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|a dc
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|a CMS Collaboration
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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 Abercrombie, Daniel Robert
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|a Allen, Brandon Leigh
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|a Apyan, Aram
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|a Azzolini, Virginia
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|a Barbieri, Richard Alexander
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|a Levin, Amy Elizabeth
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|a Luckey Jr, P David
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|a Maier, Benedikt
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|a Marini, Andrea Carlo
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|a McGinn, Christopher Francis
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|a Mironov, Camelia Maria
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|a Narayanan, Siddharth Madhavan
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|a Niu, Xinmei
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|a Paus, Christoph M. E.
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|a Roland, Christof E
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|a Salfeld-Nebgen, Jakob Maxillian Henry
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|a Stephans, George S. F.
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|a Allen, Brandon Leigh
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|a Apyan, Aram
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|a Azzolini, Virginia
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|a Barbieri, Richard Alexander
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|a Baty, Austin Alan
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|a Bi, Ran
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|a Bierwagen, Katharina
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|a Brandt, Stephanie Akemi
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|a Busza, Wit
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|a Cali, Ivan Amos
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|a Demiragli, Zeynep
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|a Di Matteo, Leonardo
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|a Gomez-Ceballos, Guillelmo
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|a Goncharov, Maxim
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|a Hsu, Dylan George
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|a Iiyama, Yutaro
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|a Innocenti, Gian Michele
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|a Klute, Markus
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|a Kovalskyi, Dmytro
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|a Krajczar, Krisztian F.
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|a Lai, Yue Shi
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|a Lee, Yen-Jie
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|a Levin, Amy Elizabeth
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|a Luckey Jr, P David
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|a Maier, Benedikt
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|a Marini, Andrea Carlo
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|a McGinn, Christopher Francis
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|a Mironov, Camelia Maria
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|a Narayanan, Siddharth Madhavan
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|a Niu, Xinmei
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|a Paus, Christoph M. E.
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|a Roland, Christof E
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|a Roland, Gunther M
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|a Salfeld-Nebgen, Jakob Maxillian Henry
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|a Stephans, George S. F.
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|a Tatar, Kaya
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|a Varma, Mukund Madhav
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|a Velicanu, Dragos Alexandru
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|a Veverka, Jan
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|a Wang, Jing
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|a Wang, Ta-Wei
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|a Wyslouch, Boleslaw
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|a Yang, Ming
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|a Wyslouch, Victoria
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|a Cross Section Measurement of t -Channel Single Top Quark Production in pp Collisions at √s = 13 TeV
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|b Elsevier BV,
|c 2018-06-07T20:05:19Z.
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|z Get fulltext
|u http://hdl.handle.net/1721.1/116175
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|a The cross section for the production of single top quarks in the t channel is measured in proton-proton collisions at 13 TeV with the CMS detector at the LHC. The analyzed data correspond to an integrated luminosity of 2.2fb[superscript −1]. The event selection requires one muon and two jets where one of the jets is identified as originating from a bottom quark. Several kinematic variables are then combined into a multivariate discriminator to distinguish signal from background events. A fit to the distribution of the discriminating variable yields a total cross section of 238±13(stat)±29(syst) pb and a ratio of top quark and top antiquark production of R t-ch. =1.81±0.18(stat)±0.15(syst). From the total cross section the absolute value of the CKM matrix element V[subscript tb] is calculated to be 1.05±0.07(exp)±0.02(theo). All results are in agreement with the standard model predictions.
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|a Article
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|t Physics Letters B
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