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[PDF] Top 20 Search for flavour-changing neutral current top quark decays $t\to Hq$ in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

Has 10000 "Search for flavour-changing neutral current top quark decays $t\to Hq$ in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector" found on our website. Below are the top 20 most common "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

Search for flavour-changing neutral current top quark decays $t\to Hq$ in $pp$ collisions at $\sqrt{s}=8$ 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, Canada; CERN; CONICYT, Chile; ... See full document

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Search for associated production of a Z boson with a single top quark and for tZ flavour-changing interactions in pp collisions at $ \sqrt{s}=8 $ TeV

Search for associated production of a Z boson with a single top quark and for tZ flavour-changing interactions in pp collisions at $ \sqrt{s}=8 $ TeV

... of the corresponding ECAL cluster, and the energy sum of all bremsstrahlung photons spatially compatible with originating from the electron ...track. The momentum of the muons is ... See full document

42

Search for high-mass dilepton resonances in pp collisions at $\sqrt{s}=8$  TeV with the ATLAS detector

Search for high-mass dilepton resonances in pp collisions at $\sqrt{s}=8$  TeV with the ATLAS detector

... only the central values for ABM11 fall outside of the MSTW2008NNLO PDF’s uncertainty ...of the latter uncertainty and the ABM11 cen- tral value is formed with respect to ... See full document

31

Search for resonances decaying into top-quark pairs using fully hadronic decays in $pp$ collisions with ATLAS at $\sqrt{s}=7$ TeV

Search for resonances decaying into top-quark pairs using fully hadronic decays in $pp$ collisions with ATLAS at $\sqrt{s}=7$ TeV

... events in the signal region (subsample P) is calculated with an iterative method that uses the lack of correlation in b-tagging efficiencies between the leading and recoil ... See full document

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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

... K. Mochizuki 97 , P. Mogg 51 , S. Mohapatra 38 , S. Molander 148a,148b , R. Moles-Valls 23 , R. Monden 71 , M.C. Mondragon 93 , K. Mönig 45 , J. Monk 39 , E. Monnier 88 , A. Montalbano 150 , J. Montejo ... See full document

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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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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. Jakobsen 30 , T. Jakoubek 127 , J. Jakubek 128 , D.O. Jamin 114 , D.K. Jana 79 , E. Jansen 78 , R. Jansky 62 , J. Janssen 21 , M. Janus 54 , G. Jarlskog 81 , N. Javadov 65,b , T. Jav˚urek 48 , L. ... See full document

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Search for heavy Majorana neutrinos with the ATLAS detector in pp collisions at $ \sqrt{s}=8 $ TeV

Search for heavy Majorana neutrinos with the ATLAS detector in pp collisions at $ \sqrt{s}=8 $ TeV

... measured in a selection of events which contain a large number of fake and non-prompt ...leptons. In these control samples, any residual prompt background is subtracted using MC estimates, and low-mass ... See full document

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Search for $W' \rightarrow tb \rightarrow qqbb$ decays in $pp$ collisions at $\sqrt{s}$  = 8 TeV with the ATLAS detector

Search for $W' \rightarrow tb \rightarrow qqbb$ decays in $pp$ collisions at $\sqrt{s}$  = 8 TeV with the ATLAS detector

... ratios to the tb final state are obtained from next-to-leading order (NLO) QCD calculations [ 11 , 23 ] and are shown for dif- ferent W 0 masses in Table 1 .... The mass of a possible ... See full document

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Search for $s$-channel single top-quark production in proton–proton collisions at $\sqrt s=8$ TeV with the ATLAS detector

Search for $s$-channel single top-quark production in proton–proton collisions at $\sqrt s=8$ TeV with the ATLAS detector

... of the backgrounds is validated by comparing the expected event distributions to the data in two control re- ...gions. The first control sample is defined by requiring both jets ... See full document

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Search for Scalar Charm Quark Pair Production in $pp$ Collisions at $\sqrt{s}=$ 8  TeV with the ATLAS Detector

Search for Scalar Charm Quark Pair Production in $pp$ Collisions at $\sqrt{s}=$ 8  TeV with the ATLAS Detector

... dedicated search for pair production of scalar partners of charm quarks are re- ...ported. The search is based on an integrated luminosity of ...of pp collisions ats = ... See full document

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Search for FCNC single top-quark production at $\sqrt{s}=7$ TeV with the ATLAS detector

Search for FCNC single top-quark production at $\sqrt{s}=7$ TeV with the ATLAS detector

... object to test the Standard Model (SM) of particle physics. The properties of the top quark can be studied from proton- proton (pp) collisions ats ... See full document

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Searches for scalar leptoquarks in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

Searches for scalar leptoquarks in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

... is the production of Z bosons in association with heavy-flavour jets where the Z boson subsequently decays to two neutrinos (Z(→ νν) + ...data in an opposite-sign ... See full document

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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

... decaying to tau lepton pairs are both theoretically and experimentally well motivated ...arise in grand unified theories and while they are typically considered to obey lepton universality, this is ... See full document

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Search for a CP-odd Higgs boson decaying to Zh in pp collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector

Search for a CP-odd Higgs boson decaying to Zh in pp collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector

... contributions to the background are from diboson and triboson production, t¯ t pro- duction in association with a Z boson, and SM Higgs boson ...amount to about 95% (65%) ... See full document

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Measurement of the $t$-channel single top-quark production cross section in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Measurement of the $t$-channel single top-quark production cross section in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... of the W+jets back- ground, which comprises contributions from W+heavy flavour jets (Wb ¯b+jets, Wc¯c+jets and Wc+jets) and W+light jets, are taken from samples of simulated events, while the ... 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

... 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 misidentified as ... See full document

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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

... late the matrix elements for each process, while MadE- vent [20] with the MSTW2008 parton distribution func- tions (PDF) set [21] simulates the initial hard scatter- ing and the N and L ... See full document

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Search for Anomalous Single Top Quark Production in Association with a Photon in $pp$ Collisions at $ \sqrt{s}=8 $ TeV

Search for Anomalous Single Top Quark Production in Association with a Photon in $pp$ Collisions at $ \sqrt{s}=8 $ TeV

... and the modeling of pileup are propagated to the uncertainties in the sig- nal and SM background ...expectations. The uncertainty in modeling the pileup is esti- ... See full document

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Search for flavor-changing neutral currents in top quark decays $t\to Hc$ and $t \to Hu$ in multilepton final states in proton-proton collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector

Search for flavor-changing neutral currents in top quark decays $t\to Hc$ and $t \to Hu$ in multilepton final states in proton-proton collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector

... measured in control regions with the same selection criteria as the 2lSS signal category except that the number of jets must be two or three, one lepton need only satisfy L criteria, ... See full document

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