2018
DOI: 10.1007/jhep06(2018)079
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Probing the top-Higgs Yukawa CP structure in dileptonic $$ t\overline{t}h $$ with M2-assisted reconstruction

Abstract: Constraining the Higgs boson properties is a cornerstone of the LHC program. We study the potential to directly probe the Higgs-top CP-structure via the tth channel at the LHC with the Higgs boson decaying to a bottom pair and top-quarks in the dileptonic mode. We show that a combination of laboratory and tt rest frame observables display large CP-sensitivity, exploring the spin correlations in the top decays. To efficiently reconstruct our final state, we present a method based on simple mass minimization and… Show more

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Cited by 48 publications
(45 citation statements)
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References 81 publications
(114 reference statements)
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“…Additional complex phases in the SM Yukawa sector would be another source of CP-violation, e.g. in the tth interaction [28][29][30][31]. Any kinematic effect from this interaction would be degenerate with O HG in gluon-fusion production as long as the m t threshold is not resolved kinematically, which does not happen for our choice of measurements.…”
Section: Theoretical Frameworkmentioning
confidence: 99%
See 2 more Smart Citations
“…Additional complex phases in the SM Yukawa sector would be another source of CP-violation, e.g. in the tth interaction [28][29][30][31]. Any kinematic effect from this interaction would be degenerate with O HG in gluon-fusion production as long as the m t threshold is not resolved kinematically, which does not happen for our choice of measurements.…”
Section: Theoretical Frameworkmentioning
confidence: 99%
“…This is not the case for terms proportional to 1/Λ 4 , which contain the squared dimension-6 amplitude and produce a CP-even effect regardless of the nature of the operator. This has historically served as a motivation to constrain CP-odd operators with momentumdependent observables in a range of production modes [25,29,31,[38][39][40][41][42][43][44][45]. However, such an approach is more model-dependent since it neglects dimension-8 operators that interfere with the SM and in general produce similar O(1/Λ 4 ) effects.…”
Section: Theoretical Frameworkmentioning
confidence: 99%
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“…where φ ,1 (φ ,2 ) is the azimuthal angle of the first (second) charged lepton [28]. The leptons are ordered according to their rapidity, i.e.…”
Section: B Observablesmentioning
confidence: 99%
“…An analogous observable can be constructed for top quarkassociated Higgs production as well, as discussed in detail recently in Ref. [27,28]. Working in the dimension six linearised approximation, such observables are the only phenomenologically viable ones because the interference terms cancel identically for any CP-even observable, such as total cross sections, decay widths as well as momentum transfer-dependent observables such as transverse momenta and invariant masses.…”
Section: Introductionmentioning
confidence: 99%