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[PDF] Top 20 Search for Heavy Higgs Bosons $A/H$ Decaying to a Top Quark Pair in $pp$ Collisions at $\sqrt{s}=8\text{ }\text{ }\mathrm{TeV}$ with the ATLAS Detector

Has 10000 "Search for Heavy Higgs Bosons $A/H$ Decaying to a Top Quark Pair in $pp$ Collisions at $\sqrt{s}=8\text{ }\text{ }\mathrm{TeV}$ with the ATLAS Detector" found on our website. Below are the top 20 most common "Search for Heavy Higgs Bosons $A/H$ Decaying to a Top Quark Pair in $pp$ Collisions at $\sqrt{s}=8\text{ }\text{ }\mathrm{TeV}$ with the ATLAS Detector".

Search for Heavy Higgs Bosons $A/H$ Decaying to a Top Quark Pair in $pp$ Collisions at $\sqrt{s}=8\text{ }\text{ }\mathrm{TeV}$ with the ATLAS Detector

Search for Heavy Higgs Bosons $A/H$ Decaying to a Top Quark Pair in $pp$ Collisions at $\sqrt{s}=8\text{ }\text{ }\mathrm{TeV}$ with the ATLAS Detector

... J. Boudreau 127 , J. Bou ffard 2 , E.V. Bouhova-Thacker 75 , D. Boumediene 37 , C. Bourdarios 119 , S.K. Boutle 56 , A. Boveia 113 , J. Boyd 32 , I.R. Boyko 68 , J. Bracinik 19 , A. Brandt 8 , G. Brandt 57 , O. ... See full document

30

Search for Higgs bosons produced via vector-boson fusion and decaying into bottom quark pairs in $\sqrt{s} = 13$ $\mathrm{TeV}$ $pp$ collisions with the ATLAS detector

Search for Higgs bosons produced via vector-boson fusion and decaying into bottom quark pairs in $\sqrt{s} = 13$ $\mathrm{TeV}$ $pp$ collisions with the ATLAS detector

... channels, the lowest-order polynomial which satisfies basic goodness-of-fit requirements, includ- ing χ 2 and F tests, is chosen as a ...criteria in fits to the data sidebands, an additional ... See full document

29

Search for beyond the standard model Higgs bosons decaying into a $\mathrm{b\overline{b}}$ pair in pp collisions at $\sqrt{s} =$ 13 TeV

Search for beyond the standard model Higgs bosons decaying into a $\mathrm{b\overline{b}}$ pair in pp collisions at $\sqrt{s} =$ 13 TeV

... like to thank Stefan Liebler and Oscar St˚al for their help with the inter- pretation of the results in the 2HDM ...colleagues in the CERN accelerator departments ... See full document

43

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

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

... ies. The first category consists of events with three prompt leptons produced in the decays of electroweak gauge bosons, which are estimated using the simulated samples described ... See full document

37

Search for direct pair production of supersymmetric top quarks decaying to all-hadronic final states in pp collisions at $\sqrt{s} = 8\;\text {TeV} $

Search for direct pair production of supersymmetric top quarks decaying to all-hadronic final states in pp collisions at $\sqrt{s} = 8\;\text {TeV} $

... uncertainty in the ttZ production cross section is estimated from a data control sample with three reconstructed charged leptons drawn from a larger event sample that has been collected with a ... See full document

66

Search for Low Mass Vector Resonances Decaying to Quark-Antiquark Pairs in Proton-Proton Collisions at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$

Search for Low Mass Vector Resonances Decaying to Quark-Antiquark Pairs in Proton-Proton Collisions at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$

... Over the past half-century, searches for narrow resonances in the dijet invariant mass spectrum have been an important part of the physics program at every ...within the many ... See full document

30

Search for Higgs boson pair production in the $bb\tau\tau$ final state in proton-proton collisions at $\sqrt{(}s)=8\text{ }\text{ }\mathrm{TeV}$

Search for Higgs boson pair production in the $bb\tau\tau$ final state in proton-proton collisions at $\sqrt{(}s)=8\text{ }\text{ }\mathrm{TeV}$

... τ h candidates in multijet events are typically due to the misidentification of quark or gluon ...jets. The contribution from this background in the signal region, ... See full document

25

Search for neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

Search for neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

... between the two searches are that they are optimized for different production mechanisms and Higgs boson mass ...Additionally, the three Higgs bosons of the MSSM, which can have ... See full document

55

Search for heavy particles decaying into top-quark pairs using lepton-plus-jets events in proton–proton collisions at $\sqrt{s} = 13$   $\text {TeV}$ with the ATLAS detector

Search for heavy particles decaying into top-quark pairs using lepton-plus-jets events in proton–proton collisions at $\sqrt{s} = 13$   $\text {TeV}$ with the ATLAS detector

... fits to the distributions of relevant reconstructed variables, using MC events for which the reconstructed objects are matched to partons, from Z 0 samples with masses from ...0.5 ... See full document

56

Search for a light charged Higgs boson decaying to $ \mathrm{c}\overline{\mathrm{s}} $ in pp collisions at $ \sqrt{s}=8 $ TeV

