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|a Apyan, Aram
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|a Massachusetts Institute of Technology. Department of Physics
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|a Massachusetts Institute of Technology. Laboratory for Nuclear Science
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|a Apyan, Aram
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|a Barbieri, Richard Alexander
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|a Bauer, Gerry P.
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|a Busza, Wit
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|a Cali, Ivan Amos
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|a Chan, M.
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|a Di Matteo, Leonardo
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|a Dutta, Valentina
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|a Gomez-Ceballos, Guillelmo
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|a Goncharov, Maxim
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|a Gulhan, Doga Can
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|a Klute, Markus
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|a Lai, Yue Shi
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|a Lee, Yen-Jie
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|a Luckey, P. David
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|a Ma, T.
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|a Paus, Christoph M. E.
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|a Ralph, Duncan Kelley
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|a Roland, Christof E.
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|a Roland, Gunther M.
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|a Stephans, George S. F.
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|a Stoeckli, Fabian
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|a Sumorok, Konstanty C.
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|a Velicanu, Dragos Alexandru
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|a Veverka, Jan
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|a Wyslouch, Boleslaw
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|a Yang, M.
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|a Zanetti, Marco
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|a Zhukova, Victoria
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|a Barbieri, Richard Alexander
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|a Bauer, Gerry P.
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|a Busza, Wit
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|a Cali, Ivan Amos
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|a Chan, M.
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|a Di Matteo, Leonardo
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|a Dutta, Valentina
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|a Gomez-Ceballos, Guillelmo
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|a Goncharov, Maxim
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|a Gulhan, Doga Can
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|a Klute, Markus
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|a Lai, Yue Shi
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|a Lee, Yen-Jie
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|a Luckey, P. David
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|a Ma, T.
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|a Paus, Christoph M. E.
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|a Ralph, Duncan Kelley
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|a Roland, Christof E.
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|a Roland, Gunther M.
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|a Stephans, George S. F.
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|a Stoeckli, Fabian
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|a Sumorok, Konstanty C.
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|a Velicanu, Dragos Alexandru
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|a Veverka, Jan
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|a Wyslouch, Boleslaw
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|a Yang, M.
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|a Zanetti, Marco
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|a Zhukova, Victoria
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|a ATLAS Collaboration
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|a Search for top-squark pairs decaying into Higgs or Z bosons in pp collisions at √s = 8 TeV
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|b Elsevier B.V.,
|c 2014-10-27T15:01:23Z.
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|z Get fulltext
|u http://hdl.handle.net/1721.1/91178
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|a A search for supersymmetry through the direct pair production of top squarks, with Higgs (H) or Z bosons in the decay chain, is performed using a data sample of proton-proton collisions at √s=8 TeV collected in 2012 with the CMS detector at the LHC. The sample corresponds to an integrated luminosity of 19.5 fb[superscript −1]. The search is performed using a selection of events containing leptons and bottom-quark jets. No evidence for a significant excess of events over the standard model background prediction is observed. The results are interpreted in the context of simplified supersymmetric models with pair production of a heavier top-squark mass eigenstate t˜2 decaying to a lighter top-squark mass eigenstate t˜1 via either ˜2→Ht˜1 or t˜2→Zt˜1, followed in both cases by t˜1→tχ˜10, where χ˜10 is an undetected, stable, lightest supersymmetric particle. The interpretation is performed in the region where the mass difference between thet˜1 and χ˜10 states is approximately equal to the top-quark mass (m[subscript t˜1]−mχ˜10≃mt), which is not probed by searches for direct t˜1 squark pair production. The analysis excludes top squarks with masses m[subscript t˜2]<575 GeV and m[subscript t˜1]<400 GeV at a 95% confidence level.
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|a National Science Foundation (U.S.)
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|a United States. Dept. of Energy
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|a en_US
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|a Article
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|t Physics Letters B
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