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Creators/Authors contains: "Vanegas Arbelaez, N."

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  1. ; ; ; ; ; ; ; ; ; ; et al (, Physical Review D)
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  2. ; ; ; ; ; ; ; ; ; ; et al (, Physics Letters B)
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  3. ; ; ; ; ; ; ; ; ; ; et al (, Physical Review D)
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  4. ; ; ; ; ; ; ; ; ; ; et al (, Journal of High Energy Physics)
    A<sc>bstract</sc> Results are presented from a search for CP violation in top quark pair production, using proton-proton collisions at a center-of-mass energy of 13 TeV. The data used for this analysis consist of final states with two charged leptons collected by the CMS experiment, and correspond to an integrated luminosity of 35.9 fb−1. The search uses two observables,$$ \mathcal{O} $$ O 1and$$ \mathcal{O} $$ O 3, which are Lorentz scalars. The observable$$ \mathcal{O} $$ O 1is constructed from the four-momenta of the charged leptons and the reconstructed top quarks, while$$ \mathcal{O} $$ O 3consists of the four-momenta of the charged leptons and the b quarks originating from the top quarks. Asymmetries in these observables are sensitive to CP violation, and their measurement is used to determine the chromoelectric dipole moment of the top quark. The results are consistent with the expectation from the standard model. 
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  5. ; ; ; ; ; ; ; ; ; ; et al (, Physics Letters B)
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  6. ; ; ; ; ; ; ; ; ; ; et al (, Physics Letters B)
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  7. ; ; ; ; ; ; ; ; ; ; et al (, Physical Review Letters)
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  8. ; ; ; ; ; ; ; ; ; ; et al (, Physics Letters B)
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  10. ; ; ; ; ; ; ; ; ; ; et al (, Journal of High Energy Physics)
    A bstract The cross sections for inclusive and Mueller-Navelet dijet production are measured as a function of the rapidity separation between the jets in proton-proton collisions at $$ \sqrt{s} $$ s = 2 . 76 TeV for jets with transverse momentum p T > 35 GeV and rapidity | y | < 4 . 7. Various dijet production cross section ratios are also measured. A veto on additional jets with p T > 20 GeV is introduced to improve the sensitivity to the effects of the Balitsky-Fadin-Kuraev-Lipatov (BFKL) evolution. The measurement is compared with the predictions of various Monte Carlo models based on leading-order and next-to-leading-order calculations including the Dokshitzer-Gribov-Lipatov-Altarelli-Parisi leading-logarithm (LL) parton shower as well as the LL BFKL resummation. 
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