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[PDF] Top 20 Search for heavy resonances that decay into a vector boson and a Higgs boson in hadronic final states at $\sqrt{s} = 13$ $\,\text {TeV}$

Has 10000 "Search for heavy resonances that decay into a vector boson and a Higgs boson in hadronic final states at $\sqrt{s} = 13$ $\,\text {TeV}$" found on our website. Below are the top 20 most common "Search for heavy resonances that decay into a vector boson and a Higgs boson in hadronic final states at $\sqrt{s} = 13$ $\,\text {TeV}$".

Search for heavy resonances that decay into a vector boson and a Higgs boson in hadronic final states at $\sqrt{s} = 13$ $\,\text {TeV}$

Search for heavy resonances that decay into a vector boson and a Higgs boson in hadronic final states at $\sqrt{s} = 13$ $\,\text {TeV}$

... 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 institutes ... See full document

36

Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

... scribed in detail in ...electromagnetic and hadronic calorimeters and a muon spectrometer with a toroidal magnetic ...installed in 2014, a silicon microstrip detector, and ... See full document

23

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 $\sqrt s = 13$ 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 $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector

... SNSF and Cantons of Bern and Geneva, Switzerland; MOST, Taiwan; TAEK, Turkey; STFC, United Kingdom; DOE and NSF, United States of ...America. In addition, individual groups and ... See full document

52

Search for vector-like T and B quark pairs in final states with leptons at $\sqrt{s} =$ 13 TeV

Search for vector-like T and B quark pairs in final states with leptons at $\sqrt{s} =$ 13 TeV

... We search for a vector-like T quark with charge 2e/3 that is produced in pairs with its antiquark, T, via the strong interaction in proton-proton collisions ats = ... See full document

48

Search for high-mass resonances in final states with a lepton and missing transverse momentum at $ \sqrt{s}=13 $ TeV

Search for high-mass resonances in final states with a lepton and missing transverse momentum at $ \sqrt{s}=13 $ TeV

... A search for new high-mass resonances in proton-proton collisions having final states with an electron or muon and missing transverse momentum is ...collected in 2016 with ... See full document

41

Search for a pseudoscalar boson decaying into a Z boson and the 125 GeV Higgs boson in $ℓ^+ℓ^−b\overline{b}$ final states

Search for a pseudoscalar boson decaying into a Z boson and the 125 GeV Higgs boson in $ℓ^+ℓ^−b\overline{b}$ final states

... SM Higgs sector is provided in two Higgs doublet models (2HDM) [4], which introduce a second scalar doublet in addition to the one from the ...quarks and to leptons. In Type-I ... See full document

34

Search for the decay of a Higgs boson in the $\ell\ell\gamma$ channel in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Search for the decay of a Higgs boson in the $\ell\ell\gamma$ channel in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... solenoid, 13 m in length and 6 m in diameter, which provides an axial magnetic field of ...pixel and silicon strip trackers, covering 0 ≤ φ ≤ 2π in azimuth and | η | < ... See full document

42

Search for pair production of heavy vector-like quarks decaying into hadronic final states in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

Search for pair production of heavy vector-like quarks decaying into hadronic final states in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

... HGF, and MPG, Germany; GSRT, Greece; RGC, Hong Kong SAR, China; ISF and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; NWO, Netherlands; RCN, Norway; MNiSW and ... See full document

36

Search for supersymmetry with Higgs boson to diphoton decays using the razor variables at $\sqrt{s} = $ 13 TeV

Search for supersymmetry with Higgs boson to diphoton decays using the razor variables at $\sqrt{s} = $ 13 TeV

... the Higgs boson [1–3] , the first fundamen- tal scalar particle ever observed, has opened a new window for exploring physics not described by the standard model (SM) of par- ticle ...of heavy ... See full document

25

Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

... from hadronic decays of W or Z ...functions that are based on the energies of and pairwise angular distances between the jet’s constituents [58,59] ...parton and those coming from the two-body ... See full document

23

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

... Z boson produced in the decay of a heavy ...background, in this paper we consider just the merged jet topology (Jγ), and thus the search in the hadronic ... See full document

40

Search for the dimuon decay of the Higgs boson in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

Search for the dimuon decay of the Higgs boson in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

... 4.5, and the jet p T must be larger than 25 (30) GeV for jηj < ...track and vertex informa- tion inside a jet [43] is imposed on jets with jηj < ...2.4 and p T < 60 ...neutrinos and b ... See full document

20

Search for massive resonances decaying into $WW$, $WZ$, $ZZ$, $qW$, and $qZ$ with dijet final states at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$

Search for massive resonances decaying into $WW$, $WZ$, $ZZ$, $qW$, and $qZ$ with dijet final states at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$

... W boson candidate if its soft-drop mass falls into the range 65 –85 GeV, while it is deemed a Z boson candidate if it falls into the range 85 –105 ...WZ, and ZZ) for the double-tag ... See full document

25

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

... the TeV scale, giving rise to new massive gauge bosons denoted as Z 0 ...0 vector boson can, in the narrow-width approximation (NWA), be expressed in terms of the quantity c u w u + c d ... See full document

42

Search for heavy resonances decaying to a $W$ or $Z$ boson and a Higgs boson in the $q\bar{q}^{(\prime)}b\bar{b}$ final state in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

Search for heavy resonances decaying to a $W$ or $Z$ boson and a Higgs boson in the $q\bar{q}^{(\prime)}b\bar{b}$ final state in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

... BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, ... See full document

36

Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at $ \sqrt{s}=13 $ TeV

Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at $ \sqrt{s}=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 institutes ... See full document

44

Search for Charged Higgs Bosons Produced via Vector Boson Fusion and Decaying into a Pair of $W$ and $Z$ Bosons Using $pp$ Collisions at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$

Search for Charged Higgs Bosons Produced via Vector Boson Fusion and Decaying into a Pair of $W$ and $Z$ Bosons Using $pp$ Collisions at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$

... A search for charged Higgs bosons produced via vector boson fusion and decaying into W and Z bosons using proton-proton collisions ats = 13 ... See full document

30

Search for a heavy resonance decaying into a Z boson and a Z or W boson in 2ℓ2q final states at $ \sqrt{s}=13 $ TeV

Search for a heavy resonance decaying into a Z boson and a Z or W boson in 2ℓ2q final states at $ \sqrt{s}=13 $ TeV

... resulting in a change of ...propagated, and a smaller impact is observed compared with that due to the uncertainty in the energy ...uncertainty in the signal selection efficiency is the ... See full document

43

Search for the Standard Model Higgs boson produced in association with a vector boson and decaying into a tau pair in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector

Search for the Standard Model Higgs boson produced in association with a vector boson and decaying into a tau pair in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector

... leptons that decay to hadron(s) and a neutrino, or τ had , are reconstructed using clusters of energy deposited in the electromagnetic and hadronic calorimeters ... See full document

25

Measurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at $ \sqrt{s}=13 $ TeV

Measurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at $ \sqrt{s}=13 $ TeV

... values) that control the contributions of the main SM Higgs boson pro- duction ...WH and ZH processes are merged, and then split based on the decay of the associated ... See full document

52

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