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[PDF] Top 20 Searches for the Z gamma decay mode of the Higgs boson and for new high-mass resonances in pp collisions at root s=13 TeV with the ATLAS detector

Has 10000 "Searches for the Z gamma decay mode of the Higgs boson and for new high-mass resonances in pp collisions at root s=13 TeV with the ATLAS detector" found on our website. Below are the top 20 most common "Searches for the Z gamma decay mode of the Higgs boson and for new high-mass resonances in pp collisions at root s=13 TeV with the ATLAS detector".

Searches for the Zγ decay mode of the Higgs boson and for new high mass resonances in pp collisions at s=13 TeV with the ATLAS detector

Searches for the Zγ decay mode of the Higgs boson and for new high mass resonances in pp collisions at s=13 TeV with the ATLAS detector

... GeV Higgs boson. Many models of physics beyond the SM introduce new heavy bosons (X) through ex- tensions of the Higgs sector or as additional gauge ...fields. Searches for heavy Zγ ... See full document

51

Search for dark matter in association with a Higgs boson decaying to b-quarks in pp collisions at root s=13 TeV with the ATLAS detector

Search for dark matter in association with a Higgs boson decaying to b-quarks in pp collisions at root s=13 TeV with the ATLAS detector

... of searches at the Large Hadron Collider (LHC) [4] have been performed recently, where X is considered to be a hadronic jet [5, 6], b− or t− quarks [7–9], a photon [10–13], or a W /Z boson ... See full document

36

Measurements of the production cross section of a Z boson in association with jets in pp collisions at root s=13 TeV with the ATLAS detector

Measurements of the production cross section of a Z boson in association with jets in pp collisions at root s=13 TeV with the ATLAS detector

... a Z boson 1 in association with jets, Z + jets, constitutes a powerful test of perturbative quantum chromodynamics (QCD) [1, ...the Z boson to charged leptonic final states offer clean ... See full document

47

Measurement of the Higgs boson mass in the H → ZZ∗→4ℓ and H →γγ channels with √s = 13 TeV pp collisions using the ATLAS detector

Measurement of the Higgs boson mass in the H → ZZ∗→4ℓ and H →γγ channels with √s = 13 TeV pp collisions using the ATLAS detector

... to detector effects for some specific category of photons are performed by par- titioning the entire data sample into detector-oriented categories, different from those used for the nominal result, and ... See full document

23

Searches for invisible decays of the Higgs boson in pp collisions at √s = 7, 8, and 13 TeV

Searches for invisible decays of the Higgs boson in pp collisions at √s = 7, 8, and 13 TeV

... and 13 TeV data ...the 13 TeV analysis compared to the 8 TeV ...leptonic Z boson decays in the case where the lepton pair is produced at high Lorentz boost causing ... See full document

56

Search for the Higgs boson in the H >WW >lνjj decay channel in pp collisions at √s=7 TeV with the ATLAS detector

Search for the Higgs boson in the H >WW >lνjj decay channel in pp collisions at √s=7 TeV with the ATLAS detector

... and Z bosons [4–6], and manifests itself directly as the so-called Higgs ...for Higgs boson production in high energy proton-proton ...the Higgs boson is predominantly ... See full document

19

Searches for lepton-flavour-violating decays of the Higgs boson in \sqrt{s} = 13 TeV pp collisions with the ATLAS detector

Searches for lepton-flavour-violating decays of the Higgs boson in \sqrt{s} = 13 TeV pp collisions with the ATLAS detector

... P. Massarotti 69a , 69b , P. Mastrandrea 71a , 71b , A. Mastroberardino 41b , 41a , T. Masubuchi 163 , D. Matakias 10 , A. Matic 114 , P. Mättig 24 , J. Maurer 27b , B. Maˇcek 91 , S.J. Maxfield 90 , D.A. Maximov 122b , ... See full document

23

Search for heavy resonances decaying to a W or Z boson and a Higgs boson in the qq¯⁽´⁾bb¯ final state in pp collisions at √s=13 TeV with the ATLAS detector

Search for heavy resonances decaying to a W or Z boson and a Higgs boson in the qq¯⁽´⁾bb¯ final state in pp collisions at √s=13 TeV with the ATLAS detector

... The ATLAS detector is described in detail elsewhere ...the ATLAS detector are an inner detector (ID) surrounded by a thin superconducting solenoid providing a 2 T axial magnetic field, ... See full document

43

Search for high mass dilepton resonances in pp collisions at root s = 8 TeV with the ATLAS detector

Search for high mass dilepton resonances in pp collisions at root s = 8 TeV with the ATLAS detector

... the decay of a new resonance are determined at 95% ...of mass is different for each model considered due to different angular distributions, boosts, and line ... See full document

