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[PDF] Top 20 Measurement of exclusive $\gamma\gamma\rightarrow W^+W^-$ production and search for exclusive Higgs boson production in $pp$ collisions at $\sqrt{s} = 8$ TeV using the ATLAS detector

Has 10000 "Measurement of exclusive $\gamma\gamma\rightarrow W^+W^-$ production and search for exclusive Higgs boson production in $pp$ collisions at $\sqrt{s} = 8$ TeV using the ATLAS detector" found on our website. Below are the top 20 most common "Measurement of exclusive $\gamma\gamma\rightarrow W^+W^-$ production and search for exclusive Higgs boson production in $pp$ collisions at $\sqrt{s} = 8$ TeV using the ATLAS detector".

Measurement of exclusive $\gamma\gamma\rightarrow W^+W^-$ production and search for exclusive Higgs boson production in $pp$ collisions at $\sqrt{s} = 8$ TeV using the ATLAS detector

Measurement of exclusive $\gamma\gamma\rightarrow W^+W^-$ production and search for exclusive Higgs boson production in $pp$ collisions at $\sqrt{s} = 8$ TeV using the ATLAS detector

... DNRF and DNSRC, Denmark; IN2P3-CNRS, CEA-DSM /IRFU, France; GNSF, Geor- gia; BMBF, HGF, and MPG, Germany; GSRT, Greece; RGC, Hong Kong SAR, China; ISF, I-CORE and Benoziyo Center, Israel; INFN, ... See full document

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Search for Higgs boson pair production in the $\gamma\gamma\mathrm{b\overline{b}}$ final state in pp collisions at $\sqrt{s}=$ 13 TeV

Search for Higgs boson pair production in the $\gamma\gamma\mathrm{b\overline{b}}$ final state in pp collisions at $\sqrt{s}=$ 13 TeV

... personnel of the Worldwide LHC Computing Grid for delivering so effectively the computing infrastructure essential to our ...acknowledge the enduring support for the construc- tion ... See full document

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Simultaneous measurements of the $t\bar{t}$, $W^+W^-$, and $Z/\gamma^{*}\rightarrow\tau\tau$ production cross-sections in $pp$ collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector

Simultaneous measurements of the $t\bar{t}$, $W^+W^-$, and $Z/\gamma^{*}\rightarrow\tau\tau$ production cross-sections in $pp$ collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector

... MPG and AvH Foundation, Germany; GSRT and NSRF, Greece; ISF, MINERVA, GIF, I-CORE and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, ... See full document

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Measurement of $W \gamma$ and $Z \gamma$ production cross sections in $pp$ collisions at $\sqrt{s}=7$ TeV and limits on anomalous triple gauge couplings with the ATLAS detector

Measurement of $W \gamma$ and $Z \gamma$ production cross sections in $pp$ collisions at $\sqrt{s}=7$ TeV and limits on anomalous triple gauge couplings with the ATLAS detector

... uncertainties. The limits on a given aTGC parameter ...from the Bayesian posterior, given the extended fiducial ...measurements. The Bayesian posterior probabil- ity density function is ... See full document

24

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

Measurement of the $W^{\pm}Z$ boson pair-production cross section in $pp$ collisions at $\sqrt{s}=13$ 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 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

... A.R. Weidberg 119 , P. Weigell 100 , B. Weinert 60 , J. Weingarten 54 , C. Weiser 48 , H. Weits 106 , P.S. Wells 30 , T. Wenaus 25 , D. Wendland 16 , Z. Weng 152,r , T. Wengler 30 , S. Wenig 30 , N. Wermes 21 , M. ... See full document

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Search for exclusive or semi-exclusive photon pair production and observation of exclusive and semi-exclusive electron pair production in $pp$ collisions at $\sqrt{s}=7$ TeV

Search for exclusive or semi-exclusive photon pair production and observation of exclusive and semi-exclusive electron pair production in $pp$ collisions at $\sqrt{s}=7$ TeV

... At the Large Hadron Collider (LHC), exclusive γγ (hereafter referred to as “diphoton”) events can be produced by means of IPIP exchange, interpreted in partonic terms as gg → γγ via a ... See full document

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Evidence for Electroweak Production of $W^{\pm}W^{\pm}jj$ in $pp$ Collisions at $\sqrt{s}=8$ TeV with the ATLAS Detector

Evidence for Electroweak Production of $W^{\pm}W^{\pm}jj$ in $pp$ Collisions at $\sqrt{s}=8$ TeV with the ATLAS Detector

... ZZ+jets and t¯ t + W/Z are also ...estimated using MC simulation. In the VBS region strong W ± W ± jj is estimated using simula- tion and normalized to ... 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. Medinnis 44 , S. Meehan 139 , S. Mehlhase 101 , A. Mehta 76 , K. Meier 60a , C. Meineck 101 , B. Meirose 43 , D. Melini 167 , B.R. Mellado Garcia 146c , M. Melo 145a , F. Meloni 18 , A. Mengarelli 22a , ... See full document

