K. Kleinknecht 86 , P. Klimek 110 , A. Klimentov 27 , R. Klingenberg 46 , T. Klingl 23 , T. Klioutchnikova 32 , E.-E. Kluge 60a , P. Kluit 109 , ... See full document

48

Measurements of the $\mathrm {p}\mathrm {p}\rightarrow \mathrm{Z}\mathrm{Z}$ production cross section and the $\mathrm{Z}\rightarrow 4\ell $ branching fraction, and constraints on anomalous triple gauge couplings at $\sqrt{s} = 13\,\text {TeV} $

Measurements of the $\mathrm {p}\mathrm {p}\rightarrow \mathrm{Z}\mathrm{Z}$ production cross section and the $\mathrm{Z}\rightarrow 4\ell $ branching fraction, and constraints on anomalous triple gauge couplings at $\sqrt{s} = 13\,\text {TeV} $

... set to their SM values. The systematic uncertainties described in Section 7 are treated as nuisance parameters with log-normal ...deriving the limits so that the results ... See full document

42

Measurement of the Zγ Production Cross Section in pp Collisions at 8 TeV and Search for Anomalous Triple Gauge Boson Couplings

Measurement of the Zγ Production Cross Section in pp Collisions at 8 TeV and Search for Anomalous Triple Gauge Boson Couplings

... 3.0 in two endcap regions (EE). A preshower detector consisting of two planes of silicon sensors interleaved with a total of three radiation lengths of lead is located in front of the ... See full document

39

Measurement of the Higgs boson coupling properties in the $H\rightarrow ZZ^{*} \rightarrow 4\ell$ decay channel at $\sqrt{s}$ = 13 TeV with the ATLAS detector

Measurement of the Higgs boson coupling properties in the $H\rightarrow ZZ^{*} \rightarrow 4\ell$ decay channel at $\sqrt{s}$ = 13 TeV with the ATLAS detector

... NLO to LO cross-section ratio, as well as several kinematic quantities that affect the categorization of reconstructed events, such as the jet transverse momenta, receive higher-order ... See full document

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Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector

Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector

... events with a W boson produced in association with jets ...include the production of top quarks, multijets, dibo- sons and Z ...bosons with associated jets were simulated using ... See full document

44

Measurement of the $W W$ cross section in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector and limits on anomalous gauge couplings

Measurement of the $W W$ cross section in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector and limits on anomalous gauge couplings

... used to check the W + jet prediction and give consistent ...results. The first method applies the measured f e and f µ ratios to an in- clusive W + jets data ... See full document

26

Measurement of the $ZZ$ production cross section in proton-proton collisions at $\sqrt s =$ 8 TeV using the $ZZ\to\ell^{-}\ell^{+}\ell^{\prime -}\ell^{\prime +}$ and $ZZ\to\ell^{-}\ell^{+}\nu\bar{\nu}$ channels with the ATLAS detector

Measurement of the $ZZ$ production cross section in proton-proton collisions at $\sqrt s =$ 8 TeV using the $ZZ\to\ell^{-}\ell^{+}\ell^{\prime -}\ell^{\prime +}$ and $ZZ\to\ell^{-}\ell^{+}\nu\bar{\nu}$ channels with the ATLAS detector

... M. Svatos 128 , M. Swiatlowski 33 , I. Sykora 147a , T. Sykora 130 , D. Ta 50 , C. Taccini 135a,135b , K. Tackmann 44 , J. Taenzer 162 , A. Taffard 167 , R. Tafirout 164a , N. Taiblum 156 , H. Takai 27 , R. Takashima 71 ... See full document

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Search for photonic signatures of gauge-mediated supersymmetry in 13 TeV $pp$ collisions with the ATLAS detector

Search for photonic signatures of gauge-mediated supersymmetry in 13 TeV $pp$ collisions with the ATLAS detector

... A search is presented for photonic signatures, motivated by generalized models of gauge-mediated supersymmetry ...This search makes use of proton-proton collision data at p ffiffiffi s ¼ 13 ... See full document

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

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

... In the µνee, eνµµ and µνµµ channels, the top-quark background contribution is evaluated from the average den- sity of events in the side-bands around the Z mass ... See full document