Search for a light charged Higgs boson decaying to $ \mathrm{c}\overline{\mathrm{s}} $ in pp collisions at $ \sqrt{s}=8 $ TeV

... A search for a light charged Higgs boson, originating from the decay of a top quark and subsequently decaying into a charm quark and a strange antiquark, is ...presented. ... See full document

34

Search for type-III Seesaw heavy leptons in $pp$ collisions at $\sqrt{s}= 8$ TeV with the ATLAS Detector

Search for type-III Seesaw heavy leptons in $pp$ collisions at $\sqrt{s}= 8$ TeV with the ATLAS Detector

... A search for the pair-production of heavy leptons (N 0 , L ± ) predicted by the type-III seesaw theory formulated to explain the origin of small neutrino masses is ... See full document

22

Search for flavour-changing neutral current top quark decays $t\to Hq$ in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

Search for flavour-changing neutral current top quark decays $t\to Hq$ in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

... C. Gwenlan 120 , C.B. Gwilliam 74 , A. Haas 110 , C. Haber 15 , H.K. Hadavand 8 , N. Haddad 135e , P. Haefner 21 , S. Hageböck 21 , Z. Hajduk 39 , H. Hakobyan 177 , M. Haleem 42 , J. Haley 114 , D. ... See full document

60

Search for Higgs bosons decaying to $aa$ in the $\mu\mu\tau\tau$ final state in $pp$ collisions at $\sqrt{s} = $ 8 TeV with the ATLAS experiment

Search for Higgs bosons decaying to $aa$ in the $\mu\mu\tau\tau$ final state in $pp$ collisions at $\sqrt{s} = $ 8 TeV with the ATLAS experiment

... J. Cummings 176 , M. Curatolo 47 , C. Cuthbert 150 , H. Czirr 141 , P. Czodrowski 3 , S. D’Auria 53 , M. D’Onofrio 74 , M.J. Da Cunha Sargedas De Sousa 126a,126b , C. Da Via 84 , W. Dabrowski 38a , A. ... See full document

24

Measurement of top quark-antiquark pair production in association with a W or Z boson in pp collisions at $\sqrt{s} = 8$ $\,\text {TeV}$

Measurement of top quark-antiquark pair production in association with a W or Z boson in pp collisions at $\sqrt{s} = 8$ $\,\text {TeV}$

... passing the selection ...and to calculate a “track-to-lepton” ratio, which depends on the heavy-flavour content and jet ...activity. The track-to-lepton ratio is ... See full document

39

Search for a $W$ ' boson decaying to a bottom quark and a top quark in $pp$ collisions at $\sqrt{s}=7$ TeV

Search for a $W$ ' boson decaying to a bottom quark and a top quark in $pp$ collisions at $\sqrt{s}=7$ TeV

... gauge bosons, usually called W 0 , are predicted by various extensions of the standard model (SM), for example ...[1–4]. In contrast to the W boson, which couples only to ... See full document

33

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

39

A search for high-mass resonances decaying to $\tau^{+}\tau^{-}$ in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

A search for high-mass resonances decaying to $\tau^{+}\tau^{-}$ in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

... new heavy resonances decaying to tau lepton pairs are both theoretically and experimentally well motivated ...[1–6]. Heavy Z 0 bosons often arise in grand unified theories and ... See full document

50

Search for a Heavy Neutral Particle Decaying to $e\mu$, $e\tau$, or $\mu\tau$ in $pp$ Collisions at $\sqrt{s}=8$ TeV with the ATLAS Detector

Search for a Heavy Neutral Particle Decaying to $e\mu$, $e\tau$, or $\mu\tau$ in $pp$ Collisions at $\sqrt{s}=8$ TeV with the ATLAS Detector

... G.N. Hamity 146c , P.G. Hamnett 42 , L. Han 33b , K. Hanagaki 118 , K. Hanawa 156 , M. Hance 15 , P. Hanke 58a , R. Hanna 137 , J.B. Hansen 36 , J.D. Hansen 36 , M.C. Hansen 21 , P.H. Hansen 36 , K. Hara 161 , A.S. Hard ... See full document

25

Search for charged Higgs bosons in the $H^{\pm} \rightarrow tb$ decay channel in $pp$ collisions at $\sqrt{s}=8 $ TeV using the ATLAS detector

Search for charged Higgs bosons in the $H^{\pm} \rightarrow tb$ decay channel in $pp$ collisions at $\sqrt{s}=8 $ TeV using the ATLAS detector

... contain at least one particle jet that is matched to a b-flavoured hadron not originating from the decay of the t¯t ...where at least one particle jet is matched to a c-flavoured ... See full document

48

Search for top squarks decaying to tau sleptons in $pp$ collisions at  $\sqrt{s}= 13$ TeV with the ATLAS detector

Search for top squarks decaying to tau sleptons in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector

... momentum. The dominant SM background process with this signature is pair production of top ...contribute in two different ways. In the first case, the objects from ... See full document

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