21

Measurement of inclusive W and Z boson production cross sections in pp collisions at $\sqrt{s}$ = 8 TeV

Measurement of inclusive W and Z boson production cross sections in pp collisions at $\sqrt{s}$ = 8 TeV

... levels of instantaneous luminosity reached by the LHC in 2012 present challenges for the precise measurement of the W boson cross section because of ... See full document

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Search for a multi-Higgs-boson cascade in $W^+W^−b\bar{b}$ events with the ATLAS detector in pp collisions at $\sqrt{s} = 8$  TeV

Search for a multi-Higgs-boson cascade in $W^+W^−b\bar{b}$ events with the ATLAS detector in pp collisions at $\sqrt{s} = 8$  TeV

... ), and a light Higgs boson (h 0 ). The analysis searches for events involving the production of a single heavy neutral Higgs boson which decays to the ... See full document

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Measurement of $W^+W^-$ production in pp collisions at $\sqrt{s}$=7  TeV with the ATLAS detector and limits on anomalous WWZ and WWγ couplings

Measurement of $W^+W^-$ production in pp collisions at $\sqrt{s}$=7  TeV with the ATLAS detector and limits on anomalous WWZ and WWγ couplings

... renormalization and factor- ization scales up and down by a factor of 2 for both the inclusive (≥ 0) and exclusive (≥ 1) jet cross sections and adding these two ... See full document

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Search for pair production of a new heavy quark that decays into a $W$ boson and a light quark in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector

Search for pair production of a new heavy quark that decays into a $W$ boson and a light quark in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector

... S. Strandberg 146a,146b , A. Strandlie 119 , E. Strauss 143 , M. Strauss 113 , P. Strizenec 144b , R. Ströhmer 174 , D.M. Strom 116 , R. Stroynowski 40 , A. Strubig 106 , S.A. Stucci 17 , B. Stugu 14 , N.A. Styles ... See full document

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Measurement of the cross-section for W boson production in association with b-jets in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector

Measurement of the cross-section for W boson production in association with b-jets in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector

... compare the NLO calculations with data, the impact of non-perturbative effects and double-parton interactions has to be ...considered. The MCFM predictions are only available at ... See full document

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Search for $W' \rightarrow tb$ decays in the hadronic final state using pp collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

Search for $W' \rightarrow tb$ decays in the hadronic final state using pp collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

... identify the jets compatible with orig- inating from a b-quark created either directly from the W  boson or from the top-quark ...GeV and | η | < 2 . 5 (in order to be ... See full document

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Measurement of differential cross sections and $W^+/W^-$ cross-section ratios for $W$ boson production in association with jets at $\sqrt{s}=8$ TeV with the ATLAS detector

Measurement of differential cross sections and $W^+/W^-$ cross-section ratios for $W$ boson production in association with jets at $\sqrt{s}=8$ TeV with the ATLAS detector

... tion and the underlying ...emissions at LO in pQCD. The calculation uses the NNPDF ...set and dynamic renormalisation and factorisation scales determined by ... See full document

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Search for top quark decays $t\rightarrow qH$, with $H\to\gamma\gamma$, in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector

Search for top quark decays $t\rightarrow qH$, with $H\to\gamma\gamma$, in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector

... The ATLAS detector [ 36 ] consists of an inner detector for tracking surrounded by a superconducting solenoid providing a 2 T magnetic field, electromagnetic and hadronic ... See full document

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Search for a charged Higgs boson in pp collisions at $ \sqrt{s}=8 $ TeV

Search for a charged Higgs boson in pp collisions at $ \sqrt{s}=8 $ TeV

... events in which both W bosons decay leptonically, and surpasses by more than one order of magnitude the sum of the remaining ...simulation. The dilepton trigger ... See full document

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Search for a Higgs boson decaying into $\gamma^* \gamma \to \ell \ell \gamma$ with low dilepton mass in pp collisions at $\sqrt s = $ 8 TeV

Search for a Higgs boson decaying into $\gamma^* \gamma \to \ell \ell \gamma$ with low dilepton mass in pp collisions at $\sqrt s = $ 8 TeV

... sum of signals in the ECAL crystals [16]. The ECAL signals are calibrated and corrected [17], and a multivariate regression technique, developed for the H → γγ analysis ... See full document

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Search for invisible decays of a Higgs boson using vector-boson fusion in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

Search for invisible decays of a Higgs boson using vector-boson fusion in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

... direction of the jet that was misidentified as a lepton. As a result, the multijet background tends to have significantly lower m T than the W+jets ...modelling the jets ... See full document

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