18

Search for resonant $WZ$ production in the $WZ \to \ell \nu \ell^\prime\ell^\prime$ channel in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector

Search for resonant $WZ$ production in the $WZ \to \ell \nu \ell^\prime\ell^\prime$ channel in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector

... removing the a T contribution at the generator level. The SM W Z production, which is an irreducible back- ground for this search, is modeled by the mc@nlo event generator [22], which ... See full document

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Measurement of the $pp \to ZZ$ production cross section and constraints on anomalous triple gauge couplings in four-lepton final states at $\sqrt s=$8 TeV

Measurement of the $pp \to ZZ$ production cross section and constraints on anomalous triple gauge couplings in four-lepton final states at $\sqrt s=$8 TeV

... production in proton-proton collisions provides an important test of the electroweak sector of the standard model (SM), especially the non-Abelian structure of the SM ... See full document

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Search for ZZ resonances in the 2$\ell$2$\nu$ final state in proton-proton collisions at 13 TeV

Search for ZZ resonances in the 2$\ell$2$\nu$ final state in proton-proton collisions at 13 TeV

... colleagues in the CERN accelerator departments for the excellent perfor- mance of the LHC and thank the technical and administrative staffs at CERN and at other CMS ... See full document

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Search for the standard model Higgs boson in the $H$ to $Z Z$ to $\ell \ell \tau \tau$ decay channel in $pp$ collisions at $\sqrt{s}=7$ TeV

Search for the standard model Higgs boson in the $H$ to $Z Z$ to $\ell \ell \tau \tau$ decay channel in $pp$ collisions at $\sqrt{s}=7$ TeV

... The search for the standard model (SM) [1–3] Higgs boson is one of the main goals of the Large Hadron Collider (LHC) physics ...programme. The discovery of the SM Higgs ... See full document

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Search for a Higgs boson in the decay channel $H$ to ZZ(*) to $q$ qbar $\ell^-$ l+ in $pp$ collisions at $\sqrt{s}=7$ TeV

Search for a Higgs boson in the decay channel $H$ to ZZ(*) to $q$ qbar $\ell^-$ l+ in $pp$ collisions at $\sqrt{s}=7$ TeV

... wish to congratulate our colleagues in the CERN accelerator departments for the excel- lent performance of the LHC ...thank the technical and administrative staff at CERN ... See full document

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Search for a standard sodel Higgs boson in the H $\to$ ZZ $\to \ell^{+}\ell^{-}\nu \bar{\nu}$ decay channel using 4.7 fb$^{-1}$ of $\sqrt{s} =$ 7 TeV data with the ATLAS detector

Search for a standard sodel Higgs boson in the H $\to$ ZZ $\to \ell^{+}\ell^{-}\nu \bar{\nu}$ decay channel using 4.7 fb$^{-1}$ of $\sqrt{s} =$ 7 TeV data with the ATLAS detector

... production cross sections and de- cay branching ratios, as well as their uncertainties, are taken from ...25]. The cross sections for the gluon fusion process have been calculated ... See full document

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Search for resonant and nonresonant Higgs boson pair production in the $ \mathrm{b}\overline{\mathrm{b}}\mathit{\ell \nu \ell \nu } $ final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for resonant and nonresonant Higgs boson pair production in the $ \mathrm{b}\overline{\mathrm{b}}\mathit{\ell \nu \ell \nu } $ final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... [74] in order to ensure optimal sensitivity on the full range of signal hypotheses considered in these ...searches. In this approach, one or more physics parameters describing ... See full document

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Search for anomalous couplings in boosted $\mathrm{ WW/WZ }\to\ell\nu\mathrm{ q \bar{q} }$ production in proton-proton collisions at $\sqrt{s} =$ 8 TeV

Search for anomalous couplings in boosted $\mathrm{ WW/WZ }\to\ell\nu\mathrm{ q \bar{q} }$ production in proton-proton collisions at $\sqrt{s} =$ 8 TeV

... processes. The τ lepton decays are simulated with tauola [17] . The pythia ...provides the fragmentation and parton shower simulation, with the parameters of the ... See full document

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