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[PDF] Top 20 Search for ZZ resonances in the 2$\ell$2$\nu$ final state in proton-proton collisions at 13 TeV

Has 10000 "Search for ZZ resonances in the 2$\ell$2$\nu$ final state in proton-proton collisions at 13 TeV" found on our website. Below are the top 20 most common "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

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

36

Search for pair-produced resonances decaying to quark pairs in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for pair-produced resonances decaying to quark pairs in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... general search for the pair production of resonances, each decaying to two quarks, is ...reported. The search is conducted separately for heavier resonances (masses above 400 ... See full document

25

Searches for heavy $ZZ$ and $ZW$ resonances in the $\ell\ell qq$ and $\nu\nu qq$ final states in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

Searches for heavy $ZZ$ and $ZW$ resonances in the $\ell\ell qq$ and $\nu\nu qq$ final states in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

... P.O.J. Gradin 168 , J. Gramling 166 , E. Gramstad 121 , S. Grancagnolo 17 , V. Gratchev 125 , P.M. Gravila 28f , C. Gray 56 , H.M. Gray 16 , Z.D. Greenwood 82,u , C. Grefe 23 , K. Gregersen 81 , I.M. Gregor 45 , P. ... See full document

52

Search for additional neutral MSSM Higgs bosons in the $\tau\tau$ final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for additional neutral MSSM Higgs bosons in the $\tau\tau$ final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... for the production of a single narrow resonance, φ, with a mass between 90 GeV and ...3.2 TeV in the ττ final state (left) for the pro- duction via gluon fusion (ggφ) and ... See full document

56

Search For Heavy Resonances Decaying To Tau Lepton Pairs In Proton-proton Collisions At Root S=13 Tev

Search For Heavy Resonances Decaying To Tau Lepton Pairs In Proton-proton Collisions At Root S=13 Tev

... from the standard model. Upper limits at 95% confidence level are derived for the product of the cross section and branching fraction for a Z 0 boson decaying to a tau lepton pair, as a ... See full document

36

Search for Z$\gamma$ resonances using leptonic and hadronic final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for Z$\gamma$ resonances using leptonic and hadronic final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... to the background-only hypotheses are represented by the red lines, with their 68% CL uncertainty bands given by the gray ...of the background prediction with the dashed lines. ... See full document

40

Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... from the standard model. Upper limits at 95% confidence level are derived for the product of the cross section and branching fraction for a Z 0 boson decaying to a tau lepton pair, as a ... See full document

32

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

... events in which both bosons decay leptonically and one of the three leptons is not reconstructed in the detector, and ZZ → ` − ` + ` 0 − ` 0 + events in which two of the ... See full document

54

Search for heavy resonances decaying to a top quark and a bottom quark in the lepton+jets final state in proton–proton collisions at 13 TeV

Search for heavy resonances decaying to a top quark and a bottom quark in the lepton+jets final state in proton–proton collisions at 13 TeV

... lepton in each event is required to have fired a single- lepton trigger that has no isolation requirement, be within the detector acceptance ( | η | < 2 ...excluding the barrel endcap ... See full document

25

Search for pair-produced resonances each decaying into at least four quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for pair-produced resonances each decaying into at least four quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... this search comes from natural SUSY, but the analysis aims more broadly for new phenomena in ...about the helicity, the intermediate decay topology, or the presence of secondary ... See full document

18

Search for $\mathrm{t}\overline{\mathrm{t}}$H production in the all-jet final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for $\mathrm{t}\overline{\mathrm{t}}$H production in the all-jet final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... to 13%, depending on the process. The PDF uncertainties [70] range between 2 and 4%, and are treated as fully correlated for all processes that share the same dominant ini- tial ... See full document

44

Search for new resonances decaying via WZ to leptons in proton-proton collisions at $\sqrt s =$ 8 TeV

Search for new resonances decaying via WZ to leptons in proton-proton collisions at $\sqrt s =$ 8 TeV

... misidentified. The primary background is the irreducible SM WZ ...boson in the final state, such as top quark pair (t¯t), multijet, W+jet, Wγ+jet, and WW+jet production, are also ... See full document

33

Search for dijet resonances in proton–proton collisions at $\sqrt{s}$ = 13 TeV and constraints on dark matter and other models

Search for dijet resonances in proton–proton collisions at $\sqrt{s}$ = 13 TeV and constraints on dark matter and other models

... Fig. 2 are calculated in the narrow-width approximation [14] using the CTEQ6L1 [49] PDF at leading order, with a next-to-leading or- der correction factor of approximately ...for ... See full document

23

Search for high-mass new phenomena in the dilepton final state using proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

Search for high-mass new phenomena in the dilepton final state using proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

... GeV. The prior probability is chosen to be uniform and positive in the cross-section for the Z ′ limit calculation and 1/Λ 2 or 1/Λ 4 for the CI limit ...For the CI limit ... See full document

35

Search for low-mass resonances decaying into bottom quark-antiquark pairs in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Search for low-mass resonances decaying into bottom quark-antiquark pairs in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... A search for narrow, low-mass, scalar, and pseudoscalar resonances decaying to bottom quark-antiquark pairs is ...presented. The search is based on events recorded in p ffiffiffi s ¼ ... See full document

25

Search for resonant $WZ$ production in the fully leptonic final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

Search for resonant $WZ$ production in the fully leptonic final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

... For the HVT interpretation, W  → W Z samples were gener- ...provided in Ref. [ 15 ], are used. In Model A, weakly coupled vector resonances arise from an exten- sion of the SM gauge ... See full document

21

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

... from the Marie-Curie programme and the European Re- search Council and Horizon 2020 Grant, contract ...Union); the Leventis Foundation; the A. P. Sloan Foundation; the Alexander ... See full document

42

Search for high-mass resonances in dilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for high-mass resonances in dilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... Neutral resonances decaying to lepton pairs occur in a variety of theoretical models that at- tempt to extend the standard model (SM) of particle ...of the three forces at a high ... See full document

42

Search for heavy ZZ resonances in the $\ell ^+\ell ^-\ell ^+\ell ^-$ and $\ell ^+\ell ^-\nu \bar{\nu }$ final states using proton–proton collisions at $\sqrt{s}= 13$   $\text {TeV}$ with the ATLAS detector

Search for heavy ZZ resonances in the $\ell ^+\ell ^-\ell ^+\ell ^-$ and $\ell ^+\ell ^-\nu \bar{\nu }$ final states using proton–proton collisions at $\sqrt{s}= 13$   $\text {TeV}$ with the ATLAS detector

... reconstructed in the ID and MS, and their identification is primarily based on the presence of the track or track segment in the MS [ 63 ...present in both the ID ... See full document

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Search for high-mass diphoton resonances in proton–proton collisions at 13 TeV and combination with 8 TeV search

Search for high-mass diphoton resonances in proton–proton collisions at 13 TeV and combination with 8 TeV search

... successful in describing physical phenomena but it is widely con- sidered to be an incomplete theory because of various shortcom- ...ings. In particular, the SM suffers from the so-called ... See full document

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