31

Search for Higgs boson decays to a photon and a Z boson in pp collisions at s=7 and 8 TeV with the ATLAS detector

Search for Higgs boson decays to a photon and a Z boson in pp collisions at s=7 and 8 TeV with the ATLAS detector

... the Z boson candidate decays to muons and to 10% for events in which the Z boson candidate decays to ...any Higgs boson mass in the range 120–150 GeV is taken as an ... See full document

21

Search for heavy lepton resonances decaying to a Z boson and a lepton in pp collisions at s=8 TeV with the ATLAS detector

Search for heavy lepton resonances decaying to a Z boson and a lepton in pp collisions at s=8 TeV with the ATLAS detector

... trilepton resonances are motivated by several extensions of the Standard Model ...the mass hierarchy between the different lepton generations ...composite Higgs models [11, 12] and models of warped ... See full document

38

Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 fb(-1) of root s=13 TeV pp collisions with the ATLAS detector

Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 fb(-1) of root s=13 TeV pp collisions with the ATLAS detector

... L.K. Gladilin 101 , C. Glasman 85 , J. Glatzer 13 , P.C.F. Glaysher 45 , A. Glazov 45 , M. Goblirsch-Kolb 25 , J. Godlewski 42 , S. Goldfarb 91 , T. Golling 52 , D. Golubkov 132 , A. Gomes 128a,128b,128d , ... See full document

52

Search for the Dimuon Decay of the Higgs Boson in pp Collisions at root s=13 TeV with the ATLAS Detector

Search for the Dimuon Decay of the Higgs Boson in pp Collisions at root s=13 TeV with the ATLAS Detector

... two high-p T forward jets in opposite detector hemispheres and little hadronic activity between ...the Z= γ → μμ (Drell-Yan) ...invariant mass m μμ in all the categories is performed in the ... See full document

20

Search for Higgs boson decays to a photon and a Z boson in pp collisions at sqrt(s)=7 and 8 TeV with the ATLAS detector

Search for Higgs boson decays to a photon and a Z boson in pp collisions at sqrt(s)=7 and 8 TeV with the ATLAS detector

... the Z boson candidate decays to muons and to 10% for events in which the Z boson candidate decays to ...any Higgs boson mass in the range 120–150 GeV is taken as an ... See full document

20

Searches for heavy diboson resonances in pp collisions at √s=13 TeV with the ATLAS detector

Searches for heavy diboson resonances in pp collisions at √s=13 TeV with the ATLAS detector

... (W Z, W W ) search and in figure 3 for those relevant to the scalar resonance and bulk RS G ∗ → W W, ZZ searches, ...W Z channel are also shown in table ...a mass of 1.6 TeV, with a ... See full document

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Combination of searches for Higgs boson pairs in pp collisions at \sqrt{s} = 13 TeV with the ATLAS detector

Combination of searches for Higgs boson pairs in pp collisions at \sqrt{s} = 13 TeV with the ATLAS detector

... ( pp → H H ) = 33 . 5 + − 2 2 . . 8 4 fb at √ s = 13 TeV [11], calculated first at next-to-leading order (NLO) in QCD with the heavy top-quark approximation [12], then numerically with full ... See full document

23

Search for heavy resonances decaying to a Z boson and a photon in pp collisions at root s=13 TeV with the ATLAS detector

Search for heavy resonances decaying to a Z boson and a photon in pp collisions at root s=13 TeV with the ATLAS detector

... centre-of-mass pp collision energy of 13 ...the ATLAS detector response [16] based on G eant 4 ...proton–proton collisions (referred to as pile-up) are simulated with the soft ... See full document

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Search for dark matter produced in association with a Higgs boson decaying to two bottom quarks in pp collisions at root s=8 TeV with the ATLAS detector

Search for dark matter produced in association with a Higgs boson decaying to two bottom quarks in pp collisions at root s=8 TeV with the ATLAS detector

... the Z ð→ ν¯ νÞ þ jets estimation is derived from the control regions with no b-tagged jets for both the resolved and boosted ...the Z ð→ ν¯ νÞ þ jets normaliza- tion in both ... See full document

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Measurement of W± and Z-boson production cross sections in pp   collisions at  √s = 13 TeV with the ATLAS detector

Measurement of W± and Z-boson production cross sections in pp collisions at √s = 13 TeV with the ATLAS detector

... the detector and the resulting photons subsequently convert and are reconstructed as high p T ...of Z → ee events in which both electrons are reconstructed with the same charge and is found to be ... See full document

21

Beyond-the-Standard Model Higgs Physics using the ATLAS Experiment

Beyond-the-Standard Model Higgs Physics using the ATLAS Experiment

... additional Higgs bosons or exotic decay of the SM Higgs boson can give us direct evidences about physics beyond the Standard Model ...two Higgs doublet models (2HDMs) [6–9], ... See full document

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